diff --git a/B2Kemu/Col_aproval/Makefile b/B2Kemu/Col_aproval/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/B2Kemu/Col_aproval/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/B2Kemu/Col_aproval/beamercolorthemeFlip.sty b/B2Kemu/Col_aproval/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/B2Kemu/Col_aproval/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/B2Kemu/Col_aproval/beamerinnerthemeFlip.sty b/B2Kemu/Col_aproval/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/B2Kemu/Col_aproval/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/B2Kemu/Col_aproval/beamerouterthemeFlip.sty b/B2Kemu/Col_aproval/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/B2Kemu/Col_aproval/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/B2Kemu/Col_aproval/beamerouterthemedecolines.sty b/B2Kemu/Col_aproval/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/B2Kemu/Col_aproval/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/B2Kemu/Col_aproval/beamerthemeFlip.sty b/B2Kemu/Col_aproval/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/B2Kemu/Col_aproval/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files 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mchrzasz $ +%%% ====================================================================== +%%% Purpose: Standard LHCb aliases +%%% Author: Originally Ulrik Egede, adapted by Tomasz Skwarnicki for templates, +%%% rewritten by Chris Parkes +%%% Maintainer : Ulrik Egede (2010 - 2012) +%%% Maintainer : Rolf Oldeman (2012 - 2014) +%%% ======================================================================= + +%%% To use this file outside the normal LHCb document environment, the +%%% following should be added in a preamble (before \begin{document} +%%% +%%%\usepackage{ifthen} +%%%\newboolean{uprightparticles} +%%%\setboolean{uprightparticles}{false} %Set true for upright particle symbols +\usepackage{xspace} +\usepackage{upgreek} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% +%%% The following is to ensure that the template automatically can process +%%% this file. +%%% +%%% Add comments with at least three %%% preceding. +%%% Add new sections with one % preceding +%%% Add new subsections with two %% preceding +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +%%%%%%%%%%%%% +% Experiments +%%%%%%%%%%%%% +\def\lhcb {\mbox{LHCb}\xspace} +\def\atlas {\mbox{ATLAS}\xspace} +\def\cms {\mbox{CMS}\xspace} +\def\alice {\mbox{ALICE}\xspace} +\def\babar {\mbox{BaBar}\xspace} +\def\belle {\mbox{Belle}\xspace} +\def\cleo {\mbox{CLEO}\xspace} +\def\cdf {\mbox{CDF}\xspace} +\def\dzero {\mbox{D0}\xspace} +\def\aleph {\mbox{ALEPH}\xspace} +\def\delphi {\mbox{DELPHI}\xspace} +\def\opal {\mbox{OPAL}\xspace} +\def\lthree {\mbox{L3}\xspace} +\def\sld {\mbox{SLD}\xspace} +%%%\def\argus {\mbox{ARGUS}\xspace} +%%%\def\uaone {\mbox{UA1}\xspace} +%%%\def\uatwo {\mbox{UA2}\xspace} +%%%\def\ux85 {\mbox{UX85}\xspace} +\def\cern {\mbox{CERN}\xspace} +\def\lhc {\mbox{LHC}\xspace} +\def\lep {\mbox{LEP}\xspace} +\def\tevatron {Tevatron\xspace} + +%% LHCb sub-detectors and sub-systems + +%%%\def\pu {PU\xspace} +\def\velo {VELO\xspace} +\def\rich {RICH\xspace} +\def\richone {RICH1\xspace} +\def\richtwo {RICH2\xspace} +\def\ttracker {TT\xspace} +\def\intr {IT\xspace} +\def\st {ST\xspace} +\def\ot {OT\xspace} +\def\herschel {\mbox{\textsc{HeRSCheL}}\xspace} +%%%\def\Tone {T1\xspace} +%%%\def\Ttwo {T2\xspace} +%%%\def\Tthree {T3\xspace} +%%%\def\Mone {M1\xspace} +%%%\def\Mtwo {M2\xspace} +%%%\def\Mthree {M3\xspace} +%%%\def\Mfour {M4\xspace} +%%%\def\Mfive {M5\xspace} +\def\spd {SPD\xspace} +\def\presh {PS\xspace} +\def\ecal {ECAL\xspace} +\def\hcal {HCAL\xspace} +%%%\def\bcm {BCM\xspace} +\def\MagUp {\mbox{\em Mag\kern -0.05em Up}\xspace} +\def\MagDown {\mbox{\em MagDown}\xspace} + +\def\ode {ODE\xspace} +\def\daq {DAQ\xspace} +\def\tfc {TFC\xspace} +\def\ecs {ECS\xspace} +\def\lone {L0\xspace} +\def\hlt {HLT\xspace} +\def\hltone {HLT1\xspace} +\def\hlttwo {HLT2\xspace} + +%%% Upright (not slanted) Particles + + + +{\def\Palpha {\ensuremath{\alpha}\xspace} + \def\Pbeta {\ensuremath{\beta}\xspace} + \def\Pgamma {\ensuremath{\gamma}\xspace} + \def\Pdelta {\ensuremath{\delta}\xspace} + \def\Pepsilon {\ensuremath{\epsilon}\xspace} + \def\Pvarepsilon {\ensuremath{\varepsilon}\xspace} + \def\Pzeta {\ensuremath{\zeta}\xspace} + \def\Peta {\ensuremath{\eta}\xspace} + \def\Ptheta {\ensuremath{\theta}\xspace} + \def\Pvartheta {\ensuremath{\vartheta}\xspace} + \def\Piota {\ensuremath{\iota}\xspace} + \def\Pkappa {\ensuremath{\kappa}\xspace} + \def\Plambda {\ensuremath{\lambda}\xspace} + \def\Pmu {\ensuremath{\mu}\xspace} + \def\Pnu {\ensuremath{\nu}\xspace} + \def\Pxi {\ensuremath{\xi}\xspace} + \def\Ppi {\ensuremath{\pi}\xspace} + \def\Pvarpi {\ensuremath{\varpi}\xspace} + \def\Prho {\ensuremath{\rho}\xspace} + \def\Pvarrho {\ensuremath{\varrho}\xspace} + \def\Ptau {\ensuremath{\tau}\xspace} + \def\Pupsilon {\ensuremath{\upsilon}\xspace} + \def\Pphi {\ensuremath{\phi}\xspace} + \def\Pvarphi {\ensuremath{\varphi}\xspace} + \def\Pchi {\ensuremath{\chi}\xspace} + \def\Ppsi {\ensuremath{\psi}\xspace} + \def\Pomega {\ensuremath{\omega}\xspace} + \mathchardef\PDelta="7101 + \mathchardef\PXi="7104 + \mathchardef\PLambda="7103 + \mathchardef\PSigma="7106 + \mathchardef\POmega="710A + \mathchardef\PUpsilon="7107 + \def\PA {\ensuremath{A}\xspace} + \def\PB {\ensuremath{B}\xspace} + \def\PC {\ensuremath{C}\xspace} + \def\PD {\ensuremath{D}\xspace} + \def\PE {\ensuremath{E}\xspace} + \def\PF {\ensuremath{F}\xspace} + \def\PG {\ensuremath{G}\xspace} + \def\PH {\ensuremath{H}\xspace} + \def\PI {\ensuremath{I}\xspace} + \def\PJ {\ensuremath{J}\xspace} + \def\PK {\ensuremath{K}\xspace} + \def\PL {\ensuremath{L}\xspace} + \def\PM {\ensuremath{M}\xspace} + \def\PN {\ensuremath{N}\xspace} + \def\PO {\ensuremath{O}\xspace} + \def\PP {\ensuremath{P}\xspace} + \def\PQ {\ensuremath{Q}\xspace} + \def\PR {\ensuremath{R}\xspace} + \def\PS {\ensuremath{S}\xspace} + \def\PT {\ensuremath{T}\xspace} + \def\PU {\ensuremath{U}\xspace} + \def\PV {\ensuremath{V}\xspace} + \def\PW {\ensuremath{W}\xspace} + \def\PX {\ensuremath{X}\xspace} + \def\PY {\ensuremath{Y}\xspace} + \def\PZ {\ensuremath{Z}\xspace} + \def\Pa {\ensuremath{a}\xspace} + \def\Pb {\ensuremath{b}\xspace} + \def\Pc {\ensuremath{c}\xspace} + \def\Pd {\ensuremath{d}\xspace} + \def\Pe {\ensuremath{e}\xspace} + \def\Pf {\ensuremath{f}\xspace} + \def\Pg {\ensuremath{g}\xspace} + \def\Ph {\ensuremath{h}\xspace} + \def\Pi {\ensuremath{i}\xspace} + \def\Pj {\ensuremath{j}\xspace} + \def\Pk {\ensuremath{k}\xspace} + \def\Pl {\ensuremath{l}\xspace} + \def\Pm {\ensuremath{m}\xspace} + \def\Pn {\ensuremath{n}\xspace} + \def\Po {\ensuremath{o}\xspace} + \def\Pp {\ensuremath{p}\xspace} + \def\Pq {\ensuremath{q}\xspace} + \def\Pr {\ensuremath{r}\xspace} + \def\Ps {\ensuremath{s}\xspace} + \def\Pt {\ensuremath{t}\xspace} + \def\Pu {\ensuremath{u}\xspace} + \def\Pv {\ensuremath{v}\xspace} + \def\Pw {\ensuremath{w}\xspace} + \def\Px {\ensuremath{x}\xspace} + \def\Py {\ensuremath{y}\xspace} + \def\Pz {\ensuremath{z}\xspace} +} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Particles + + +\DeclareRobustCommand{\optbar}[1]{\shortstack{{\miniscule (\rule[.5ex]{1.25em}{.18mm})} + \\ [-.7ex] $#1$}} + + +%% Leptons + +\let\emi\en +\def\electron {{\ensuremath{\Pe}}\xspace} +\def\en {{\ensuremath{\Pe^-}}\xspace} % electron negative (\em is taken) +\def\ep {{\ensuremath{\Pe^+}}\xspace} +\def\epm {{\ensuremath{\Pe^\pm}}\xspace} +\def\emp {{\ensuremath{\Pe^\mp}}\xspace} +\def\epem {{\ensuremath{\Pe^+\Pe^-}}\xspace} +%%%\def\ee {\ensuremath{\Pe^-\Pe^-}\xspace} + +\def\muon {{\ensuremath{\Pmu}}\xspace} +\def\mup {{\ensuremath{\Pmu^+}}\xspace} +\def\mun {{\ensuremath{\Pmu^-}}\xspace} % muon negative (\mum is taken) +\def\mupm {{\ensuremath{\Pmu^{\pm}}}\xspace} +\def\mump {{\ensuremath{\Pmu^{\mp}}}\xspace} +\def\mumu {{\ensuremath{\Pmu^+\Pmu^-}}\xspace} + +\def\tauon {{\ensuremath{\Ptau}}\xspace} +\def\taup {{\ensuremath{\Ptau^+}}\xspace} +\def\taum {{\ensuremath{\Ptau^-}}\xspace} +\def\tautau {{\ensuremath{\Ptau^+\Ptau^-}}\xspace} + +\def\lepton {{\ensuremath{\ell}}\xspace} +\def\ellm {{\ensuremath{\ell^-}}\xspace} +\def\ellp {{\ensuremath{\ell^+}}\xspace} +\def\ellell {\ensuremath{\ell^+ \ell^-}\xspace} + +\def\neu {{\ensuremath{\Pnu}}\xspace} +\def\neub {{\ensuremath{\overline{\Pnu}}}\xspace} +%%%\def\nuenueb {\ensuremath{\neu\neub}\xspace} +\def\neue {{\ensuremath{\neu_e}}\xspace} +\def\neueb {{\ensuremath{\neub_e}}\xspace} +%%%\def\neueneueb {\ensuremath{\neue\neueb}\xspace} +\def\neum {{\ensuremath{\neu_\mu}}\xspace} +\def\neumb {{\ensuremath{\neub_\mu}}\xspace} +%%%\def\neumneumb {\ensuremath{\neum\neumb}\xspace} +\def\neut {{\ensuremath{\neu_\tau}}\xspace} +\def\neutb {{\ensuremath{\neub_\tau}}\xspace} +%%%\def\neutneutb {\ensuremath{\neut\neutb}\xspace} +\def\neul {{\ensuremath{\neu_\ell}}\xspace} +\def\neulb {{\ensuremath{\neub_\ell}}\xspace} +%%%\def\neulneulb {\ensuremath{\neul\neulb}\xspace} + +%% Gauge bosons and scalars + +\def\g {{\ensuremath{\Pgamma}}\xspace} +\def\H {{\ensuremath{\PH^0}}\xspace} +\def\Hp {{\ensuremath{\PH^+}}\xspace} +\def\Hm {{\ensuremath{\PH^-}}\xspace} +\def\Hpm {{\ensuremath{\PH^\pm}}\xspace} +\def\W {{\ensuremath{\PW}}\xspace} +\def\Wp {{\ensuremath{\PW^+}}\xspace} +\def\Wm {{\ensuremath{\PW^-}}\xspace} +\def\Wpm {{\ensuremath{\PW^\pm}}\xspace} +\def\Z {{\ensuremath{\PZ}}\xspace} + +%% Quarks + +\def\quark {{\ensuremath{\Pq}}\xspace} +\def\quarkbar {{\ensuremath{\overline \quark}}\xspace} +\def\qqbar {{\ensuremath{\quark\quarkbar}}\xspace} +\def\uquark {{\ensuremath{\Pu}}\xspace} +\def\uquarkbar {{\ensuremath{\overline \uquark}}\xspace} +\def\uubar {{\ensuremath{\uquark\uquarkbar}}\xspace} +\def\dquark {{\ensuremath{\Pd}}\xspace} +\def\dquarkbar {{\ensuremath{\overline \dquark}}\xspace} +\def\ddbar {{\ensuremath{\dquark\dquarkbar}}\xspace} +\def\squark {{\ensuremath{\Ps}}\xspace} +\def\squarkbar {{\ensuremath{\overline \squark}}\xspace} +\def\ssbar {{\ensuremath{\squark\squarkbar}}\xspace} +\def\cquark {{\ensuremath{\Pc}}\xspace} +\def\cquarkbar {{\ensuremath{\overline \cquark}}\xspace} +\def\ccbar {{\ensuremath{\cquark\cquarkbar}}\xspace} +\def\bquark {{\ensuremath{\Pb}}\xspace} +\def\bquarkbar {{\ensuremath{\overline \bquark}}\xspace} +\def\bbbar {{\ensuremath{\bquark\bquarkbar}}\xspace} +\def\tquark {{\ensuremath{\Pt}}\xspace} +\def\tquarkbar {{\ensuremath{\overline \tquark}}\xspace} +\def\ttbar {{\ensuremath{\tquark\tquarkbar}}\xspace} + +%% Light mesons + +\def\hadron {{\ensuremath{\Ph}}\xspace} +\def\pion {{\ensuremath{\Ppi}}\xspace} +\def\piz {{\ensuremath{\pion^0}}\xspace} +\def\pizs {{\ensuremath{\pion^0\mbox\,\mathrm{s}}}\xspace} +\def\pip {{\ensuremath{\pion^+}}\xspace} +\def\pim {{\ensuremath{\pion^-}}\xspace} +\def\pipm {{\ensuremath{\pion^\pm}}\xspace} +\def\pimp {{\ensuremath{\pion^\mp}}\xspace} + +\def\rhomeson {{\ensuremath{\Prho}}\xspace} +\def\rhoz {{\ensuremath{\rhomeson^0}}\xspace} +\def\rhop {{\ensuremath{\rhomeson^+}}\xspace} +\def\rhom {{\ensuremath{\rhomeson^-}}\xspace} +\def\rhopm {{\ensuremath{\rhomeson^\pm}}\xspace} +\def\rhomp {{\ensuremath{\rhomeson^\mp}}\xspace} + +\def\kaon {{\ensuremath{\PK}}\xspace} +%%% do NOT use ensuremath here + \def\Kbar {{\kern 0.2em\overline{\kern -0.2em \PK}{}}\xspace} +\def\Kb {{\ensuremath{\Kbar}}\xspace} +\def\KorKbar {\kern 0.18em\optbar{\kern -0.18em K}{}\xspace} +\def\Kz {{\ensuremath{\kaon^0}}\xspace} +\def\Kzb {{\ensuremath{\Kbar{}^0}}\xspace} +\def\Kp {{\ensuremath{\kaon^+}}\xspace} +\def\Km {{\ensuremath{\kaon^-}}\xspace} +\def\Kpm {{\ensuremath{\kaon^\pm}}\xspace} +\def\Kmp {{\ensuremath{\kaon^\mp}}\xspace} +\def\KS {{\ensuremath{\kaon^0_{\mathrm{ \scriptscriptstyle S}}}}\xspace} +\def\KL {{\ensuremath{\kaon^0_{\mathrm{ \scriptscriptstyle L}}}}\xspace} +\def\Kstarz {{\ensuremath{\kaon^{*0}}}\xspace} +\def\Kstarzb {{\ensuremath{\Kbar{}^{*0}}}\xspace} +\def\Kstar {{\ensuremath{\kaon^*}}\xspace} +\def\Kstarb {{\ensuremath{\Kbar{}^*}}\xspace} +\def\Kstarp {{\ensuremath{\kaon^{*+}}}\xspace} +\def\Kstarm {{\ensuremath{\kaon^{*-}}}\xspace} +\def\Kstarpm {{\ensuremath{\kaon^{*\pm}}}\xspace} +\def\Kstarmp {{\ensuremath{\kaon^{*\mp}}}\xspace} + +\newcommand{\etaz}{\ensuremath{\Peta}\xspace} +\newcommand{\etapr}{\ensuremath{\Peta^{\prime}}\xspace} +\newcommand{\phiz}{\ensuremath{\Pphi}\xspace} +\newcommand{\omegaz}{\ensuremath{\Pomega}\xspace} + +%% Heavy mesons + +%%% do NOT use ensuremath here + \def\Dbar {{\kern 0.2em\overline{\kern -0.2em \PD}{}}\xspace} +\def\D {{\ensuremath{\PD}}\xspace} +\def\Db {{\ensuremath{\Dbar}}\xspace} +\def\DorDbar {\kern 0.18em\optbar{\kern -0.18em D}{}\xspace} +\def\Dz {{\ensuremath{\D^0}}\xspace} +\def\Dzb {{\ensuremath{\Dbar{}^0}}\xspace} +\def\Dp {{\ensuremath{\D^+}}\xspace} +\def\Dm {{\ensuremath{\D^-}}\xspace} +\def\Dpm {{\ensuremath{\D^\pm}}\xspace} +\def\Dmp {{\ensuremath{\D^\mp}}\xspace} +\def\Dstar {{\ensuremath{\D^*}}\xspace} +\def\Dstarb {{\ensuremath{\Dbar{}^*}}\xspace} +\def\Dstarz {{\ensuremath{\D^{*0}}}\xspace} +\def\Dstarzb {{\ensuremath{\Dbar{}^{*0}}}\xspace} +\def\Dstarp {{\ensuremath{\D^{*+}}}\xspace} +\def\Dstarm {{\ensuremath{\D^{*-}}}\xspace} +\def\Dstarpm {{\ensuremath{\D^{*\pm}}}\xspace} +\def\Dstarmp {{\ensuremath{\D^{*\mp}}}\xspace} +\def\Ds {{\ensuremath{\D^+_\squark}}\xspace} +\def\Dsp {{\ensuremath{\D^+_\squark}}\xspace} +\def\Dsm {{\ensuremath{\D^-_\squark}}\xspace} +\def\Dspm {{\ensuremath{\D^{\pm}_\squark}}\xspace} +\def\Dsmp {{\ensuremath{\D^{\mp}_\squark}}\xspace} +\def\Dss {{\ensuremath{\D^{*+}_\squark}}\xspace} +\def\Dssp {{\ensuremath{\D^{*+}_\squark}}\xspace} +\def\Dssm {{\ensuremath{\D^{*-}_\squark}}\xspace} +\def\Dsspm {{\ensuremath{\D^{*\pm}_\squark}}\xspace} +\def\Dssmp {{\ensuremath{\D^{*\mp}_\squark}}\xspace} + +\def\B {{\ensuremath{\PB}}\xspace} +%%% do NOT use ensuremath here +\def\Bbar {{\ensuremath{\kern 0.18em\overline{\kern -0.18em \PB}{}}}\xspace} +\def\Bb {{\ensuremath{\Bbar}}\xspace} +\def\BorBbar {\kern 0.18em\optbar{\kern -0.18em B}{}\xspace} +\def\Bz {{\ensuremath{\B^0}}\xspace} +\def\Bzb {{\ensuremath{\Bbar{}^0}}\xspace} +\def\Bu {{\ensuremath{\B^+}}\xspace} +\def\Bub {{\ensuremath{\B^-}}\xspace} +\def\Bp {{\ensuremath{\Bu}}\xspace} +\def\Bm {{\ensuremath{\Bub}}\xspace} +\def\Bpm {{\ensuremath{\B^\pm}}\xspace} +\def\Bmp {{\ensuremath{\B^\mp}}\xspace} +\def\Bd {{\ensuremath{\B^0}}\xspace} +\def\Bs {{\ensuremath{\B^0_\squark}}\xspace} +\def\Bsb {{\ensuremath{\Bbar{}^0_\squark}}\xspace} +\def\Bdb {{\ensuremath{\Bbar{}^0}}\xspace} +\def\Bc {{\ensuremath{\B_\cquark^+}}\xspace} +\def\Bcp {{\ensuremath{\B_\cquark^+}}\xspace} +\def\Bcm {{\ensuremath{\B_\cquark^-}}\xspace} +\def\Bcpm {{\ensuremath{\B_\cquark^\pm}}\xspace} + +%% Onia + +\def\jpsi {{\ensuremath{{\PJ\mskip -3mu/\mskip -2mu\Ppsi\mskip 2mu}}}\xspace} +\def\psitwos {{\ensuremath{\Ppsi{(2S)}}}\xspace} +\def\psiprpr {{\ensuremath{\Ppsi(3770)}}\xspace} +\def\etac {{\ensuremath{\Peta_\cquark}}\xspace} +\def\chiczero {{\ensuremath{\Pchi_{\cquark 0}}}\xspace} +\def\chicone {{\ensuremath{\Pchi_{\cquark 1}}}\xspace} +\def\chictwo {{\ensuremath{\Pchi_{\cquark 2}}}\xspace} + %\mathchardef\Upsilon="7107 + \def\Y#1S{\ensuremath{\PUpsilon{(#1S)}}\xspace}% no space before {...}! +\def\OneS {{\Y1S}} +\def\TwoS {{\Y2S}} +\def\ThreeS{{\Y3S}} +\def\FourS {{\Y4S}} +\def\FiveS {{\Y5S}} + +\def\chic {{\ensuremath{\Pchi_{c}}}\xspace} + +%% Baryons + +\def\proton {{\ensuremath{\Pp}}\xspace} +\def\antiproton {{\ensuremath{\overline \proton}}\xspace} +\def\neutron {{\ensuremath{\Pn}}\xspace} +\def\antineutron {{\ensuremath{\overline \neutron}}\xspace} +\def\Deltares {{\ensuremath{\PDelta}}\xspace} +\def\Deltaresbar {{\ensuremath{\overline \Deltares}}\xspace} +\def\Xires {{\ensuremath{\PXi}}\xspace} +\def\Xiresbar {{\ensuremath{\overline \Xires}}\xspace} +\def\Lz {{\ensuremath{\PLambda}}\xspace} +\def\Lbar {{\ensuremath{\kern 0.1em\overline{\kern -0.1em\PLambda}}}\xspace} +\def\LorLbar {\kern 0.18em\optbar{\kern -0.18em \PLambda}{}\xspace} +\def\Lambdares {{\ensuremath{\PLambda}}\xspace} +\def\Lambdaresbar{{\ensuremath{\Lbar}}\xspace} +\def\Sigmares {{\ensuremath{\PSigma}}\xspace} +\def\Sigmaresbar {{\ensuremath{\overline \Sigmares}}\xspace} +\def\Omegares {{\ensuremath{\POmega}}\xspace} +\def\Omegaresbar {{\ensuremath{\overline \POmega}}\xspace} + +%%% do NOT use ensuremath here + % \def\Deltabar{\kern 0.25em\overline{\kern -0.25em \Deltares}{}\xspace} + % \def\Sigbar{\kern 0.2em\overline{\kern -0.2em \Sigma}{}\xspace} + % \def\Xibar{\kern 0.2em\overline{\kern -0.2em \Xi}{}\xspace} + % \def\Obar{\kern 0.2em\overline{\kern -0.2em \Omega}{}\xspace} + % \def\Nbar{\kern 0.2em\overline{\kern -0.2em N}{}\xspace} + % \def\Xb{\kern 0.2em\overline{\kern -0.2em X}{}\xspace} + +\def\Lb {{\ensuremath{\Lz^0_\bquark}}\xspace} +\def\Lbbar {{\ensuremath{\Lbar{}^0_\bquark}}\xspace} +\def\Lc {{\ensuremath{\Lz^+_\cquark}}\xspace} +\def\Lcbar {{\ensuremath{\Lbar{}^-_\cquark}}\xspace} +\def\Xib {{\ensuremath{\Xires_\bquark}}\xspace} +\def\Xibz {{\ensuremath{\Xires^0_\bquark}}\xspace} +\def\Xibm {{\ensuremath{\Xires^-_\bquark}}\xspace} +\def\Xibbar {{\ensuremath{\Xiresbar{}_\bquark}}\xspace} +\def\Xibbarz {{\ensuremath{\Xiresbar{}_\bquark^0}}\xspace} +\def\Xibbarp {{\ensuremath{\Xiresbar{}_\bquark^+}}\xspace} +\def\Xic {{\ensuremath{\Xires_\cquark}}\xspace} +\def\Xicz {{\ensuremath{\Xires^0_\cquark}}\xspace} +\def\Xicp {{\ensuremath{\Xires^+_\cquark}}\xspace} +\def\Xicbar {{\ensuremath{\Xiresbar{}_\cquark}}\xspace} +\def\Xicbarz {{\ensuremath{\Xiresbar{}_\cquark^0}}\xspace} +\def\Xicbarm {{\ensuremath{\Xiresbar{}_\cquark^-}}\xspace} +\def\Omegac {{\ensuremath{\Omegares^0_\cquark}}\xspace} +\def\Omegacbar {{\ensuremath{\Omegaresbar{}_\cquark^0}}\xspace} +\def\Omegab {{\ensuremath{\Omegares^-_\bquark}}\xspace} +\def\Omegabbar {{\ensuremath{\Omegaresbar{}_\bquark^+}}\xspace} + +%%%%%%%%%%%%%%%%%% +% Physics symbols +%%%%%%%%%%%%%%%%% + +%% Decays +\def\BF {{\ensuremath{\mathcal{B}}}\xspace} +\def\BRvis {{\ensuremath{\BR_{\mathrm{{vis}}}}}} +\def\BR {\BF} +\newcommand{\decay}[2]{\ensuremath{#1\!\to #2}\xspace} % {\Pa}{\Pb \Pc} +\def\ra {\ensuremath{\rightarrow}\xspace} +\def\to {\ensuremath{\rightarrow}\xspace} + +%% Lifetimes +\newcommand{\tauBs}{{\ensuremath{\tau_{\Bs}}}\xspace} +\newcommand{\tauBd}{{\ensuremath{\tau_{\Bd}}}\xspace} +\newcommand{\tauBz}{{\ensuremath{\tau_{\Bz}}}\xspace} +\newcommand{\tauBu}{{\ensuremath{\tau_{\Bp}}}\xspace} +\newcommand{\tauDp}{{\ensuremath{\tau_{\Dp}}}\xspace} +\newcommand{\tauDz}{{\ensuremath{\tau_{\Dz}}}\xspace} +\newcommand{\tauL}{{\ensuremath{\tau_{\mathrm{ L}}}}\xspace} +\newcommand{\tauH}{{\ensuremath{\tau_{\mathrm{ H}}}}\xspace} + +%% Masses +\newcommand{\mBd}{{\ensuremath{m_{\Bd}}}\xspace} +\newcommand{\mBp}{{\ensuremath{m_{\Bp}}}\xspace} +\newcommand{\mBs}{{\ensuremath{m_{\Bs}}}\xspace} +\newcommand{\mBc}{{\ensuremath{m_{\Bc}}}\xspace} +\newcommand{\mLb}{{\ensuremath{m_{\Lb}}}\xspace} + +%% EW theory, groups +\def\grpsuthree {{\ensuremath{\mathrm{SU}(3)}}\xspace} +\def\grpsutw {{\ensuremath{\mathrm{SU}(2)}}\xspace} +\def\grpuone {{\ensuremath{\mathrm{U}(1)}}\xspace} + +\def\ssqtw {{\ensuremath{\sin^{2}\!\theta_{\mathrm{W}}}}\xspace} +\def\csqtw {{\ensuremath{\cos^{2}\!\theta_{\mathrm{W}}}}\xspace} +\def\stw {{\ensuremath{\sin\theta_{\mathrm{W}}}}\xspace} +\def\ctw {{\ensuremath{\cos\theta_{\mathrm{W}}}}\xspace} +\def\ssqtwef {{\ensuremath{{\sin}^{2}\theta_{\mathrm{W}}^{\mathrm{eff}}}}\xspace} +\def\csqtwef {{\ensuremath{{\cos}^{2}\theta_{\mathrm{W}}^{\mathrm{eff}}}}\xspace} +\def\stwef {{\ensuremath{\sin\theta_{\mathrm{W}}^{\mathrm{eff}}}}\xspace} +\def\ctwef {{\ensuremath{\cos\theta_{\mathrm{W}}^{\mathrm{eff}}}}\xspace} +\def\gv {{\ensuremath{g_{\mbox{\tiny V}}}}\xspace} +\def\ga {{\ensuremath{g_{\mbox{\tiny A}}}}\xspace} + +\def\order {{\ensuremath{\mathcal{O}}}\xspace} +\def\ordalph {{\ensuremath{\mathcal{O}(\alpha)}}\xspace} +\def\ordalsq {{\ensuremath{\mathcal{O}(\alpha^{2})}}\xspace} +\def\ordalcb {{\ensuremath{\mathcal{O}(\alpha^{3})}}\xspace} + +%% QCD parameters +\newcommand{\as}{{\ensuremath{\alpha_s}}\xspace} +\newcommand{\MSb}{{\ensuremath{\overline{\mathrm{MS}}}}\xspace} +\newcommand{\lqcd}{{\ensuremath{\Lambda_{\mathrm{QCD}}}}\xspace} +\def\qsq {{\ensuremath{q^2}}\xspace} + +%% CKM, CP violation + +\def\eps {{\ensuremath{\varepsilon}}\xspace} +\def\epsK {{\ensuremath{\varepsilon_K}}\xspace} +\def\epsB {{\ensuremath{\varepsilon_B}}\xspace} +\def\epsp {{\ensuremath{\varepsilon^\prime_K}}\xspace} + +\def\CP {{\ensuremath{C\!P}}\xspace} +\def\CPT {{\ensuremath{C\!PT}}\xspace} + +\def\rhobar {{\ensuremath{\overline \rho}}\xspace} +\def\etabar {{\ensuremath{\overline \eta}}\xspace} + +\def\Vud {{\ensuremath{V_{\uquark\dquark}}}\xspace} +\def\Vcd {{\ensuremath{V_{\cquark\dquark}}}\xspace} +\def\Vtd {{\ensuremath{V_{\tquark\dquark}}}\xspace} +\def\Vus {{\ensuremath{V_{\uquark\squark}}}\xspace} +\def\Vcs {{\ensuremath{V_{\cquark\squark}}}\xspace} +\def\Vts {{\ensuremath{V_{\tquark\squark}}}\xspace} +\def\Vub {{\ensuremath{V_{\uquark\bquark}}}\xspace} +\def\Vcb {{\ensuremath{V_{\cquark\bquark}}}\xspace} +\def\Vtb {{\ensuremath{V_{\tquark\bquark}}}\xspace} +\def\Vuds {{\ensuremath{V_{\uquark\dquark}^\ast}}\xspace} +\def\Vcds {{\ensuremath{V_{\cquark\dquark}^\ast}}\xspace} +\def\Vtds {{\ensuremath{V_{\tquark\dquark}^\ast}}\xspace} +\def\Vuss {{\ensuremath{V_{\uquark\squark}^\ast}}\xspace} +\def\Vcss {{\ensuremath{V_{\cquark\squark}^\ast}}\xspace} +\def\Vtss {{\ensuremath{V_{\tquark\squark}^\ast}}\xspace} +\def\Vubs {{\ensuremath{V_{\uquark\bquark}^\ast}}\xspace} +\def\Vcbs {{\ensuremath{V_{\cquark\bquark}^\ast}}\xspace} +\def\Vtbs {{\ensuremath{V_{\tquark\bquark}^\ast}}\xspace} + +%% Oscillations + +\newcommand{\dm}{{\ensuremath{\Delta m}}\xspace} +\newcommand{\dms}{{\ensuremath{\Delta m_{\squark}}}\xspace} +\newcommand{\dmd}{{\ensuremath{\Delta m_{\dquark}}}\xspace} +\newcommand{\DG}{{\ensuremath{\Delta\Gamma}}\xspace} +\newcommand{\DGs}{{\ensuremath{\Delta\Gamma_{\squark}}}\xspace} +\newcommand{\DGd}{{\ensuremath{\Delta\Gamma_{\dquark}}}\xspace} +\newcommand{\Gs}{{\ensuremath{\Gamma_{\squark}}}\xspace} +\newcommand{\Gd}{{\ensuremath{\Gamma_{\dquark}}}\xspace} +\newcommand{\MBq}{{\ensuremath{M_{\B_\quark}}}\xspace} +\newcommand{\DGq}{{\ensuremath{\Delta\Gamma_{\quark}}}\xspace} +\newcommand{\Gq}{{\ensuremath{\Gamma_{\quark}}}\xspace} +\newcommand{\dmq}{{\ensuremath{\Delta m_{\quark}}}\xspace} +\newcommand{\GL}{{\ensuremath{\Gamma_{\mathrm{ L}}}}\xspace} +\newcommand{\GH}{{\ensuremath{\Gamma_{\mathrm{ H}}}}\xspace} +\newcommand{\DGsGs}{{\ensuremath{\Delta\Gamma_{\squark}/\Gamma_{\squark}}}\xspace} +\newcommand{\Delm}{{\mbox{$\Delta m $}}\xspace} +\newcommand{\ACP}{{\ensuremath{{\mathcal{A}}^{\CP}}}\xspace} +\newcommand{\Adir}{{\ensuremath{{\mathcal{A}}^{\mathrm{ dir}}}}\xspace} +\newcommand{\Amix}{{\ensuremath{{\mathcal{A}}^{\mathrm{ mix}}}}\xspace} +\newcommand{\ADelta}{{\ensuremath{{\mathcal{A}}^\Delta}}\xspace} +\newcommand{\phid}{{\ensuremath{\phi_{\dquark}}}\xspace} +\newcommand{\sinphid}{{\ensuremath{\sin\!\phid}}\xspace} +\newcommand{\phis}{{\ensuremath{\phi_{\squark}}}\xspace} +\newcommand{\betas}{{\ensuremath{\beta_{\squark}}}\xspace} +\newcommand{\sbetas}{{\ensuremath{\sigma(\beta_{\squark})}}\xspace} +\newcommand{\stbetas}{{\ensuremath{\sigma(2\beta_{\squark})}}\xspace} +\newcommand{\stphis}{{\ensuremath{\sigma(\phi_{\squark})}}\xspace} +\newcommand{\sinphis}{{\ensuremath{\sin\!\phis}}\xspace} + +%% Tagging +\newcommand{\edet}{{\ensuremath{\varepsilon_{\mathrm{ det}}}}\xspace} +\newcommand{\erec}{{\ensuremath{\varepsilon_{\mathrm{ rec/det}}}}\xspace} +\newcommand{\esel}{{\ensuremath{\varepsilon_{\mathrm{ sel/rec}}}}\xspace} +\newcommand{\etrg}{{\ensuremath{\varepsilon_{\mathrm{ trg/sel}}}}\xspace} +\newcommand{\etot}{{\ensuremath{\varepsilon_{\mathrm{ tot}}}}\xspace} + +\newcommand{\mistag}{\ensuremath{\omega}\xspace} +\newcommand{\wcomb}{\ensuremath{\omega^{\mathrm{comb}}}\xspace} +\newcommand{\etag}{{\ensuremath{\varepsilon_{\mathrm{tag}}}}\xspace} +\newcommand{\etagcomb}{{\ensuremath{\varepsilon_{\mathrm{tag}}^{\mathrm{comb}}}}\xspace} +\newcommand{\effeff}{\ensuremath{\varepsilon_{\mathrm{eff}}}\xspace} +\newcommand{\effeffcomb}{\ensuremath{\varepsilon_{\mathrm{eff}}^{\mathrm{comb}}}\xspace} +\newcommand{\efftag}{{\ensuremath{\etag(1-2\omega)^2}}\xspace} +\newcommand{\effD}{{\ensuremath{\etag D^2}}\xspace} + +\newcommand{\etagprompt}{{\ensuremath{\varepsilon_{\mathrm{ tag}}^{\mathrm{Pr}}}}\xspace} +\newcommand{\etagLL}{{\ensuremath{\varepsilon_{\mathrm{ tag}}^{\mathrm{LL}}}}\xspace} + +%% Key decay channels + +\def\BdToKstmm {\decay{\Bd}{\Kstarz\mup\mun}} +\def\BdbToKstmm {\decay{\Bdb}{\Kstarzb\mup\mun}} + +\def\BsToJPsiPhi {\decay{\Bs}{\jpsi\phi}} +\def\BdToJPsiKst {\decay{\Bd}{\jpsi\Kstarz}} +\def\BdbToJPsiKst {\decay{\Bdb}{\jpsi\Kstarzb}} + +\def\BsPhiGam {\decay{\Bs}{\phi \g}} +\def\BdKstGam {\decay{\Bd}{\Kstarz \g}} + +\def\BTohh {\decay{\B}{\Ph^+ \Ph'^-}} +\def\BdTopipi {\decay{\Bd}{\pip\pim}} +\def\BdToKpi {\decay{\Bd}{\Kp\pim}} +\def\BsToKK {\decay{\Bs}{\Kp\Km}} +\def\BsTopiK {\decay{\Bs}{\pip\Km}} + + + + + +%% Rare decays +\def\BdKstee {\decay{\Bd}{\Kstarz\epem}} +\def\BdbKstee {\decay{\Bdb}{\Kstarzb\epem}} +\def\bsll {\decay{\bquark}{\squark \ell^+ \ell^-}} +\def\AFB {\ensuremath{A_{\mathrm{FB}}}\xspace} +\def\FL {\ensuremath{F_{\mathrm{L}}}\xspace} +\def\AT#1 {\ensuremath{A_{\mathrm{T}}^{#1}}\xspace} % 2 +\def\btosgam {\decay{\bquark}{\squark \g}} +\def\btodgam {\decay{\bquark}{\dquark \g}} +\def\Bsmm {\decay{\Bs}{\mup\mun}} +\def\Bdmm {\decay{\Bd}{\mup\mun}} +\def\ctl {\ensuremath{\cos{\theta_\ell}}\xspace} +\def\ctk {\ensuremath{\cos{\theta_K}}\xspace} + +\def\BToKem {\decay{\Bp}{\Kp \mupm \emp}} +\def\BToKemp {\decay{\Bp}{\Kp \mup \en}} +\def\BToKemm {\decay{\Bp}{\Kp \mun \ep}} +\def\BToKemSS {\decay{\Bp}{\Kp \mun \en}} +\def\BToJpsiK {\decay{\Bp}{\Kp \jpsi ( \to \mup \mun)}} +\def\BToKmumu {\decay{\Bp}{\Kp \mup \mun}} +\def\BToKee {\decay{\Bp}{\Kp \ep \en}} +\def\BToJpsieeK {\decay{\Bp}{\Kp \jpsi ( \to \ep \en)}} + +\def\BToKmtau {\decay{\Bp}{\Kp \mupm \Ptau^{\mp} }} + + +%% Wilson coefficients and operators +\def\C#1 {\ensuremath{\mathcal{C}_{#1}}\xspace} % 9 +\def\Cp#1 {\ensuremath{\mathcal{C}_{#1}^{'}}\xspace} % 7 +\def\Ceff#1 {\ensuremath{\mathcal{C}_{#1}^{\mathrm{(eff)}}}\xspace} % 9 +\def\Cpeff#1 {\ensuremath{\mathcal{C}_{#1}^{'\mathrm{(eff)}}}\xspace} % 7 +\def\Ope#1 {\ensuremath{\mathcal{O}_{#1}}\xspace} % 2 +\def\Opep#1 {\ensuremath{\mathcal{O}_{#1}^{'}}\xspace} % 7 + +%% Charm + +\def\xprime {\ensuremath{x^{\prime}}\xspace} +\def\yprime {\ensuremath{y^{\prime}}\xspace} +\def\ycp {\ensuremath{y_{\CP}}\xspace} +\def\agamma {\ensuremath{A_{\Gamma}}\xspace} +%%%\def\kpi {\ensuremath{\PK\Ppi}\xspace} +%%%\def\kk {\ensuremath{\PK\PK}\xspace} +%%%\def\dkpi {\decay{\PD}{\PK\Ppi}} +%%%\def\dkk {\decay{\PD}{\PK\PK}} +\def\dkpicf {\decay{\Dz}{\Km\pip}} + +%% QM +\newcommand{\bra}[1]{\ensuremath{\langle #1|}} % {a} +\newcommand{\ket}[1]{\ensuremath{|#1\rangle}} % {b} +\newcommand{\braket}[2]{\ensuremath{\langle #1|#2\rangle}} % {a}{b} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Units +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\newcommand{\unit}[1]{\ensuremath{\mathrm{ \,#1}}\xspace} % {kg} + +%% Energy and momentum +\newcommand{\tev}{\ifthenelse{\boolean{inbibliography}}{\ensuremath{~T\kern -0.05em eV}\xspace}{\ensuremath{\mathrm{\,Te\kern -0.1em V}}}\xspace} +\newcommand{\gev}{\ensuremath{\mathrm{\,Ge\kern -0.1em V}}\xspace} +\newcommand{\mev}{\ensuremath{\mathrm{\,Me\kern -0.1em V}}\xspace} +\newcommand{\kev}{\ensuremath{\mathrm{\,ke\kern -0.1em V}}\xspace} +\newcommand{\ev}{\ensuremath{\mathrm{\,e\kern -0.1em V}}\xspace} +\newcommand{\gevc}{\ensuremath{{\mathrm{\,Ge\kern -0.1em V\!/}c}}\xspace} +\newcommand{\mevc}{\ensuremath{{\mathrm{\,Me\kern -0.1em V\!/}c}}\xspace} +\newcommand{\gevcc}{\ensuremath{{\mathrm{\,Ge\kern -0.1em V\!/}c^2}}\xspace} +\newcommand{\gevgevcccc}{\ensuremath{{\mathrm{\,Ge\kern -0.1em V^2\!/}c^4}}\xspace} +\newcommand{\mevcc}{\ensuremath{{\mathrm{\,Me\kern -0.1em V\!/}c^2}}\xspace} + +%% Distance and area +\def\km {\ensuremath{\mathrm{ \,km}}\xspace} +\def\m {\ensuremath{\mathrm{ \,m}}\xspace} +\def\ma {\ensuremath{{\mathrm{ \,m}}^2}\xspace} +\def\cm {\ensuremath{\mathrm{ \,cm}}\xspace} +\def\cma {\ensuremath{{\mathrm{ \,cm}}^2}\xspace} +\def\mm {\ensuremath{\mathrm{ \,mm}}\xspace} +\def\mma {\ensuremath{{\mathrm{ \,mm}}^2}\xspace} +\def\mum {\ensuremath{{\,\upmu\mathrm{m}}}\xspace} +\def\muma {\ensuremath{{\,\upmu\mathrm{m}^2}}\xspace} +\def\nm {\ensuremath{\mathrm{ \,nm}}\xspace} +\def\fm {\ensuremath{\mathrm{ \,fm}}\xspace} +\def\barn{\ensuremath{\mathrm{ \,b}}\xspace} +%%%\def\barnhyph{\ensuremath{\mathrm{ -b}}\xspace} +\def\mbarn{\ensuremath{\mathrm{ \,mb}}\xspace} +\def\mub{\ensuremath{{\mathrm{ \,\upmu b}}}\xspace} +%%%\def\mbarnhyph{\ensuremath{\mathrm{ -mb}}\xspace} +\def\nb {\ensuremath{\mathrm{ \,nb}}\xspace} +\def\invnb {\ensuremath{\mbox{\,nb}^{-1}}\xspace} +\def\pb {\ensuremath{\mathrm{ \,pb}}\xspace} +\def\invpb {\ensuremath{\mbox{\,pb}^{-1}}\xspace} +\def\fb {\ensuremath{\mbox{\,fb}}\xspace} +\def\invfb {\ensuremath{\mbox{\,fb}^{-1}}\xspace} +\def\ab {\ensuremath{\mbox{\,ab}}\xspace} +\def\invab {\ensuremath{\mbox{\,ab}^{-1}}\xspace} + +%% Time +\def\sec {\ensuremath{\mathrm{{\,s}}}\xspace} +\def\ms {\ensuremath{{\mathrm{ \,ms}}}\xspace} +\def\mus {\ensuremath{{\,\upmu{\mathrm{ s}}}}\xspace} +\def\ns {\ensuremath{{\mathrm{ \,ns}}}\xspace} +\def\ps {\ensuremath{{\mathrm{ \,ps}}}\xspace} +\def\fs {\ensuremath{\mathrm{ \,fs}}\xspace} + +\def\mhz {\ensuremath{{\mathrm{ \,MHz}}}\xspace} +\def\khz {\ensuremath{{\mathrm{ \,kHz}}}\xspace} +\def\hz {\ensuremath{{\mathrm{ \,Hz}}}\xspace} + +\def\invps{\ensuremath{{\mathrm{ \,ps^{-1}}}}\xspace} +\def\invns{\ensuremath{{\mathrm{ \,ns^{-1}}}}\xspace} + +\def\yr {\ensuremath{\mathrm{ \,yr}}\xspace} +\def\hr {\ensuremath{\mathrm{ \,hr}}\xspace} + +%% Temperature +\def\degc {\ensuremath{^\circ}{C}\xspace} +\def\degk {\ensuremath {\mathrm{ K}}\xspace} + +%% Material lengths, radiation +\def\Xrad {\ensuremath{X_0}\xspace} +\def\NIL{\ensuremath{\lambda_{int}}\xspace} +\def\mip {MIP\xspace} +\def\neutroneq {\ensuremath{\mathrm{ \,n_{eq}}}\xspace} +\def\neqcmcm {\ensuremath{\mathrm{ \,n_{eq} / cm^2}}\xspace} +\def\kRad {\ensuremath{\mathrm{ \,kRad}}\xspace} +\def\MRad {\ensuremath{\mathrm{ \,MRad}}\xspace} +\def\ci {\ensuremath{\mathrm{ \,Ci}}\xspace} +\def\mci {\ensuremath{\mathrm{ \,mCi}}\xspace} + +%% Uncertainties +\def\sx {\ensuremath{\sigma_x}\xspace} +\def\sy {\ensuremath{\sigma_y}\xspace} +\def\sz {\ensuremath{\sigma_z}\xspace} + +\newcommand{\stat}{\ensuremath{\mathrm{\,(stat)}}\xspace} +\newcommand{\syst}{\ensuremath{\mathrm{\,(syst)}}\xspace} + +%% Maths + +\def\order{{\ensuremath{\mathcal{O}}}\xspace} +\newcommand{\chisq}{\ensuremath{\chi^2}\xspace} +\newcommand{\chisqndf}{\ensuremath{\chi^2/\mathrm{ndf}}\xspace} +\newcommand{\chisqip}{\ensuremath{\chi^2_{\text{IP}}}\xspace} +\newcommand{\chisqvs}{\ensuremath{\chi^2_{\text{VS}}}\xspace} +\newcommand{\chisqvtx}{\ensuremath{\chi^2_{\text{vtx}}}\xspace} +\newcommand{\chisqvtxndf}{\ensuremath{\chi^2_{\text{vtx}}/\mathrm{ndf}}\xspace} + +\def\deriv {\ensuremath{\mathrm{d}}} + +\def\gsim{{~\raise.15em\hbox{$>$}\kern-.85em + \lower.35em\hbox{$\sim$}~}\xspace} +\def\lsim{{~\raise.15em\hbox{$<$}\kern-.85em + \lower.35em\hbox{$\sim$}~}\xspace} + +\newcommand{\mean}[1]{\ensuremath{\left\langle #1 \right\rangle}} % {x} +\newcommand{\abs}[1]{\ensuremath{\left\|#1\right\|}} % {x} +\newcommand{\Real}{\ensuremath{\mathcal{R}e}\xspace} +\newcommand{\Imag}{\ensuremath{\mathcal{I}m}\xspace} + +\def\PDF {PDF\xspace} + +\def\sPlot{\mbox{\em sPlot}\xspace} +%%%\def\sWeight{\mbox{\em sWeight}\xspace} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Kinematics +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +%% Energy, Momenta +\def\Ebeam {\ensuremath{E_{\mbox{\tiny BEAM}}}\xspace} +\def\sqs {\ensuremath{\protect\sqrt{s}}\xspace} + +\def\ptot {\mbox{$p$}\xspace} +\def\pt {\mbox{$p_{\mathrm{ T}}$}\xspace} +\def\et {\mbox{$E_{\mathrm{ T}}$}\xspace} +\def\mt {\mbox{$M_{\mathrm{ T}}$}\xspace} +\def\dpp {\ensuremath{\Delta p/p}\xspace} +\def\msq {\ensuremath{m^2}\xspace} +\newcommand{\dedx}{\ensuremath{\mathrm{d}\hspace{-0.1em}E/\mathrm{d}x}\xspace} + +%% PID + +\def\dllkpi {\ensuremath{\mathrm{DLL}_{\kaon\pion}}\xspace} +\def\dllppi {\ensuremath{\mathrm{DLL}_{\proton\pion}}\xspace} +\def\dllepi {\ensuremath{\mathrm{DLL}_{\electron\pion}}\xspace} +\def\dllmupi {\ensuremath{\mathrm{DLL}_{\muon\pi}}\xspace} + +%% Geometry +%%%\def\mphi {\mbox{$\phi$}\xspace} +%%%\def\mtheta {\mbox{$\theta$}\xspace} +%%%\def\ctheta {\mbox{$\cos\theta$}\xspace} +%%%\def\stheta {\mbox{$\sin\theta$}\xspace} +%%%\def\ttheta {\mbox{$\tan\theta$}\xspace} + +\def\degrees{\ensuremath{^{\circ}}\xspace} +\def\krad {\ensuremath{\mathrm{ \,krad}}\xspace} +\def\mrad{\ensuremath{\mathrm{ \,mrad}}\xspace} +\def\rad{\ensuremath{\mathrm{ \,rad}}\xspace} + +%% Accelerator +\def\betastar {\ensuremath{\beta^*}} +\newcommand{\lum} {\ensuremath{\mathcal{L}}\xspace} +\newcommand{\intlum}[1]{\ensuremath{\int\lum=#1}\xspace} % {2 \,\invfb} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Software +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +%% Programs +%%%\def\ansys {\mbox{\textsc{Ansys}}\xspace} +\def\bcvegpy {\mbox{\textsc{Bcvegpy}}\xspace} +\def\boole {\mbox{\textsc{Boole}}\xspace} +\def\brunel {\mbox{\textsc{Brunel}}\xspace} +\def\davinci {\mbox{\textsc{DaVinci}}\xspace} +\def\dirac {\mbox{\textsc{Dirac}}\xspace} +%%%\def\erasmus {\mbox{\textsc{Erasmus}}\xspace} +\def\evtgen {\mbox{\textsc{EvtGen}}\xspace} +\def\fewz {\mbox{\textsc{Fewz}}\xspace} +\def\fluka {\mbox{\textsc{Fluka}}\xspace} +\def\ganga {\mbox{\textsc{Ganga}}\xspace} +%%%\def\garfield {\mbox{\textsc{Garfield}}\xspace} +\def\gaudi {\mbox{\textsc{Gaudi}}\xspace} +\def\gauss {\mbox{\textsc{Gauss}}\xspace} +\def\geant {\mbox{\textsc{Geant4}}\xspace} +\def\hepmc {\mbox{\textsc{HepMC}}\xspace} +\def\herwig {\mbox{\textsc{Herwig}}\xspace} +\def\moore {\mbox{\textsc{Moore}}\xspace} +\def\neurobayes {\mbox{\textsc{NeuroBayes}}\xspace} +\def\photos {\mbox{\textsc{Photos}}\xspace} +\def\powheg {\mbox{\textsc{Powheg}}\xspace} +%%%\def\pyroot {\mbox{\textsc{PyRoot}}\xspace} +\def\pythia {\mbox{\textsc{Pythia}}\xspace} +\def\resbos {\mbox{\textsc{ResBos}}\xspace} +\def\roofit {\mbox{\textsc{RooFit}}\xspace} +\def\root {\mbox{\textsc{Root}}\xspace} +\def\spice {\mbox{\textsc{Spice}}\xspace} +%%%\def\tosca {\mbox{\textsc{Tosca}}\xspace} +\def\urania {\mbox{\textsc{Urania}}\xspace} + +%% Languages +\def\cpp {\mbox{\textsc{C\raisebox{0.1em}{{\footnotesize{++}}}}}\xspace} +%%%\def\python {\mbox{\textsc{Python}}\xspace} +\def\ruby {\mbox{\textsc{Ruby}}\xspace} +\def\fortran {\mbox{\textsc{Fortran}}\xspace} +\def\svn {\mbox{\textsc{SVN}}\xspace} + +%% Data processing +\def\kbytes {\ensuremath{{\mathrm{ \,kbytes}}}\xspace} +\def\kbsps {\ensuremath{{\mathrm{ \,kbytes/s}}}\xspace} +\def\kbits {\ensuremath{{\mathrm{ \,kbits}}}\xspace} +\def\kbsps {\ensuremath{{\mathrm{ \,kbits/s}}}\xspace} +\def\mbsps {\ensuremath{{\mathrm{ \,Mbits/s}}}\xspace} +\def\mbytes {\ensuremath{{\mathrm{ \,Mbytes}}}\xspace} +\def\mbps {\ensuremath{{\mathrm{ \,Mbyte/s}}}\xspace} +\def\mbsps {\ensuremath{{\mathrm{ \,Mbytes/s}}}\xspace} +\def\gbsps {\ensuremath{{\mathrm{ \,Gbits/s}}}\xspace} +\def\gbytes {\ensuremath{{\mathrm{ \,Gbytes}}}\xspace} +\def\gbsps {\ensuremath{{\mathrm{ \,Gbytes/s}}}\xspace} +\def\tbytes {\ensuremath{{\mathrm{ \,Tbytes}}}\xspace} +\def\tbpy {\ensuremath{{\mathrm{ \,Tbytes/yr}}}\xspace} + +\def\dst {DST\xspace} + +%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Detector related +%%%%%%%%%%%%%%%%%%%%%%%%%%% + +%% Detector technologies +\def\nonn {\ensuremath{\mathrm{{ \mathit{n^+}} \mbox{-} on\mbox{-}{ \mathit{n}}}}\xspace} +\def\ponn {\ensuremath{\mathrm{{ \mathit{p^+}} \mbox{-} on\mbox{-}{ \mathit{n}}}}\xspace} +\def\nonp {\ensuremath{\mathrm{{ \mathit{n^+}} \mbox{-} on\mbox{-}{ \mathit{p}}}}\xspace} +\def\cvd {CVD\xspace} +\def\mwpc {MWPC\xspace} +\def\gem {GEM\xspace} + +%% Detector components, electronics +\def\tell1 {TELL1\xspace} +\def\ukl1 {UKL1\xspace} +\def\beetle {Beetle\xspace} +\def\otis {OTIS\xspace} +\def\croc {CROC\xspace} +\def\carioca {CARIOCA\xspace} +\def\dialog {DIALOG\xspace} +\def\sync {SYNC\xspace} +\def\cardiac {CARDIAC\xspace} +\def\gol {GOL\xspace} +\def\vcsel {VCSEL\xspace} +\def\ttc {TTC\xspace} +\def\ttcrx {TTCrx\xspace} +\def\hpd {HPD\xspace} +\def\pmt {PMT\xspace} +\def\specs {SPECS\xspace} +\def\elmb {ELMB\xspace} +\def\fpga {FPGA\xspace} +\def\plc {PLC\xspace} +\def\rasnik {RASNIK\xspace} +\def\elmb {ELMB\xspace} +\def\can {CAN\xspace} +\def\lvds {LVDS\xspace} +\def\ntc {NTC\xspace} +\def\adc {ADC\xspace} +\def\led {LED\xspace} +\def\ccd {CCD\xspace} +\def\hv {HV\xspace} +\def\lv {LV\xspace} +\def\pvss {PVSS\xspace} +\def\cmos {CMOS\xspace} +\def\fifo {FIFO\xspace} +\def\ccpc {CCPC\xspace} + +%% Chemical symbols +\def\cfourften {\ensuremath{\mathrm{ C_4 F_{10}}}\xspace} +\def\cffour {\ensuremath{\mathrm{ CF_4}}\xspace} +\def\cotwo {\ensuremath{\mathrm{ CO_2}}\xspace} +\def\csixffouteen {\ensuremath{\mathrm{ C_6 F_{14}}}\xspace} +\def\mgftwo {\ensuremath{\mathrm{ Mg F_2}}\xspace} +\def\siotwo {\ensuremath{\mathrm{ SiO_2}}\xspace} + +%%%%%%%%%%%%%%% +% Special Text +%%%%%%%%%%%%%%% +\newcommand{\eg}{\mbox{\itshape e.g.}\xspace} +\newcommand{\ie}{\mbox{\itshape i.e.}\xspace} +\newcommand{\etal}{\mbox{\itshape et al.}\xspace} +\newcommand{\etc}{\mbox{\itshape etc.}\xspace} +\newcommand{\cf}{\mbox{\itshape cf.}\xspace} +\newcommand{\ffp}{\mbox{\itshape ff.}\xspace} +\newcommand{\vs}{\mbox{\itshape vs.}\xspace} + +\def\fixme{{\color{red}{FIXME!}\xspace}} + + + + + diff --git a/B2Kemu/Col_aproval/mchrzasz+mp.sh b/B2Kemu/Col_aproval/mchrzasz+mp.sh new file mode 100644 index 0000000..1a24852 --- /dev/null +++ b/B2Kemu/Col_aproval/mchrzasz+mp.sh @@ -0,0 +1 @@ +#!/bin/sh diff --git a/B2Kemu/Col_aproval/mchrzasz-blx.bib b/B2Kemu/Col_aproval/mchrzasz-blx.bib new file mode 100644 index 0000000..fa04f16 --- /dev/null +++ b/B2Kemu/Col_aproval/mchrzasz-blx.bib @@ -0,0 +1,11 @@ +@Comment{$ biblatex control file $} +@Comment{$ biblatex version 2.6 $} +Do not modify this file! + +This is an auxiliary file used by the 'biblatex' package. +This file may safely be deleted. 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watermark=BG_lower, % png file for the watermark + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\TeV}{\mathrm{TeV}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mil +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} +\def\fixme{FIXME} +\def\ep{e^+} +\def\en{e^-} +\def\Lb {\Lambda_b} +\newcommand{\BToKemu}{\ensuremath{\PB^+ \to \PK^+ \mu^{\pm} e^{\mp}}} +\newcommand{\BToKem}{\ensuremath{\PB^+ \to \PK^+ \mu^{\pm} e^{\mp}}} +\newcommand{\BToKemm}{\ensuremath{\PB^+ \to \PK^+ \mu^- e^+}} +\newcommand{\BToKemp}{\ensuremath{\PB^+ \to \PK^+ \mu^+ e^-}} +\newcommand{\BTJpsiK }{\ensuremath{\PB^+ \to \PK^+ \PJpsi (\mu^+ \mu^-)}} +\newcommand{\BToKmumu }{\ensuremath{\PB^+ \to \PK^+ \mu^+ \mu^-}} +\newcommand{\BToKee }{\ensuremath{\PB^+ \to \PK^+ e^+ e^-}} +\newcommand{\BToJpsiK }{\ensuremath{\PB^+ \to \PK^+ \PJpsi (\mu^+ \mu^-)}} +\newcommand{\BToJpsieeK }{\ensuremath{\PB^+ \to \PK^+ \PJpsi (e^+ e^-)}} +\newcommand{\mev}{\ensuremath{\mathrm{\,Me\kern -0.1em V}}\xspace} +\newcommand{\mevc}{\ensuremath{{\mathrm{\,Me\kern -0.1em V\!/}c}}\xspace} +\newcommand{\mevcc}{\ensuremath{{\mathrm{\,Me\kern -0.1em V\!/}c^2}}\xspace} +\newcommand{\chisq}{\ensuremath{\chi^2}\xspace} +\newcommand{\chisqndf}{\ensuremath{\chi^2/\mathrm{ndf}}\xspace} +\newcommand{\chisqip}{\ensuremath{\chi^2_{\text{IP}}}\xspace} +\newcommand{\chisqvs}{\ensuremath{\chi^2_{\text{VS}}}\xspace} +\newcommand{\chisqvtx}{\ensuremath{\chi^2_{\text{vtx}}}\xspace} +\newcommand{\chisqvtxndf}{\ensuremath{\chi^2_{\text{vtx}}/\mathrm{ndf}}\xspace} + + + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + +\author{ {Marcin Chrzaszcz} (CERN)} +\institute{UZH} +\title[\BToKemu approval]{\BToKemu approval} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.65\textwidth} + \flushright \bfseries \Huge {Search for the lepton-flavour violating decays \BToKem} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.33\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + % \includegraphics[width=0.45\textwidth]{lhcb-logo}~~ + \includegraphics[width=0.45\textwidth]{cern} + + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.99\textwidth} +J.~Albrecht$^1$, J.~Bhom$^2$, M.~Chrzaszcz$^{4}$, G.Meier$^{1}$, +%V.~Gligorov$^{5}$, +T~.Momb\"acher$^{1}$, M.~Pikies$^{2}$, F.~Polci$^{5}$, S.~Reichert$^{1}$, N.~Serra$^{3}$ +\bigskip\\ +$^1$ Dortmund , $^2$ Krakow, $^3$ Z\"{u}rich, $^4$CERN, $^5$LPNHE +\end{column} +%\begin{column}{0.53\textwidth} +%\includegraphics[height=1.3cm]{uzh-transp} +%\end{column} +\end{columns} + +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{1.5em} + + \textcolor{normal text.fg!50!Comment}{Tue meeting, April 30, 2019} +\end{center} +\end{frame} +} + + + + + +\begin{frame}\frametitle{Yellow Pages} + +\ARROW Twiki:\\ +{\small \url{https://twiki.cern.ch/twiki/bin/viewauth/LHCbPhysics/B2hemu} } +\ARROW Time scale:\\ +\begin{itemize} +\item WG approval $21^{st}$ Nov. 2018 +\item Unblinding $25^{th}$ Apr. 2019 +\end{itemize} +\ARROW Journal target: PRL\\ +\ARROW Contact authors: \\J.Bhom (Krakow), T. Momb\"acher (Dortmund), F. Polci (LPNHE) + + + +\end{frame} + + + + +\begin{frame}\frametitle{Motivation} + +\ARROW Good ,,old'' anomalies: $P_5^{\prime}$, $R_{\PK}$, $R_{\PKstar}$ can implicate the existence of $\Pbeauty \to \Pstrange \mu e$.\\ +\ARROW LQ, neutrino CP violation, $\PZ^{\prime}$: $\mathcal{B}(\PB \to \PK e \mu) =10^{-8}-10^{-10}$.\\ +\ARROW Particularly interesting in LQ: $\mathcal{B}(\PB \to \PK e \mu) = \frac{1-R_{\PK}}{0.23} \times 10^{-8}$ should be accessible within analysis sensitivity.\\ +\ARROW Current best UL are from Babar (90\% CL) [PR D73 (2006) 092001]: +\begin{itemize} +\item $\mathcal{B}(\PB^+ \to \PK^+ e^+ \mu^-) < 9.1 \times 10^{-8} $ +\item $\mathcal{B}(\PB^+ \to \PK^+ e^- \mu^+) < 13 \times 10^{-8} $ +\end{itemize} +\pause +\ARROW Recently Belle also put its 5 cents [PRD 98 (2018) 071101]: +\begin{itemize} +\item $\mathcal{B}(\PB \to \PKstar e^+ \mu^-) < 1.6 \times 10^{-7} $ +\item $\mathcal{B}(\PB \to \PKstar e^- \mu^+) < 1.2 \times 10^{-7} $ +\end{itemize} + +\begin{footnotesize} +\ARROWR NP predictions: 1503.01084, 1504.07928, 1503.07099, 1507.01412 +\end{footnotesize} +\end{frame} + +\begin{frame}\frametitle{Analysis Strategy} + +\ARROW Blind analysis: signal window looked at after finalizing analysis procedure.\\ +\ARROW Analysis strategy: +\begin{itemize} +\item Stripping +\item Loose preselection +\item Target vetos +\item Hard MVA and PID selection +\item Upper limit setting +\item Book airplane ticket to Stockholm (optional ;) ) +\end{itemize} +\ARROW Dataset: $3~\rm fb^{-1}$, Run1. + + +\end{frame} + + + +\begin{frame}\frametitle{Normalization} +\ARROW Typically the $\Pbeauty \APbeauty$ cross section has large uncertainty.\\ +\ARROW It is more beneficial to normalize the decay rate to well know branching fraction \ARROWR reduce systematics: +\begin{align*} +\mathcal{B}(\BToKem) = N_{\tiny \BToKem} \times \frac{ { \mathcal{B}(\BToJpsiK) }}{\varepsilon_{ \BToKem}}\\ \frac{\varepsilon_{\tiny \BToJpsiK}}{N_{\tiny \BToJpsiK}} \nonumber = N_{\tiny \BToKem} \times \alpha +\end{align*} +\ARROW Some systematic cancel in the efficiency ratio. + +\end{frame} + + + +\begin{frame}\frametitle{Stripping} +\begin{center} +\begin{tiny} +\begin{tabular}{lcc} + \hline \hline + Particle or event & Variable & Cut \\ + \hline + Event & $n_{\rm SPD} $ & $<600$ \\ + \hline + + \multirow{5}{*}{$B$} & $|m-m_{\rm PDG}|$ & $< 1500 \mev$\\ + & $\chisq_{\rm vtx}/\rm{dof}$ & $<9$\\ + & $\chisq_{\rm FD}$ wrt. PV & $>100$\\ + & $\chisqip$ wrt. PV & $<25$\\ + & DIRA wrt. PV & $> 0.9995$\\ + \hline + \multirow{3}{*}{$K$} & $p_T$ & $> 400 \mev$\\ + %& $m$ & $< 2600 \mev$\\ + & $\chisqip$ & $>9$\\ + \hline + \multirow{3}{*}{$e$} & $p_T$ & $> 300 \mev$ \\ + & $\chisqip$ wrt. PV & $>9$ \\ + & $PIDe$ & $>0$ \\ + \hline + \multirow{4}{*}{$\mu$} & $p_T$ & $> 300 \mev$\\ + & $\chisqip$ wrt.PV & $>9$\\ + & ISMUON & True\\ + & HASMUON & True\\ + \hline + \multirow{2}{*}{$e\mu$ pair} & $m(e\mu)$ & $>100\mev$ \\ + & $\chisq_{\rm vtx}(e\mu)/{\rm{dof}}$ & $< 9$\\ + \hline + \multirow{5}{*}{Dimuon} & $p_T$ & $> 0 \mev$\\ + & $m$ & $< 5500 \mev$\\ + & $\chisq_{\rm vtx}/\rm{dof}$ & $<9$\\ + & $\chisq_{\rm FD}$ wrt. PV & $>16$\\ + & $\chisqip$ wrt. PV & $>0$\\ + \hline + \multirow{5}{*}{Dielectron} & $p_T$ & $> 0 \mev$ \\ + & $m$ & $< 5500 \mev$ \\ + & $\chisq_{\rm vtx}/\rm{dof}$ & $<9$ \\ + & $\chisq_{\rm FD}$ wrt. PV & $>16$ \\ + & $\chisqip$ wrt. PV & $>0$ \\ + \hline \hline + \end{tabular} + \end{tiny} + +\end{center} +\end{frame} + + +\begin{frame}\frametitle{Preselection: veto peaking backgrounds} + +\begin{columns} +\column{0.7\textwidth} + +\begin{small} + +\ARROW Double semileptonic decays:\\ +$\PB \to e \nu \PD X$, $\PD \to \mu \nu \PK X$ or $\PB \to \mu \nu \PD X$, $\PD \to e \nu \PK X$\\ +Efficiently removed by: $m_{\PK \ell} > 1885\mevcc$\\ + +\ARROW Charmonium decays:\\ +$\PB \to \PJpsi /\Ppsi(2S) \PK^+$, with missID daughters. +\begin{tabular}{lc} + \hline \hline + mass swap & mass region vetoed (\mev)\\ + \hline \hline + \multirow{2}{*}{$K$ with $\mu$ mass} & $3000{ +\includegraphics[width=0.8\textwidth]{{figs/mva1}.png} \\ +\includegraphics[width=0.8\textwidth]{{figs/mva3}.png} +} +\only<2>{ +\includegraphics[angle=-90,width=0.99\textwidth]{{images/BDTG.pdf}}\\ +\includegraphics[angle=-90,width=0.99\textwidth]{{images/ROC_BDTG.pdf}} +} +\end{columns} + + +\end{frame} + + + +\begin{frame}\frametitle{BDTHOP strategy} +\begin{columns} +\column{0.05\textwidth} +~~ +\column{0.4\textwidth} +\ARROW Apply a cut: $BDT>0.98$ prior to training\\ +\ARROW Use same inputs and strategy as for BDT with additional input of HOP\\ +\ARROW Reminder: background proxy is lower mass sideband. +\column{0.6\textwidth} +\includegraphics[width=0.8\textwidth]{{figs/HOP}.png} + +\end{columns} + + +\end{frame} + +\begin{frame}\frametitle{BDTHOP results} + +\ARROW Clearly discriminating power remains. \\ + +\begin{columns} + +\column{0.5\textwidth} +\includegraphics[width=0.95\textwidth]{{images/ROC_BDTG_HOP.png}} +\column{0.5\textwidth} + + \includegraphics[angle=-90,width=0.95\textwidth]{{images/BDTGHOP_overtrain}.pdf} + + +\end{columns} + + +\end{frame} + + + + + +\begin{frame}\frametitle{Optimization} +\ARROWR Standard question in RD: How to optimize the selection?\\ +\ARROW We used $\rm CL_s$ method for optimization [Read:451614].\\ +\ARROWR What dataset do you use?\\ +\ARROW We split the datasets for \BToKemm and \BToKemp and optimize separately.\\ +\only<1>{ + \includegraphics[width=0.99\textwidth]{{figs/opt1}.png} +} +\only<2>{ + \includegraphics[width=0.99\textwidth]{{figs/opt2}.png} +} +\end{frame} + +\begin{frame}\frametitle{Optimization - PID} +\begin{small} +\ARROW After the BDT and BDTHOP cuts there isn't much events left to perform PID optimization.\\ +\ARROW Decided to put a conservative cuts. +\end{small} + +\begin{columns} + +\column{0.5\textwidth} + + +\includegraphics[width=0.9\textwidth]{images/PID/PIDmu.png} \\ +\includegraphics[width=0.9\textwidth]{images/PID/PIDe.png}\\~\\ + +\column{0.5\textwidth} + +\includegraphics[width=0.9\textwidth]{images/PID/PIDK.png} \\ + \ARROW Conservative cuts: + \begin{eqnarray} +\label{eqn:PIDcuts} +{\rm ProbNNmu} & >& 0.7 \, ,\\ +{\rm ProbNNe} &>& 0.65 \, ,\\ +{\rm ProbNNk} &>&0.65. +\end{eqnarray} + +\end{columns} + + + +\end{frame} + +\begin{frame}\frametitle{Optimization summary} + +\ARROW After the full selection this is how our blinded data set looks like: +\begin{columns} + +\column{0.5\textwidth} + +\includegraphics[angle=-90,width=\linewidth]{images/UL/{fit_mumu_Ke_BDT}.pdf} + +\column{0.5\textwidth} + \includegraphics[angle=-90,width=\linewidth]{images/UL/{fit_mumu_Kmu_BDT}.pdf} + + +\end{columns} + + \begin{center} + \begin{tabular}{lc} +\hline +Mode & Expected background\\ \hline + \BToKemp & $3.94 \pm 1.15 $\\ + \BToKemm& $0.88 \pm 0.64$ \\ \hline + +\end{tabular} + + + \end{center} + + + +\end{frame} + + + + + +\begin{frame}\frametitle{Signal Mass Model} +\ARROW We need to know the signal model.\\ +\ARROW We used a data-driven procedure to correct the parameters $P$: +\begin{align} +P_{\mu e}^{\rm pred} = P_{ee}^{\rm data} + (P_{\mu e}^{\rm MC} - P_{ee}^{\rm MC}) \cdot \frac{ P_{ee}^{\rm data} - P_{\mu\mu}^{\rm data} }{ P_{ee}^{\rm MC} -\ + P_{\mu\mu}^{\rm MC} }. +\end{align} +\includegraphics[angle=-90,width=0.49\linewidth]{images/predict_brem0}\includegraphics[angle=-90,width=0.49\linewidth]{images/predict_brem1} + +\ARROW Cross-checked with the $\PB \to e \mu$ analysis method +\end{frame} + + + + + + +\begin{frame}\frametitle{Normalization} + +\begin{columns} + +\column{0.5\textwidth} +\ARROW The normalization factor: +\begin{align*} +\alpha=\frac{ { \mathcal{B}(\BToJpsiK) }}{\varepsilon_{ \BToKem}}\\ \frac{\varepsilon_{\tiny \BToJpsiK}}{N_{\tiny \BToJpsiK}} +\end{align*} +\ARROW Control channel yields: +\begin{footnotesize} +\begin{itemize} +\item 2011: $N_{\tiny \BToJpsiK}= 26940 \pm 170$ +\item 2012: $N_{\tiny \BToJpsiK}= 59220 \pm 250$ +\end{itemize} + +\end{footnotesize} + + + +\column{0.5\textwidth} +\includegraphics[width=0.99\linewidth]{images/B_M_data_mm_both_years_brem1_logy.png}\\ +\begin{tiny} +\begin{align*} +\mathcal{B}(\BToJpsiK) = (6.021 \pm 0.174) \times 10^{-5}~\rm PDG +\end{align*} +\end{tiny} + + + +\end{columns} + +\ARROW Combined alpha: + \begin{tabular}{lccc}\hline + Decay & $\alpha / 10^{-9}$\\ + \hline \hline + \BToKemm & $1.97 \pm 0.18$ \\ + \BToKemp & $2.21 \pm 0.19$ \\ +% \BToKem & $6.90 \pm 0.26$ & $3.08 \pm 0.11$ & $2.13 \pm 0.13$ \\ + \end{tabular} + + +\end{frame} + + + + + + + +\begin{frame}\frametitle{Peaking backgrounds} + +\begin{center} + + + \begin{tabular}{l|c|c}\hline + {Monte Carlo samples} & full mass region & signal region \\ + \hline\hline +%$\Bp \to \Kp \mu e$ & 5.45 $\pm$ 1.0 & 0.908 $\pm$0.004 & 0.91 & 1 & 4.96 $\pm$ 0.91 \\ +$\PB^+ \to \PK^+ \mu^+ \mu^-$ & 0.12 $\pm$ 0.05 & 0.10$\pm$ 0.04\\ +$\PB^+ \to \PK^+ \ep \en$ & 0.0080 $\pm$ 0.0071 & 0.0068 $\pm$ 0.0060\\ +$\PB^+ \to \PK^+ \PJpsi (\to \mu \mu)$ & $ < $ 0.53 & $<$ 0.053\\ +$\PB^+ \to \PK^+ \PJpsi (\to \ep \en)$ & $<$ 1.05 & $<$ 0.21\\ +$\PB^0 \to K^{*0} \ep \en$ & $<$ 0.0014 & $<$ 0.00014\\ +$\Lb \to p \PK^- \mu \mu$ & 0.0072$\pm$ 0.0030 & 0.0029 $\pm$ 0.0014\\ +$\Lb \to p \PK^- \ep \en$ & $<$ 0.0012 & $<$ 0.00048\\ +$\Lb \to p \PK^- \PJpsi ( \to \mu \mu)$ & $<$ 0.26 & $<$ 0.013\\ +$\Lb \to p \PK^- \PJpsi (\to \ep \en)$ & $<$ 1.08 & $<$ 0.054\\ +$\PB^- \to \PD(\to \PK^- \mu \nu) \nu \mu$ & $<$ 2.5 & $<$ 0.050\\ +$\PB^+ \to \PD (\to \PK^+ \en \nu) \ep \mu$ & $<$ 0.50 & $<$ 0.010\\ +$\PB^+ \to \PD (\to \PK^+ \pi^-) \ep \nu$ & $<$ 2.8 & $<$ 0.056\\ +$\PB^+ \to \PK^+ \pi^+ \pi^-$ & 1.8 $\pm$ 3.2 & 0.049 $\pm$ 0.82 \\ + + + \hline \hline + \end{tabular} +\end{center} +\ARROW All backgrounds are suppressed to a negligible level. +\end{frame} + + + + + + + + +\begin{frame}\frametitle{Systematics} +\begin{center} + \begin{tabular}{ccc} + \hline + {Effect} & \BToKemp & \BToKemm \\ + \hline \hline + Data-MC corrections & {$1.0$} & {$1.0$} \\ + Electron-muon differences & {$1.4$} & {$1.4$} \\ + MC model weights & {$0.2$} & {$0.2$} \\ + Fitting model & {$2.1$} & {$2.1$} \\ + PID resampling - binning & {$3.3$} & {$4.6$} \\ + PID resampling - sWeighting & {$3$} & {$3$} \\ + Background (not in $\%$) & {$0.68$} & {$1.67$} \\ + Trigger & {$1.0$} & {$1.0$} \\ + { \color{JungleGreen} Normalisation} & { \color{JungleGreen} $6.8$} & { \color{JungleGreen} $6.6$} \\ + \hline + Total & {$8.6$} & {$9.1$} \\ + \hline \hline + \end{tabular} + +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{Systematics, PID - binning} +\ARROW To perform resampling we bin the PID efficiency in nTracks, $p$ and $\eta$.\\ +\ARROW To access the systematics the finner and coarser binnings are applied. + +\begin{center} +\includegraphics[width=0.37\textwidth]{images/eta1.png} +\includegraphics[width=0.37\textwidth]{images/eta2.png} +\end{center} + + + + + +\end{frame} + + + +\begin{frame}\frametitle{Systematics, Background model} + +\only<1>{ +\ARROW In the nominal fit we assume exponential shape of the background.\\ +\ARROW The alternative model is determined with a loose selection: +\includegraphics[angle=-90,width=0.45\textwidth]{images/bg_sys/{fit_mumu_Kmu_BDT0.8_HOP-0.3}.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{images/bg_sys/{fit_mumu_Ke_BDT0.8_HOP-0.3}.pdf} +} +\only<2>{ +\ARROW Now compared to previous fit: +\includegraphics[angle=-90,width=0.45\textwidth]{images/bg_sys/{fixed_fit_mumu_Ke_BDT}.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{images/bg_sys/{fixed_fit_mumu_Kmu_BDT}.pdf} + + \begin{tabular}{| c | c | c | c |}\hline +Channel & Background systematic & Nominal fit & Alternative fit \\\hline +\BToKemp & $0.60$ & $3.93 \pm 1.14$ & $3.33 \pm 0.69$\\ +\hline +\BToKemm & $0.43$ & $0.88 \pm 0.63$ & $1.30 \pm 0.43$\\ + \hline + \end{tabular}%} +} + + + +\end{frame} + + + +\begin{frame}\frametitle{Systematics, Efficiency maps} + +\ARROW The upper limits are set assuming PHSP model.\\ +\ARROW We will also provide the efficiency maps so theorists can interpret the results in their favorite model: +\includegraphics[angle=-90,width=0.45\linewidth]{figs/dalitz_KeSS_Run1_total.pdf} +\includegraphics[angle=-90,width=0.45\linewidth]{figs/dalitz_KmuSS_Run1_total.pdf} + + + + +\end{frame} + + + +\begin{frame}\frametitle{Upper limits} + +\ARROW Upper limits set with $\rm CL_s$ method in GammaCombo.\\ +\ARROW This version of $\rm CL_s$ takes into account the signal and background shape information.\\ +\ARROW This gains the better expected upper limits by $25\%$. wrt. counting method\\ + + +\includegraphics[angle=-90,width=0.49\linewidth]{{images/B2Kemu_branchingRatio_plugin_cls_cls_KmuSS_noobserved}.pdf} +\includegraphics[angle=-90,width=0.49\linewidth]{{images/B2Kemu_branchingRatio_plugin_cls_cls_KeSS_noobserved}.pdf} + + + +\end{frame} + +\begin{frame}\frametitle{Unblinded results} + +\ARROW On the $25^{th}$ April we have unblinded our dataset.\\~\\ + \begin{tabular}{| c | c | c |}\hline +Channel & Expected background events & Observed \\\hline +\BToKemp & $3.93 \pm 1.14$ & $2$ \\ \hline +\BToKemm & $0.88 \pm 0.63$ & $1$\\ \hline + \end{tabular}\\%} \\ + \only<1>{ + \includegraphics[angle=-90,width=0.45\linewidth]{{images/data_massfits_Ke_SS}.pdf} +\includegraphics[angle=-90,width=0.45\linewidth]{{images/data_massfits_Kmu_SS}.pdf} + } +\only<2>{ +\includegraphics[angle=-90,width=0.49\linewidth]{{images/B2Kemu_branchingRatio_plugin_cls_cls_KmuSS}.pdf} +\includegraphics[angle=-90,width=0.49\linewidth]{{images/B2Kemu_branchingRatio_plugin_cls_cls_KeSS}.pdf} + } + \only<3>{ +\ARROW At 90\% (95\%) confidence level, the observed upper limits for the branching fractions are found to be +\begin{eqnarray*} + \mathcal{B} (B^+ \to K^+ e^+ \mu^-) <6.3 (8.2) \times 10^{-9}, + \end{eqnarray*} +\begin{eqnarray*} + \mathcal{B} (B^+ \to K^+ e^- \mu^+) < 5.7 (7.6) \times 10^{-9}. +\end{eqnarray*} +\begin{eqnarray*} + \mathcal{B} (B^+ \to K^+ e^\pm \mu^\mp) < 5.7 (7.8) \times 10^{-9}. +\end{eqnarray*} + + } +\end{frame} + + + +\begin{frame}\frametitle{Summary} + +\ARROW Search for \BToKemu decays has been performed\\ +\ARROW Over a order of magnitude improvement wrt. to BaBar results\\ +\ARROW We target PRL.\\ +\ARROW No significant excess of events has been observed\\ +\ARROW Proponents ask the collaboration to approve this analysis.\\ + +\pause +\begin{exampleblock}{} +Many thanks to the RC for their hard work and comments!\\ +Many thanks to Stephane for fast reading the draft. +\end{exampleblock} + + + +\end{frame} + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\begin{frame}\frametitle{Combined banana} +\centering +\includegraphics[angle=-90,width=0.65\linewidth]{{images/B2Kemu_branchingRatio_plugin_cls_cls_combined}.pdf} +\end{frame} + + + +\begin{frame}\frametitle{So large errors} +\ARROW $BR=4.2 \times 10^{-9}$ and $BR=4.5 \times 10^{-9}$. + +\centering +\includegraphics[angle=-90,width=0.45\linewidth]{{images/p_values 4}.pdf} +\includegraphics[angle=-90,width=0.45\linewidth]{{images/p_values 5}.pdf} + +\end{frame} + + + + + +\backupend + +\end{document} diff --git a/B2Kemu/Col_aproval/mchrzasz.toc b/B2Kemu/Col_aproval/mchrzasz.toc new file mode 100644 index 0000000..67e0355 --- /dev/null +++ b/B2Kemu/Col_aproval/mchrzasz.toc @@ -0,0 +1,3 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/B2Kemu/Col_aproval/tikzfeynman.sty b/B2Kemu/Col_aproval/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/B2Kemu/Col_aproval/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/B2Kemu/Weights/Makefile b/B2Kemu/Weights/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/B2Kemu/Weights/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/B2Kemu/Weights/beamercolorthemeFlip.sty b/B2Kemu/Weights/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/B2Kemu/Weights/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/B2Kemu/Weights/beamerinnerthemeFlip.sty b/B2Kemu/Weights/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/B2Kemu/Weights/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/B2Kemu/Weights/beamerouterthemeFlip.sty b/B2Kemu/Weights/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/B2Kemu/Weights/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/B2Kemu/Weights/beamerouterthemedecolines.sty b/B2Kemu/Weights/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/B2Kemu/Weights/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/B2Kemu/Weights/beamerthemeFlip.sty b/B2Kemu/Weights/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/B2Kemu/Weights/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/B2Kemu/Weights/images/.DS_Store b/B2Kemu/Weights/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/B2Kemu/Weights/images/.DS_Store Binary files differ diff --git a/B2Kemu/Weights/images/ALLCUT.pdf b/B2Kemu/Weights/images/ALLCUT.pdf new file mode 100644 index 0000000..0bc78d0 --- /dev/null +++ b/B2Kemu/Weights/images/ALLCUT.pdf Binary 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Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{$\PB \to \PK e \mu$ RC meeting, April 24, 2019} +\end{center} +\end{frame} +} + + + + + +\begin{frame}\frametitle{Reminder} + +\ARROW In the last meeting 3 things were requested: +\begin{enumerate} +\item Increase the systematic due to VTX $\chi^2$ reweighing.\\ {\color{ForestGreen} Done, nothing changed due to rounding precision.} +\pause +\item Tackle the large weight problems. +\item Provide a better efficiency maps. +\end{enumerate} + +\end{frame} + + + + +\begin{frame}\frametitle{The problem of efficiency maps} +\ARROW After we divide the 2 histograms we have large weights on the edges: + +\includegraphics[angle=-90,width=0.75\textwidth]{{images/B2Kemu_weights}.pdf} + +\end{frame} + + + +\begin{frame}\frametitle{The (NOT)solution} + +\ARROW Apply cuts: $m_{Ke}>0.6~\GeV$ and $m_{e\mu}>0.2~\GeV$ + +\includegraphics[angle=-90,width=0.75\textwidth]{{images/B2Kemu_weights_my1}.pdf} + +\ARROW Not really solving the problem... + + +\end{frame} + +\begin{frame}\frametitle{The (NOT)solution 2} + +\ARROW Apply cuts: $m_{Ke}>1.0~\GeV$ and $m_{e\mu}>1.0~\GeV$ + +\includegraphics[angle=-90,width=0.75\textwidth]{{images/B2Kemu_weights_my2}.pdf} + +\ARROW Not really solving the problem... + + +\end{frame} + +\begin{frame}\frametitle{The (NOT)solution 3} + +\ARROW Apply cuts: $m_{Ke}>1.0~\GeV$ and $m_{e\mu}>1.0~\GeV$ and $m_{K\mu}>0.7~\GeV$ + +\includegraphics[angle=-90,width=0.75\textwidth]{{images/B2Kemu_weights_my3}.pdf} + +\ARROW Not really solving the problem... + + +\end{frame} + + +\begin{frame}\frametitle{The (NOT)solution 3} + +\ARROW Apply cuts: $m_{Ke}>1.0~\GeV$ and $m_{e\mu}>1.0~\GeV$ and $m_{K\mu}>1.5~\GeV$ + +\includegraphics[angle=-90,width=0.75\textwidth]{{images/B2Kemu_weights_my4}.pdf} + +\ARROW Not really solving the problem... + + +\end{frame} + + +\begin{frame}\frametitle{The (NOT)solution} + +\ARROW No matter what you do you will not avoid this problem, due to geometry. + +\end{frame} + + +\begin{frame}\frametitle{The solution} + + +\ARROW We determine the change induced by the weight cut on the BALL sample (0.5\%, by counting the candidates on the unweighted simulation)\\ +\ARROW We determine the change induced by the weight cut on the PHSP sample (0.2\%, by determining the sum of weights with and w/o including the large weights)\\ +\ARROW The larger number is conservatively assigned as systematic uncertainty\\ + + +\end{frame} + +\begin{frame}\frametitle{Lucky mistake} + +\ARROW During this we noticed that the large weights have not been removed in the efficiency calculation but only in the plots.\\ +\ARROW We therefore propose to leave them in, as we checked their effect is 0.2-0.5\%. + +\end{frame} + +\begin{frame} + +\begin{center} +\begin{Huge} +Efficiency maps +\end{Huge} +\end{center} + + + +\end{frame} + + + +\begin{frame}\frametitle{Efficiency maps} + +\begin{alertblock}{} +\includegraphics[angle=-90,width=0.49\textwidth]{{images/dalitz_KeSS_Run1_total1}.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{{images/dalitz_KmuSS_Run1_total1}.pdf} +\end{alertblock} + + +\end{frame} + + + + + + +\begin{frame} + +\begin{table}[h] + + \begin{center}\begin{tabular}{lc} + \hline \hline + mass swap & mass region vetoed \\ + \hline \hline + \multirow{2}{*}{$K$ with $\mu$ mass} & $3000 diff --git a/CERN_retreat/beamerinnerthemeFlip.sty b/CERN_retreat/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/CERN_retreat/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/CERN_retreat/beamerouterthemeFlip.sty b/CERN_retreat/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/CERN_retreat/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/CERN_retreat/beamerouterthemedecolines.sty b/CERN_retreat/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/CERN_retreat/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/CERN_retreat/beamerthemeFlip.sty b/CERN_retreat/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/CERN_retreat/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/CERN_retreat/images/.DS_Store b/CERN_retreat/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/CERN_retreat/images/.DS_Store Binary files differ diff --git a/CERN_retreat/images/BG_both.png b/CERN_retreat/images/BG_both.png new file mode 100755 index 0000000..49b62d5 --- /dev/null +++ b/CERN_retreat/images/BG_both.png Binary files 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b/CERN_retreat/mchrzasz.synctex.gz Binary files differ diff --git a/CERN_retreat/mchrzasz.tex b/CERN_retreat/mchrzasz.tex new file mode 100644 index 0000000..d2bfcc5 --- /dev/null +++ b/CERN_retreat/mchrzasz.tex @@ -0,0 +1,331 @@ +\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} + +\usepackage[english]{babel} +\usepackage{polski} + + +\usetheme[ + bullet=circle, % Other option: square + bigpagenumber, % circled page number on lower right + topline=true, % colored bar at the top of the frame + shadow=false, % Shading for beamer blocks + watermark=BG_lower, % png file for the watermark + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +%\setmainfont{Times} % Beamer ignores "main font" in favor of sans font +%\setsansfont{Times} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +%\setbeamerfont{title}{family=\fontspec{Times}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} +\def\LcTopmumu{\Lambda_c^{+} \to p \mu^+ \mu^-} +\def\Lc{\Lambda_c^{+}} +\def\mumu{\mu\mu} +\newcommand{\BRof}[1]{\ensuremath{{\cal B}(#1)}\xspace} + +\def\LcTopphi{\Lc \to p \Pphi (\mumu)} +\def\Lcpomegano{\Lc \to p \omega} + + + + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} +\def\pt{p_T} +\def\mevc{MeV/c} +\def\mevcc{MeV/c^2} +\def\gevc{GeV/c} +\def\gevcc{GeV/c^2} +\author{ {Marcin Chrzaszcz} (CERN)} +\institute{UZH} +\title[Current and future activities]{Current and future activities} + +\date{31 January 2018} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright \bfseries \Large {Research activities} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +%\flushright \vspace{-2.8em} { \fontspec{Zapfino} Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +\flushright \vspace{-2.8em} { Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + + +\end{column} +\begin{column}{0.53\textwidth} +\hspace{2.0cm} +\includegraphics[height=1.6cm]{cern} +\end{column} +\end{columns} + + + \textcolor{normal text.fg!50!Comment}{Tuesday meeting, CERN\\January 31, 2018} +\end{center} +\end{frame} +} + + +\begin{frame}{Past activities} +\vspace{0.5em} + \begin{minipage}{\textwidth} + +\begin{columns} + +\column{0.27\textwidth} +\ARROW $\tau \to 3\mu$.\\ +\ARROW $\tau \to p \mu \mu$.\\ +\ARROW $\PBd \to \PKstar \mu \mu$.\\ +\ARROW $\PBd \to \PK \Ppi \mu \mu$.\\ +\ARROW $\PBu \to \PK \chi (\mu \mu)$.\\ +\ARROW GAMBIT.\\ +\ARROW HFLAV. + + +\column{0.73\textwidth} +\includegraphics[width=0.45\textwidth]{inflaton.png} +\includegraphics[width=0.45\textwidth]{banana_tau23mu.png}\\ +\includegraphics[width=0.45\textwidth]{hidef_Fig5.png} +\includegraphics[width=0.45\textwidth]{images/P5p.png}\\ +\includegraphics[width=0.45\textwidth]{WC_3_2_like2D.png} +\includegraphics[width=0.45\textwidth]{CMSSM_2_3_like2D.png} + +\end{columns} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + +\begin{frame}{Current activities} +\vspace{0.5em} + \begin{minipage}{\textwidth} + +\begin{columns} + +\column{0.35\textwidth} +\ARROW $\Lambda_c \to p \mu \mu$ \\ +\ARROW $\PBd \to \PKstar \mu \mu$.\\ +\ARROW Pheno work on $\Pbeauty \to \Pstrange \ell \ell$\\ +\ARROW Gambit NP scans.\\ +\ARROW LUV measurements. + + +\column{0.65\textwidth} +\includegraphics[width=0.7\textwidth]{fig-btokstarll-p5prime-paramA.png}\\ +\includegraphics[width=0.7\textwidth]{Jpsi_fit_2015.png} +\end{columns} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + + +\end{document} diff --git a/CERN_retreat/mchrzasz.tex~ b/CERN_retreat/mchrzasz.tex~ new file mode 100644 index 0000000..a3d9daf --- /dev/null +++ b/CERN_retreat/mchrzasz.tex~ @@ -0,0 +1,987 @@ +\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} + +\usepackage[english]{babel} +\usepackage{polski} + + +\usetheme[ + bullet=circle, % Other option: square + bigpagenumber, % circled page number on lower right + topline=true, % colored bar at the top of the frame + shadow=false, % Shading for beamer blocks + watermark=BG_lower, % png file for the watermark + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Times} % Beamer ignores "main font" in favor of sans font +\setsansfont{Times} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Times}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} +\def\LcTopmumu{\Lambda_c^{+} \to p \mu^+ \mu^-} +\def\Lc{\Lambda_c^{+}} +\def\mumu{\mu\mu} +\newcommand{\BRof}[1]{\ensuremath{{\cal B}(#1)}\xspace} + +\def\LcTopphi{\Lc \to p \Pphi (\mumu)} +\def\Lcpomegano{\Lc \to p \omega} + + + + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} +\def\pt{p_T} +\def\mevc{MeV/c} +\def\mevcc{MeV/c^2} +\def\gevc{GeV/c} +\def\gevcc{GeV/c^2} +\author{ {Marcin Chrzaszcz} (CERN)} +\institute{UZH} +\title[Search for the $\Lambda_c^{+} \to p \mu^+ \mu^-$ decay ]{Search for the $\Lambda_c^{+} \to p \mu^+ \mu^-$ decay } + +\date{25 September 2014} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright \bfseries \Large {Search for the suppressed $\Lambda_c^{+} \to p \mu^+ \mu^-$ decay and observation of the $\Lambda_c^{+} \to p \omega$ decay} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-2.8em} { \fontspec{Zapfino} Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +\end{column} +\begin{column}{0.53\textwidth} +\hspace{2.0cm} +\includegraphics[height=1.6cm]{cern} +\end{column} +\end{columns} + +\vspace{1em} + \footnotesize{\large With M. Jezabek, T. Lesiak, B. Nowak, M. Witek (IFJ PAN)} +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{Tuesday meeting, CERN\\September 26, 2017} +\end{center} +\end{frame} +} + + +\begin{frame}{Yellow pages} +\vspace{0.5em} + \begin{minipage}{\textwidth} + \ARROW Reviewers: Tom Blake(chair), Harry Cliff, Simon Eydelman(EB)\\ + \ARROW Twiki:\\ + \href{https://twiki.cern.ch/twiki/bin/viewauth/LHCbPhysics/Lc2PMuMu}{\url{https://twiki.cern.ch/twiki/bin/viewauth/LHCbPhysics/Lc2PMuMu}}\\ + \ARROW Review start: 31.03.2017\\ + \ARROW Fruitfull interactions with the review committee. \\ + \ARROW Unblinding: 18.07.2017\\ + \ARROW Minor changes to the analysis during the review.\\ + +\begin{center} +We would like to take this occasion and than Tom, Harry and Simon for fruitful, constructive and smooth review! +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}{Motivation} +\vspace{0.5em} + \begin{minipage}{\textwidth} + + +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\vspace{0.5em} + +\ARROW SM predictions:\\ +~~~~~~$\mathcal{O}(10^{-8})$\\ +\ARROW Long distance effects:\\ +~~~~~~$\mathcal{O}(10^{-6})$\\ +~~~~\\ +\ARROW Previous measurement done by Babar:\\ +~~${\rm Br}(\Lambda_c^{+} \to p \mu^+ \mu^-) < 4.4\cdot 10^{-5}$ at 90\% CL\\ +\begin{center} +\includegraphics[width=0.65\textwidth]{images/babar.png}\\ + +\end{center} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/indeks1.jpg}\\ +\includegraphics[width=0.95\textwidth]{images/indeks2.jpg}\\ +\begin{exampleblock}{} +Should be able to improve by \\a factor of 100! +\end{exampleblock} + + +\end{columns} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + +\begin{frame}{Analysis strategy} +\vspace{0.5em} + \begin{minipage}{\textwidth} + +\ARROW Normalization to $\Lambda_c^+ \to p \phi(\mu\mu)$.\\ +\ARROW Typical steps rare decays: +\begin{itemize} +\item Loose stripping selection. +\item BDT1 used for first preselection. +\item BDT2 used to further suppress the background. +\item PID used to fight the peaking background. +\end{itemize} +\ARROW Search performed in several dimuon mass windows.\\ +\ARROW Selection optimized on $\rm CL_s$.\\ +\ARROW Unblinding and calculate the UL of BR using $\rm CL_s$. +\pause +\begin{center} +\includegraphics[width=0.5\textwidth]{images/blind.jpg} +\end{center} + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +\begin{frame}{Normalization channel} +\vspace{0.5em} + \begin{minipage}{\textwidth} +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +{\Large Use the $\Lambda_c^{+} \to p \phi(\mu\mu)$.}\\ +\ARROW Same final state, same selection, a lot of systematics cancel.\\ +\ARROWR The Branching fraction of $\Lambda_c^{+} \to p \phi$ is known with $22~\%$. + +{\Large Use the $\Lambda_c^{+} \to p K \pi$.}\\ +\ARROW More precisely known branching fraction (precision: $6.4~\%$).\\ +\ARROWR A lot of additional systematics due to different final states, different selections + +\column{2in} +\only<1>{ +\includegraphics[width=0.9\textwidth]{images/quovadis.jpg} +} +\only<2>{ +\includegraphics[width=0.9\textwidth]{images/quovadis2.jpg} +} +\end{columns} +\begin{exampleblock}{We choose the $\Lambda_c^{+} \to p \phi(\mu\mu)$ option} +\ARROWR In the most optimistic scenario where you assume the $22~\%$ systematic to go town to $6.4~\%$ the UL. \\ +In this case the UL gets worse $7.8~\%$. +\end{exampleblock} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\begin{frame}{Data sets and Stripping} +\vspace{0.5em} + \begin{minipage}{\textwidth} +\ARROW 2011+2012 (aka Run1) Stripping 20.\\ +\begin{center} + +\begin{tabular}{|c|c|} +\hline +Condition & ~~$\LcTopmumu$~~\\ +\hline +$\mu^{\pm}$ and $p$ & \\ +$\pt$ & {$>300\mevc$} \\ +Track $\chi^2$/ndf & {$<3 $} \\ +IP $\chi^2$/ndf & {$>9 $} \\ +PID $\mu^\pm$ & PIDmu$ >$ -5 and (PIDmu - PIDK) $>$ 0 \\ +PID p & PIDp$>$10 \\ +\hline +$\Lc$ & {~} \\ +$\Delta m$ & $<150\mevcc$ \\ +Vertex $\chi^2$ & {$<15$} \\ +IP $\chi^2$ & {$<225 $} \\ +$c\tau$ & {$>100\rm \mu m$} \\ +Lifetime fit $\chi^2$ & {$<225 $} \\ +%\hline +%$m_{\mu^+\mu^-}$ & $> 450\mevcc$ \\ +%$m_{\mu^+\mu^+}$ & $> 250\mevcc$ \\ +\hline +\end{tabular} +\end{center} + \end{minipage} + \vspace*{2.cm} +\end{frame} + + +\begin{frame}{Preselection} +\vspace{0.5em} + \begin{minipage}{\textwidth} + +\ARROW Additional cuts: + +\begin{center}\begin{tabular}{|c|} + \hline + Common cuts \\ + \hline + $m_{\mumu}$ $< 1400~\mevcc$ \\ + proton $ProbNNp > 0.1 $ \\ % Podzielic te ciecia i opisac gdzie t + $\mu^+,\mu^-$ $ ProbNNmu > 0.1 $ \\ + $ 10~\gevc < p_{proton} < 100~\gevc $ \\ + \hline + \end{tabular}\end{center} + +\ARROW We define couple of dimuom mass regions: +\begin{center} + \begin{tabular}{|c | c|} +\hline +$m(\mu\mu)$ region & $\left[ \mevcc \right]$\\ \hline +$\phi$ region & $\left[985, 1055\right]$\\ +$\omega$ region & $\left[759 , 805\right]$\\ +{\it{non resonant} } & $\left[210, 747 \right] \cup \left[817, 980 \right] \cup \left[1060, 1400\right]$ \\ \hline +\end{tabular} +\end{center} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + +\begin{frame}{Trigger} +\vspace{0.5em} + \begin{minipage}{\textwidth} + \vspace{0.5em} + +\ARROW We require the following triggers (all are TOS): +\begin{itemize} + \item L0 + \begin{itemize} + \item L0MuonDecision + \end{itemize} + \item HLT1 + \begin{itemize} + \item Hlt1TrackMuonDecision + \item Hlt1DiMuonLowMassDecision + \item Hlt1TrackAllL0Decision + \end{itemize} + \item HLT2 + \begin{itemize} + \item Hlt2DiMuonDetachedDecision + \item Hlt2CharmSemilep3bodyD2KMuMuDecision + \item Hlt2CharmSemilepD2HMuMuDecision + \end{itemize} +\end{itemize} + +\ARROW The TIS increase the signal yield by $<10~\%$ and were asked to be removed at the WG review stage. + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + +\begin{frame}{BDT1 training} +\vspace{0.5em} + \begin{minipage}{\textwidth} + \vspace{0.5em} +\begin{columns} + +\column{0.1in} +{~}\\ + +\column{3in} +\ARROW The normalization channel is also a rather ``rare decay'':\\ +${\rm Br}(\Lambda_c^+ \to p \phi) \cdot {\rm Br}(\phi \to \mu \mu) = 3.1 \cdot 10^{-7}$\\ +\ARROW After the previous preselection a simple BDT is trained using variables that are well simulated in the MC. k-folding used ($k=10$) +\ARROW The BDT1 (not surprisingly) likes the prompt $\Lambda_c$ rather the secondary ones. +\begin{center} +\includegraphics[angle=-90,width=0.7\textwidth]{images/BDT_pre_history.pdf} + +\end{center} + +\column{2in} +\includegraphics[angle=-90,width=0.95\textwidth]{images/compare_BDT1_2011.pdf} \\ +\includegraphics[angle=-90,width=0.95\textwidth]{images/compare_BDT1_2012.pdf} \\ + + + +\end{columns} + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}{BDT1 selection} +\vspace{0.5em} + \begin{minipage}{\textwidth} +\ARROW The selection based on BDT1 is not optimised.\\ +\ARROW A loose cut: +\begin{equation} +{\rm BDT1} > -0.1 \nonumber +\end{equation} + + \begin{center} +\includegraphics[angle=-90,width=0.49\linewidth]{images//Lc2pPhi5_pre.pdf} + \includegraphics[angle=-90,width=0.49\linewidth]{images/expected_bck5_pre.pdf} + + + \end{center} + \ARROW The normalization channel peak is observed. + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}{BDT2 selection} +\vspace{0.5em} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.1in} +{~}\\ + +\column{3in} + +\ARROW Variables used: + +\begin{footnotesize} +\begin{itemize} + \item + flight distance - the one between the production and decay points. + \item + $\chi^2$ of flight distance, + \item + transformed decay time - $T=\exp{(-1000 \cdot \tau / {\mathrm{ns}})}$, + \item + IP - impact parameter with respect to primary vertex, + \item + $\chi^2$ of IP of $\Lc$ + \item + $\log(\chi^2_{DTF})$, + \item + $p_T$ - transverse momentum of $\Lc$, + + \item + minimum of $\chi^2$ of $p$, $\mu^+$, $\mu^-$ w.r.t. primary vertex, + \item + transverse momenta + \item + minimum of $\chi^2$/NDF of track fit of $p$, $\mu^+$, $\mu^-$. +\end{itemize} +\end{footnotesize} + + + +\column{2in} +\vspace{3.0em} +\includegraphics[angle=-90,width=0.95\textwidth]{images/compare_BDT2_2011.pdf} \\ + +\includegraphics[angle=-90,width=0.95\textwidth]{images/compare_BDT2_2012.pdf} \\ +\vspace{3.0em} +{~} + + +\end{columns} + \end{minipage} + \vspace*{2.cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +\begin{frame}{BDT2} +\vspace{0.5em} + \begin{minipage}{\textwidth} + +\begin{columns} + +\column{0.02\textwidth} +{~}\\ + +\column{0.48\textwidth} +\begin{small} +\ARROW After correcting the DATA/MC differences the BDT distribution shows a good DATA/MC agreement.\\ +\ARROW No mass correlation observed. +\end{small} +\includegraphics[angle=-90,width=0.95\textwidth]{images/mBDT2_profile.pdf} + + +\column{0.48\textwidth} + +\includegraphics[angle=-90,width=0.95\textwidth]{images/Comparison_BDT_data_mc_shifted.pdf} + +\includegraphics[angle=-90,width=0.95\textwidth]{images/BDT_check_3mu_bkg_1.pdf} + + +\column{0.02\textwidth} +{~}\\ + + + +\end{columns} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\begin{frame}{PID} +\vspace{0.5em} + \begin{minipage}{\textwidth} +\begin{small} + +\ARROW MC resampling is choose to correct the PID distributions:\\ +For MC samples the ProbNNp and ProbNNmu are drawn from the PIDCalib distributions.\\ + +\begin{columns} +\column{0.5\textwidth} + +\ARROWR The PIDCalib doesn't cover the low $\pt$ region for muons ($10\%$).\\ +\ARROWR Decided to use for them the $D_s \to \phi(\mu\mu)$ sample.\\ + +\includegraphics[angle=-90,width=0.95\textwidth]{images/Comparison_ProbNNmu_data_mc.pdf} + + +\column{0.5\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{images/effmu_pid.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{images/Comparison_ProbNNp_data_mc.pdf} + + +\end{columns} + + + +\end{small} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + +\begin{frame}{Selection optimization} +\vspace{1.5em} + \begin{minipage}{\textwidth} +\begin{small} +\begin{columns} + +\column{0.01\textwidth} +{~}\\ + +\column{0.68\textwidth} + +\ARROW The final selection of the analysis is optimized!\\ +\ARROW $\rm CL_s$ method used.\\ +\ARROW Toy experiment used to find the optimum. +{~}\\ +\begin{center}\begin{tabular}{lc} + \hline + Variable & Condition \\ + \hline + BDT & $> 0.0$ \\ + $ProbNNp(p)$ & $> 0.68$ \\ + minimum $ProbNNmu(\mu^{\pm})$ & $> 0.38$ \\ + \hline + \end{tabular}\end{center} + + + +\includegraphics[angle=-90,width=0.5\linewidth]{images/Lc2pPhi5.pdf} +\includegraphics[angle=-90,width=0.5\linewidth]{images/expected_bck5.pdf} + +\column{0.3\textwidth} +\includegraphics[width=0.99\textwidth]{images/scan_ul.pdf} +\column{0.01\textwidth} + + + + +\end{columns} + + +\end{small} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +\begin{frame}{Peaking backgrounds} +\vspace{1.5em} + \begin{minipage}{\textwidth} + + +\begin{columns} + +\column{0.6\textwidth} +\ARROW The tight PID cuts essentially kill the peaking bkg!\\ +\ARROW The only bkg left is the $\Lambda_c^{+} \to p \pi \pi$.\\ + +\begin{center} + \includegraphics[angle=-90,width=0.80\linewidth]{images/mass_bkg_p2pi.pdf} +\end{center} + \ARROW Estimated contamination: \\$1.96 \pm 1.13$ \ARROWR assigned as systematic +\column{0.4\textwidth} + +\begin{center} + \includegraphics[angle=-90,width=0.99\linewidth]{images/ref_Lc2pmumu.pdf} \\ + \includegraphics[angle=-90,width=0.99\linewidth]{images/ref_Lc2ppipi.pdf} \\ + \includegraphics[angle=-90,width=0.99\linewidth]{images/ref_Lc2pkpi.pdf} \\ + \includegraphics[angle=-90,width=0.99\linewidth]{images/ref_Ds2kmumu.pdf} \\ + \includegraphics[angle=-90,width=0.99\linewidth]{images/ref_Dp2kpipi.pdf} + \vspace*{-1.0cm} +\end{center} + + +\end{columns} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}{Normalization} +\vspace{1.5em} + \begin{minipage}{\textwidth} +\ARROW The gold equation: + +\begin{equation*} +{\frac{\BRof\LcTopmumu}{\BRof\LcTopphi} = +\frac{\rm +{\epsilon\mathstrut_{norm}}^{TOT} +}{\rm +{\epsilon\mathstrut_{sig}}^{TOT} +} +\times\frac{N_{\rm sig}}{N_{\rm norm}}, } +\label{eq:normalization} +\end{equation*} +\ARROW We take advantage of the cancellation that: + +\begin{equation*} +{\frac{\rm {\epsilon\mathstrut_{norm}}^{TOT} }{\rm {\epsilon\mathstrut_{sig}}^{TOT}}} += +{\frac{\rm {\epsilon\mathstrut_{norm}}^{STRIP}}{\rm {\epsilon\mathstrut_{sig}}^{STRIP}}} +\times +{\frac{\rm {\epsilon\mathstrut_{norm}}^{COMM}}{\rm {\epsilon\mathstrut_{sig}}^{COMM}}} +\times +{\frac{\rm {\epsilon\mathstrut_{norm}}^{SPEC}}{\rm {\epsilon\mathstrut_{sig}}^{SPEC}}} ,~~ {\frac{\rm {\epsilon\mathstrut_{norm}}^{i}}{\rm {\epsilon\mathstrut_{sig}}^{i}}} \simeq 1 +\label{eq:effprod} +\end{equation*} + +\begin{columns} +\column{0.02\textwidth} + +\column{0.56\textwidth} +\ARROW In addition we have added 6 mass bins to increase the sensitivity.\\ +\ARROW Signal is modelled by a double Crystall Ball. + +\column{0.4\textwidth} +\includegraphics[width=0.85\textwidth]{images/massbin.png} + +\column{0.02\textwidth} + + +\end{columns} + + + + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + +\begin{frame}{Expected background} +\vspace{1.5em} + \begin{minipage}{\textwidth} + + + \begin{small} +\begin{columns} + +\column{0.02\textwidth} + +\column{0.48\textwidth} +\ARROW Background modelled with a linear function.\\ + + \includegraphics[width=0.9\linewidth]{images/expected_bck5_obs_with_signal1.pdf} + +\column{0.48\textwidth} + + + +\begin{center}\begin{tabular}{|c|c|} +\hline +bin & no events \\ +\hline +bin1 & $ 8.56136 \pm 0.540302 $ \\ +bin2 & $ 8.60318 \pm 0.536917 $ \\ +bin3 & $ 8.64582 \pm 0.536561 $ \\ +bin4 & $ 8.6887 \pm 0.539208 $ \\ +bin5 & $ 8.7304 \pm 0.544752 $ \\ +bin6 & $ 8.77226 \pm 0.553162 $ \\ +\hline + \end{tabular}\end{center} + + +\column{0.02\textwidth} + + + +\end{columns} + +\begin{columns} + +\column{0.6\textwidth} + + \includegraphics[angle=-90,width=0.49\linewidth]{images/br90rel.pdf} + \includegraphics[angle=-90,width=0.49\linewidth]{images/br90abs.pdf} + +\column{0.4\textwidth} + + +\ARROW Expected upper limits: +$\BRof\LcTopmumu < 5.91 \times 10^{-8}$ at 90~\% CL + +\end{columns} + + + + + +\end{small} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\begin{frame}{Observed Upper limits} +\vspace{1.5em} + \begin{minipage}{\textwidth} + + +\begin{columns} + +\column{0.6\textwidth} + +\ARROW After the green light from RC we have unblinded; no significant access of events have been observed. +\ARROW We have set an UL: +\begin{equation*} +\BRof\LcTopmumu < 7.68 \times 10^{-8}~ \rm at 90~\%~CL +\end{equation*} + +\column{0.4\textwidth} + \includegraphics[angle=-90,width=0.9\linewidth]{images/expected_bck5_obs_with_signal.pdf} + + +\end{columns} + + \includegraphics[angle=-90,width=0.45\linewidth]{images/br90rel_obs.pdf} + \includegraphics[angle=-90,width=0.45\linewidth]{images/br90abs_obs.pdf} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}{By product :)} +\vspace{1.5em} + \begin{minipage}{\textwidth} + + + \begin{columns} + +\column{0.5\textwidth} + + \ARROW We also looked at the $\omega$ dimuon region.\\ +\begin{exampleblock}{We observed an access} +Using Wilks theorem we have calculated the singificance to be $5.0~\sigma$! +\end{exampleblock} +\ARROW This is the first observation of this decay!!!\\ +$\BRof\Lcpomegano = (7.6 \pm 2.6~(stat) \pm 0.9~(syst1) \pm 3.1~(syst2) )~\times 10^{-4}$ + +\column{0.5\textwidth} +\includegraphics[angle=-90,width=0.99\textwidth]{images/Lc2pomega_DATA_mass_sel.pdf}\\ +\includegraphics[angle=-90,width=0.99\textwidth]{images/mumu_mass_fit_sel.pdf} + + +\end{columns} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + +\begin{frame}{Conclusion} +\vspace{1.5em} + \begin{minipage}{\textwidth} + + \begin{itemize} + \item Improved the UL for $\BRof\LcTopmumu$ by two orders of magnitude!\\ + \pause + \includegraphics[width=0.5\textwidth]{images/mr_bean_laboratory.jpg} + + \item First time observed the decay $\Lcpomegano$!! + \item Paper is beeing prepared, aiming PRL + \item We would like to ask the collaboration for approving this analysis. + \end{itemize} +\begin{center} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/CERN_retreat/mchrzasz.toc b/CERN_retreat/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/CERN_retreat/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/CERN_retreat/missfont.log b/CERN_retreat/missfont.log new file mode 100644 index 0000000..5dde65f --- /dev/null +++ b/CERN_retreat/missfont.log @@ -0,0 +1,23 @@ +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times/BI +mktextfm Times +mktextfm Times/B +mktextfm Times +mktextfm Times/I +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times +mktextfm Times diff --git a/CERN_retreat/tikzfeynman.sty b/CERN_retreat/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/CERN_retreat/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/FPCP_2018/Makefile b/FPCP_2018/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/FPCP_2018/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/FPCP_2018/beamercolorthemeFlip.sty b/FPCP_2018/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/FPCP_2018/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/FPCP_2018/beamerinnerthemeFlip.sty b/FPCP_2018/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/FPCP_2018/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/FPCP_2018/beamerouterthemeFlip.sty b/FPCP_2018/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/FPCP_2018/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/FPCP_2018/beamerouterthemedecolines.sty b/FPCP_2018/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/FPCP_2018/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/FPCP_2018/beamerthemeFlip.sty b/FPCP_2018/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/FPCP_2018/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/FPCP_2018/images/.DS_Store b/FPCP_2018/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/FPCP_2018/images/.DS_Store Binary files differ diff --git a/FPCP_2018/images/1-s2.0-S0370269315000738-gr002.jpg b/FPCP_2018/images/1-s2.0-S0370269315000738-gr002.jpg new file mode 100644 index 0000000..7a84874 --- /dev/null +++ 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+\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} + +\newcommand\textref[1]{% + \begin{textblock*}{\paperwidth}(0pt,0.025\textheight) + \raggedleft \small{{\color{RoyalBlue} \emph{#1}}}\hspace{1.5em} + \end{textblock*}} + +\newcommand\textahref[2]{% + \begin{textblock*}{\paperwidth}(0pt,0.025\textheight) + \raggedleft \small{\emph{\href{#1}{#2} }}\hspace{1.5em} + \end{textblock*}} + + + +\author{ {M.Chrzaszcz} (CERN)} +\institute{UZH} +\title[Rare decays in the beauty, charm and strange sector]{Rare decays in the beauty, charm and strange sector} +\date{28 March 2018} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright\bfseries \Huge {Rare decays in the beauty, charm and strange sector} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} { \Large Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=1.3cm]{cern} +\end{column} +\end{columns} +\vspace{0.2em} + + +\vspace{1em} + +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{FPCP, Hyderabad\\14-18 July 2018 +} +\end{center} +\end{frame} +} + + +\begin{frame}{Outline} + +\begin{enumerate} +\item Beauty decays +\begin{itemize} +\item $\Lambda_b \to \Lambda \mu \mu$ +\item $\APBs \to \PKstar \mu \mu$ +\item $\PB_{(s)} \to e \mu$ +\item $\PB \to \PKstar e \mu$. +\end{itemize} +\item Charm decays +\begin{itemize} +\item $\Lambda_c \to \Pproton \mu \mu$ +\item $\PD \to hh \mu\mu$ +\end{itemize} +\item Strange decays +\begin{itemize} +\item $\PKshort \to \mu \mu$ +\item $\Sigma \to \Pproton \mu \mu$ +\end{itemize} +\end{enumerate} + + + +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{Why rare decays?} +\begin{columns} +\column{4in} +\begin{itemize} +\item The SM allows only charged interactions to change flavour. +\begin{itemize} +\item Other interactions are flavour conserving. +\end{itemize} +\item One can escape this constraint and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. +\begin{itemize} +\item These kinds of processes are suppressed in the SM $\to$~Rare decays. +\item New Physics can enter in the loops. +\end{itemize} +\end{itemize} +\begin{center} +\includegraphics[scale=0.3]{images/lupa.png} +\includegraphics[scale=0.3]{images/example.png} +\end{center} +\column{1.5in} +\includegraphics[width=0.61\textwidth]{images/couplings.png} +\end{columns} + +\end{frame} + + + +\begin{frame} +\only<1>{\frametitle{LHCb detector - tracking} + +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/sketch.png} +\end{columns} +\begin{itemize} +\item Excellent Impact Parameter (IP) resolution ($20~\rm \mu m$).\\ +$\Rightarrow$ Identify secondary vertices from heavy flavour decays +\item Proper time resolution $\sim~40-50~\rm fs$.\\ +$\Rightarrow$ Good separation of primary and secondary vertices. +\item Excellent momentum ($\delta p/p \sim 0.5 - 1.0\%$) and inv. mass resolution.\\ +$\Rightarrow$ Low combinatorial background. + +\end{itemize} + +} + +\only<2>{\frametitle{LHCb detector - PID} + +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/cher.png} +\end{columns} +\begin{itemize} +\item Excellent Muon identification $\epsilon_{\mu \to \mu} \sim 97\%$, $\epsilon_{\pi \to \mu} \sim 1-3\%$ +\item Good $\PK-\Ppi$ separation via RICH detectors, $\epsilon_{\PK \to \PK} \sim 95\%$, $\epsilon_{\Ppi \to \PK} \sim 5\%$.\\ +$\Rightarrow$ Reject peaking backgrounds. +\item High trigger efficiencies, low momentum thresholds.\\ +%Muons: $p_T > 1.76 \GeV/c$ at L0, $p_T > 1.0 \GeV/c$ at HLT1,\\ +$B \to \PJpsi X $: Trigger $\sim 90\%$. + +\end{itemize} + + +} + +\textref{Int. J. Mod. Phys. A30 (2015) 1530022} +\vspace*{2.1cm} +\end{frame} + + + + +\begin{frame}{Rare beauty decays} + +\begin{columns} + +\column{0.5\textwidth} +\begin{exampleblock}{$\Pbeauty \to \Pstrange \ell \ell$ family} +\begin{itemize} +\item $\PB \to \PKstar \mu \mu$ +\item $\PBs \to \Pphi \mu \mu$ +\item $\Lambda_b \to \Pproton \PK \mu \mu$ +\item LUV: $R_K$, $R_{\PKstar}$ +\end{itemize} +\end{exampleblock} +{~}\\ +\ARROW Too many results to be covered in one talk! Please see A.~Oyanguren's talk for more! + +\column{0.5\textwidth} +\begin{alertblock}{$\Pbeauty \to \Pstrange \gamma$ family} +\begin{itemize} +\item $\PB \to \PJpsi \gamma$ +\item $\PB \to \PK \Ppi \Ppi \gamma$ +\end{itemize} +\end{alertblock} + +\begin{block}{$\Pbeauty \to \Pdown \ell \ell$ family} +\begin{itemize} +\item $\PB \to \pi \pi \mu \mu$ +\item $\APBs \to \PKstar \mu \mu$ +\item $\Lambda_b \to \Pproton \pi \mu \mu$ +\end{itemize} + +\end{block} + +\begin{exampleblock}{Purely leptonic family} +\begin{itemize} +\item $\PB \to \ell \ell$ +\item LFV: $\PB \to \ell \ell^{\prime}$ +\item LFV in $\tau$ + +\end{itemize} + +\end{exampleblock} + +\end{columns} + + + +\end{frame} + + + +{ +\usebackgroundtemplate{\includegraphics[width=\paperwidth,height=\paperheight]{images/familie.jpg}} +\begin{frame}[plain] +\end{frame} +} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 + +\begin{frame}{$\Lambda_b \to \Lambda \mu \mu$} +\begin{columns} +\column{0.01\textwidth} +{~} +\column{0.5\textwidth} +\ARROW $\Pbeauty \to \Pstrange \mu \mu$ in baryon sector. \\ +\ARROW Because of spin $1/2$ nature of the baryon there the system has to be described by 5 angles:~\href{https://arxiv.org/pdf/1710.00746.pdf}{{\color{blue}1710.00746}}\\ +\ARROW Impossible to perform a likelihood fit. Need to use moments: +\begin{align*} +M_i = \frac{3}{32\pi^2} \int \sum_{i=1}^{34} K_i(q^2) f(\overrightarrow{\Omega}) d\overrightarrow{\Omega} +\end{align*} + +\column{0.5\textwidth} +\includegraphics[width=0.99\textwidth]{{images/angular_basis.pdf}} + +~~\ARROW In total we have 34 observables! + +\end{columns} + +\textref{LHCb-PAPER-2018-029} +\end{frame} + + +\begin{frame}{$\Lambda_b \to \Lambda \mu \mu$} +\begin{columns} +\column{0.01\textwidth} +{~} +\column{0.6\textwidth} +\ARROW Update with $5~\invfb$.\\ +\ARROW 610 events observed at high $q^2$.\\ +\ARROW Angular efficiency modelled in 6D.\\{~}\\ +\includegraphics[width=0.99\textwidth]{{images/angles.pdf}} + +\column{0.4\textwidth} +\includegraphics[width=0.99\textwidth]{{images/figure51.pdf}}\\ +\ARROW The results:\\{~}\\ +\includegraphics[width=0.99\textwidth]{{images/Ki.pdf}}\\ + + +\end{columns} + +\textref{LHCb-PAPER-2018-029} +\end{frame} + + + +\begin{frame}{$\Pbeauty \to \Pdown$ transitions} + +\ARROW The $\Pbeauty \to \Pdown$ is further suppressed by $\vert V_{td}\vert / \vert V_{ts}\vert$ $\rightarrow~\mathcal{B} \sim \mathcal{O} (10^{-8})$.\\ +\ARROW Already lots of results in Run1: + +\begin{columns} +\column{0.01\textwidth} +{~} +\column{0.33\textwidth} +\includegraphics[angle=-90,width=0.99\textwidth]{{images/pimumu_fitresult0_col}.pdf} +\begin{turn}{90} +\hspace{-2.5cm}\href{ https://arxiv.org/abs/1509.00414 }{ \begin{footnotesize} [JHEP 10 (2015) 034] \end{footnotesize} } +\end{turn} + + + +\column{0.33\textwidth} +\includegraphics[angle=-90,width=0.99\textwidth]{{images/pipimumu}.pdf} +\begin{turn}{90} +\hspace{-3cm}\href{https://arxiv.org/abs/1412.6433}{ \begin{tiny} [PHYS. LETT. B743 (2015) 46] \end{tiny} } +\end{turn} + + +\column{0.33\textwidth} +\includegraphics[angle=-90,width=0.99\textwidth]{{images/Fig3}.pdf} +\begin{turn}{90} +\hspace{-2.5cm}\href{https://arxiv.org/abs/1701.08705}{ \begin{footnotesize} [JHEP 04 (2017) 029] \end{footnotesize} } +\end{turn} + + + +\end{columns} + +\ARROW The ratio between the $\Pbeauty \to \Pstrange$ and $\Pbeauty \to \Pdown$ can be used to determine some CKM elements: +\begin{equation} +\frac{\mathcal{B}(\PB \to \pi \mu \mu)}{\mathcal{B}(\PB \to \PK \mu \mu)} \sim \vert V_{td}/V_{ts} \vert = 0.20 \pm 0.02 \nonumber +\end{equation} +\ARROW Large improvements expected in Run2. + + +\end{frame} + + +\begin{frame}{$\APBs \to \PKstar \mu \mu$} + +\begin{columns} +\column{0.01\textwidth} +{~} +\column{0.5\textwidth} +\ARROW $4.6~\invfb$ of data!\\ +\ARROW Analysis in 4 bins of NN response.\\ +\ARROW Signal yield determined from a simultaneous fit to the NN response bins. \\ +\ARROW Normalized to $\PB \to \PKstar \PJpsi$.\\ +\ARROW First evidence with $3.4~\sigma$. +\column{0.5\textwidth} +\only<2>{ +\includegraphics[angle=-90,width=0.99\textwidth]{{images/tom}.pdf} +} + +\only<1>{ +\includegraphics[angle=-90,width=0.99\textwidth]{{images/tom2}.pdf} +} +\end{columns} +\ARROW The measured branching fraction: +\begin{align*} +\mathcal{B}(\APBs \to \PKstar \mu \mu) = \left( 2.9 \pm 1.0 ({\rm stat}) \pm 0.2 ({\rm syst}) \pm 0.3({\rm norm}) \right) \times 10^{-8} +\end{align*} +\ARROW For now consistent with SM predictions \href{https://arxiv.org/abs/1803.05876}{arXiv:1803.05876} + +\textref{arxiv::1804.07167} + +\end{frame} + +\begin{frame}\frametitle{Lepton Flavour/Number Violation} +\begin{small} + Lepton Flavour Violation(LFV): +\end{small} + + +\begin{footnotesize} + +\ARROW After $\Pmuon$ was discovered it was logical to think of it as an excited $\Pelectron$. +\begin{columns} +\column{3in} +\begin{itemize} +\item Expected: $B(\mu\to\Pe\gamma) \approx 10^{-4}$ +\item Unless another $\Pnu$, in intermediate vector boson loop cancels. +\end{itemize} +\column{2in} +{~}\includegraphics[width=0.98\textwidth]{rabi.png} + +\end{columns} +\begin{columns} +\column{1in} +{~} +\column{3in} +\begin{exampleblock}{I.I.Rabi:} +"Who ordered that?" +\end{exampleblock} +\column{2in} +~~~~{~}\includegraphics[scale=0.08]{II_Rabi.jpg} + +\end{columns} + + +\begin{itemize} +\item Up to this day charged LFV is being searched for in various decay modes. +\item LFV was already found in neutrino sector. +\end{itemize} +\end{footnotesize} + + +\begin{small} + +\ARROW Anomalies may suggest connections between LUV and LFV. + +\end{small} +\begin{footnotesize} + +\begin{columns} + +\column{0.02\textwidth} +{~} +\column{0.5\textwidth} +\begin{align*} +\mathcal{B}(\PB \to \PK e \mu ) \sim 3 \cdot 10^{-8} \left( \frac{1-R_K}{0.23} \right) +\end{align*} + +\begin{align*} +\frac{ \mathcal{B}(\PBs \to e \mu )}{ \mathcal{B}(\PBs \to \mu \mu )} \sim 0.01 \left( \frac{1-R_K}{0.23} \right) +\end{align*} + +\column{0.5\textwidth} +\begin{align*} +\mathcal{B}(\PB \to \PK \mu \tau ) \sim 2 \cdot 10^{-8} \left( \frac{1-R_K}{0.23} \right) +\end{align*} +\begin{align*} +\frac{ \mathcal{B}(\PBs \to \tau \mu )}{ \mathcal{B}(\PBs \to \mu \mu )} \sim 4 \left( \frac{1-R_K}{0.23} \right) +\end{align*} + + +\end{columns} + +\end{footnotesize} + +\textref{arxiv::1609.08895} + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PB_{(s)} \to e \mu$} +\ARROW Need to deal with bremsstrahlung: different efficiency and mass shapes.\\ +\ARROW Fit performed separately in bremsstrahlung categories. + +\begin{columns} + +\column{0.01\textwidth} + +\column{0.6\textwidth} +\ARROW Primary background: $\PB \to hh$: +\includegraphics[angle=-90,width=0.80\textwidth]{images/Fig10.pdf}\\ +\ARROW Estimated with the data driven method to be $<6$ events. + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.99\textwidth]{images/Fig3left.pdf}\\ +\includegraphics[angle=-90,width=0.99\textwidth]{images/Fig3right.pdf} + +\end{columns} + +\textref{[JHEP 1803 (2018) 078]} + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PB_{(s)} \to e \mu$} + + +\begin{columns} + +\column{0.01\textwidth} + +\column{0.57\textwidth} +\ARROW With $3~\invfb$ data.\\ +\ARROW Fit the $m_{e\mu}$ mass and calculate $\rm CL_s$.\\ +\begin{align*} +\mathcal{B}(\PBzero \to e^{\pm} \mu^{\mp}) < 1.3 (1.0) \cdot 10^{-8} +\end{align*} + + +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.99\textwidth]{images/Fig9.pdf}\\ + + + +\end{columns} + + +\begin{columns} + +\column{0.01\textwidth} + +\column{0.75\textwidth} +\includegraphics[angle=-90,width=0.49\textwidth]{images/Fig5left.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/Fig5right.pdf}\\ + +\column{0.25\textwidth} + + +\end{columns} + + + + +\begin{align*} +\mathcal{B}(\PBs \to e^{\pm} \mu^{\mp}) < 6.3 (5.4) \cdot 10^{-9}~~~~~~~~~~~~{\rm if~light~eigenstate~dominates} +\end{align*} +\begin{align*} +\mathcal{B}(\PBs \to e^{\pm} \mu^{\mp}) < 7.2 (6.0) \cdot 10^{-9}~~~~~~~~~~~~{\rm if~heavy~eigenstate~dominates} +\end{align*} +\textref{[JHEP 1803 (2018) 078]} +\end{frame} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PB \to \PKstar e \mu$} + + +\ARROW Fit to $M_{bc}$: +\begin{align*} +M_{bc}=\sqrt{ (E_{beam})^2 - (p_B)^2 } +\end{align*} + +\begin{columns} + +\column{0.01\textwidth} + +\column{0.8\textwidth} +\includegraphics[width=0.99\textwidth]{images/Belle.png} + +\column{0.2\textwidth} +\begin{footnotesize} +\ARROW No statistically significant events observed, upper limits set + +\end{footnotesize} + +\end{columns} + + +\begin{columns} + +\column{0.01\textwidth} + +\column{0.4\textwidth} +\ARROW The best UL but order of magnitude above the LUV model predictions. +\column{0.6\textwidth} +\includegraphics[width=0.8\textwidth]{images/Belle2.png} + +\end{columns} + + +\textref{[Belle, arxiv::1807.03267]} +\end{frame} + + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +{ +\usebackgroundtemplate{\includegraphics[width=\paperwidth,height=\paperheight]{images/charmingpenguing.jpg}} +\begin{frame}[plain] +\end{frame} +} + +\begin{frame}\frametitle{$\Lambda_c \to \Pproton \mu \mu$} + +\vspace{0.5em} + \begin{minipage}{\textwidth} + + +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\vspace{0.5em} + +\ARROW SM predictions:\\ +~~~~~~$\mathcal{O}(10^{-8})$\\ +\ARROW Long distance effects:\\ +~~~~~~$\mathcal{O}(10^{-6})$\\ +~~~~\\ +\ARROW Previous measurement done by Babar:\\ +~~${\rm Br}(\Lambda_c^{+} \to p \mu^+ \mu^-) < 4.4\cdot 10^{-5}$ at 90\% CL\\ +\begin{center} +\includegraphics[width=0.65\textwidth]{images/babar.png}\\ + +\end{center} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/indeks1.jpg}\\ +\includegraphics[width=0.95\textwidth]{images/indeks2.jpg}\\ +\begin{exampleblock}{} +LHCb analysis with $3~\invfb$ +\end{exampleblock} + + +\end{columns} + + \end{minipage} + \vspace*{2.cm} + + + +\textref{[Phys. Rev D 84 072006]} +\end{frame} + + +\begin{frame}\frametitle{$\Lambda_c \to \Pproton \mu \mu$} +\ARROW Blind analysis with the normalization to the $\Lambda_c \to \Pproton \phi(\mu\mu)$.\\ +\ARROW BDT to reduce combinatorial background.\\ +\ARROW The dominant background: $\Lambda_c \to \Pproton \pi \pi$: $2.0\pm1.1$ events + +\begin{columns} + +\column{0.01\textwidth} + +\column{0.6\textwidth} +\includegraphics[angle=-90,width=0.85\textwidth]{{images/Lc2pPhi_presel}.pdf}\\ +Analysis performed in 3 mass windows: +\begin{itemize} +\item $\phi$ region: $m_{\mu\mu} \in \left[ 985, 1055 \right]~{\rm MeV/c^2}$ +\item $\omega$ region: $m_{\mu\mu} \in \left[ 759, 805 \right]~{\rm MeV/c^2}$ +\item nonresonant: rest of phase-space. +\end{itemize} +\column{0.4\textwidth} +\includegraphics[width=0.85\textwidth]{{images/pmumu_masses}.pdf} + + +\end{columns} + + +\textref{[PHYS. REV. D 97, 091101 (2018)]} + +\end{frame} + + + + +\begin{frame}\frametitle{$\Lambda_c \to \Pproton \mu \mu$} + +\begin{columns} + +\column{0.02\textwidth} + +\column{0.5\textwidth} +\ARROW It's the first observation of $\Lambda_c \to \Pproton \mu \mu$ in the $\omega$ region, with $5.0~\sigma$ significance.\\ +\ARROW The corresponding branching fraction reads: +\begin{align*} +\mathcal{B}(\Lambda_c \to \Pproton \omega) = \left( 9.4 \pm 3.2 \pm 1.0 \pm 2.0 \right) \cdot 10^{-4} +\end{align*} +\ARROW No significant excess observed in the nonresonant region: +\begin{align*} +\mathcal{B}(\Lambda_c \to \Pproton \mu \mu) < 7.7(9.6) \times 10^{-8} +\end{align*} +\ARROW Improving BaBar result by 3 orders of magnitude! +\column{0.5\textwidth} +\includegraphics[angle=-90,width=0.92\textwidth]{{images/Lc_mumu_mass_fit_sel}.pdf}\\ +\includegraphics[angle=-90,width=0.92\textwidth]{{images/Lc2pmumu_bf90}.pdf} + + +\end{columns} + +\textref{[PHYS. REV. D 97, 091101 (2018)]} +\end{frame} + + + + + + + + + +\begin{frame}\frametitle{$\PD \to h h \mu \mu$} + + +\begin{columns} + +\column{0.02\textwidth} + +\column{0.5\textwidth} +\includegraphics[width=0.9\textwidth]{{images/Fig1D}.pdf}\\ + +\ARROW First observation with $2~\invfb$ of data!\\ +\ARROW Dominated by long distance contributions.\\ +\ARROW Normalized to $\PD \to \PK \pi [\mu \mu]_{\omega/\rho}$ +\ARROW LHCb has measured the branching fractions: +\begin{footnotesize} +\begin{align*} +\mathcal{B}(\PD \to \pi \pi \mu \mu) = \left( 9.64 \pm 0.48 \pm 0.51 \pm 0.97 \right) \cdot 10^{-7} +\end{align*} +\begin{align*} +\mathcal{B}(\PD \to \PK \PK \mu \mu) = \left( 1.54 \pm 0.27 \pm 0.09 \pm 0.16 \right) \cdot 10^{-7} +\end{align*} +\end{footnotesize} + +\column{0.5\textwidth} +\includegraphics[angle=-90,width=0.82\textwidth]{{images/Fig7aD}.pdf}\\ +\includegraphics[angle=-90,width=0.82\textwidth]{{images/Fig7bD}.pdf} +\end{columns} + +\textref{[PHYS. REV. LETT. 119, 181805 (2017)]} +\end{frame} + + + + + +\begin{frame}\frametitle{$\PD \to h h \mu \mu$} + +\begin{columns} + +\column{0.02\textwidth} + +\column{0.5\textwidth} +\ARROW The challenge is to disentangle the SD and LD.\\ +\ARROW Angular observables can help: +\begin{footnotesize} + +\begin{align*} +A_{FB}=\frac{\Gamma(\cos \theta_{\mu} >0) - \Gamma(\cos \theta_{\mu} <0 ) }{\Gamma(\cos \theta_{\mu} >0) + \Gamma(\cos \theta_{\mu} <0) } +\end{align*} + +\begin{align*} +A_{2\phi}=\frac{\Gamma(\sin 2 \phi >0) - \Gamma(\sin 2 \phi <0 ) }{\Gamma(\sin 2 \phi >0) + \Gamma(\sin 2 \phi <0) } +\end{align*} + +\begin{align*} +A_{CP}=\frac{\Gamma(\PD \to hh\mu\mu ) - \Gamma(\APD \to hh\mu\mu ) }{\Gamma(\PD \to hh\mu\mu ) + \Gamma(\APD \to hh\mu\mu ) } +\end{align*} + +\begin{alertblock}{} +Analysis with $5~\invfb$.\\ +See M. Gersabeck talk for more details! +\end{alertblock} + +\end{footnotesize} + + + + +\column{0.5\textwidth}\includegraphics[width=0.82\textwidth]{{images/Fig1DD}.pdf}\\ +\includegraphics[angle=-90,width=0.82\textwidth]{{images/Fig2aDD}.pdf} +\end{columns} + + +\textref{[arXiv:1806.10793]} + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}\frametitle{$\PD \to h h \mu \mu$} + +\begin{columns} + +\column{0.02\textwidth} + +\column{0.5\textwidth} +\ARROW Need to perform a 4D acceptance correction.\\ +\ARROW BDT technique used to determine it.\\ +\includegraphics[width=0.6\textwidth]{{images/Fig6a}.pdf}\\ +\ARROW Yields done by a weighted likelihood fit.\\ +\begin{exampleblock}{} +All observables consistent with $0$! +\end{exampleblock} + + + +\column{0.5\textwidth} + +\includegraphics[angle=-90,width=0.45\textwidth]{{images/Fig9aDD}.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/Fig9bDD}.pdf}\\ +\includegraphics[angle=-90,width=0.45\textwidth]{{images/Fig9cDD}.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/Fig9dDD}.pdf}\\ +\includegraphics[angle=-90,width=0.45\textwidth]{{images/Fig9eDD}.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/Fig9fDD}.pdf}\\ + + +\end{columns} + + +\textref{[arXiv:1806.10793]} + +\end{frame} + + +{ +\usebackgroundtemplate{\includegraphics[width=\paperwidth,height=\paperheight]{images/strange.jpg}} +\begin{frame}[plain] +\end{frame} +} + + +\begin{frame}{$\PKshort \to \mu \mu$} +{~} +\begin{minipage}{\textwidth} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{center} + +\begin{columns} +\column{0.60\textwidth} +\ARROW $\Pproton \Pproton$ collisions create enormous amount of strange mesons.\\ +\ARROW Can be used to search for $\PKshort \to \mu \mu$.\\ +\ARROW SM prediction: $\Br(\PKshort \to \mu \mu)= (5.0 \pm 1.5) \times 10^{-12}$\\ +\ARROW Dominated by the long distance effects.\\ +%\ARROW We used two types of triggers: TIS and TOS.\\ +\ARROW Bkg dominated by $\PKshort \to \pi \pi$. + +\includegraphics[width=0.75\textwidth]{{images/ks2mumu2}.png}\\ + + + + +\column{0.4\textwidth} + +\includegraphics[width=0.95\textwidth]{images/ks2mumu.png}\\ +\ARROW No significant enhancement of signal has been observed and UL was set: +\begin{alertblock}{}\begin{small} +$\Br(\PKshort \to \mu \mu) <0.8 (1.0) \times 10^{-9}$ at $90 (95)\%$ CL +\end{small} +\end{alertblock} + + +\end{columns} +\end{center} + +\end{minipage} +\textref{EUR. PHYS. J. C, 77 10 (2017) 678} +\vspace*{2.1cm} +\end{frame} + + + + + + + +\begin{frame}\frametitle{$\Sigma \to \Pproton \mu \mu$} + +\ARROW $\Sigma \to \Pproton \mu \mu$ is a $\Pstrange \to \Pdown$ transition, which in SM are dominated by LD:~$\mathcal{O}(10^{-8})$.\\ +\begin{center} +\includegraphics[width=0.25\textwidth]{{images/Fig9aS}.pdf} +\includegraphics[width=0.25\textwidth]{{images/Fig9bS}.pdf}\\ + +\end{center} + +\ARROW Previously HyperCP collaboration reported evidence of this decay: $\mathcal{B}(\Sigma \to \Pproton \mu \mu) = \left( 8.6^{+6.6}_{-5.4} \pm 5.5 \right) \cdot 10^{-8}$ \begin{footnotesize} [Phys Rev Lett 94 021801, 2005] \end{footnotesize}\\ + +\begin{columns} +\column{0.02\textwidth} + + + +\column{0.50\textwidth} + +\ARROW Calibrated with $\PK \to \pi \pi \pi$: resolution of $4.28~{\rm MeV/c^2}$. + +\begin{exampleblock}{} +Used $3~\invfb$ of data. +\end{exampleblock} + +\column{0.5\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/Fig6S}.pdf}\\ + + +\end{columns} + + +\textref{PHYS. REV. LETT. 120, 221803 (2018)} + +\end{frame} + +\begin{frame}\frametitle{$\Sigma \to \Pproton \mu \mu$} + + +\begin{columns} +\column{0.02\textwidth} + + + +\column{0.50\textwidth} + +\ARROW Normalize to $\Sigma \to \Pproton \gamma$.\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/Fig1S}.pdf}\\ + +\ARROW Evidence with $4.1~\sigma$ significance. +\ARROW Branching fraction measured: +\begin{align*} +\mathcal{B}( \Sigma \to \Pproton \mu \mu ) = \left( 2.2^{+1.8}_{-1.3} \right) \cdot 10^{-8} +\end{align*} + +\column{0.5\textwidth} +\includegraphics[angle=-90,width=0.9\textwidth]{{images/Fig2}.pdf}\\ +\includegraphics[angle=-90,width=0.9\textwidth]{{images/Fig3S}.pdf}\\ + + +\end{columns} + + +\textref{EUR. PHYS. J. C, 77 10 (2017) 678} + + +\end{frame} + + +\begin{frame}\frametitle{Summary} + +\ARROW FCNC processes provide powerful constraints on extensions of the SM. \\ +\ARROW Large $\Pbeauty\APbeauty$ cross-section provides a large sample of ''rare'' decay processes.\\ +\ARROW More results being updated with Run2 data.\\ +\begin{center} +\includegraphics[width=0.6\textwidth]{images/2017stat.png} +\end{center} + +\ARROW Stay tuned for more results! + +\end{frame} + + + + + + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/FPCP_2018/mchrzasz.toc b/FPCP_2018/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/FPCP_2018/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/FPCP_2018/tikzfeynman.sty b/FPCP_2018/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/FPCP_2018/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/HQL_2014/LFV/hql2.log b/HQL_2014/LFV/hql2.log index 20fa92a..f63e2ad 100644 --- a/HQL_2014/LFV/hql2.log +++ b/HQL_2014/LFV/hql2.log @@ -1,4 +1,4 @@ -This is pdfTeX, Version 3.14159265-2.6-1.40.16 (TeX Live 2015/Debian) (preloaded format=pdflatex 2017.1.21) 22 MAR 2017 21:08 +This is pdfTeX, Version 3.14159265-2.6-1.40.16 (TeX Live 2015/Debian) (preloaded format=pdflatex 2018.1.14) 7 JUL 2018 11:05 entering extended mode restricted \write18 enabled. %&-line parsing enabled. @@ -1644,7 +1644,7 @@ ] LaTeX Info: Redefining \HepProcess on input line 92. - + File: det.jpg Graphic file (type jpg) Package pdftex.def Info: det.jpg used on input line 118. @@ -1665,13 +1665,13 @@ <./det.jpg>] LaTeX Info: Redefining \HepProcess on input line 120. - + File: rabi.png Graphic file (type png) Package pdftex.def Info: rabi.png used on input line 185. 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b/KIT_2018/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/KIT_2018/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/KIT_2018/beamerinnerthemeFlip.sty b/KIT_2018/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/KIT_2018/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/KIT_2018/beamerouterthemeFlip.sty b/KIT_2018/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/KIT_2018/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/KIT_2018/beamerouterthemedecolines.sty b/KIT_2018/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/KIT_2018/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/KIT_2018/beamerthemeFlip.sty b/KIT_2018/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/KIT_2018/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/KIT_2018/distracted_ilissa-ocko-cartoon.jpg b/KIT_2018/distracted_ilissa-ocko-cartoon.jpg new file mode 100644 index 0000000..5f007b0 --- /dev/null +++ b/KIT_2018/distracted_ilissa-ocko-cartoon.jpg Binary files differ diff --git a/KIT_2018/images/1.png b/KIT_2018/images/1.png new file mode 100644 index 0000000..b1b3955 --- /dev/null +++ b/KIT_2018/images/1.png Binary 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glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\MeV}{\rm{MeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\re}{{\rm Re}} +\newcommand{\invfb}{\rm{fb^{-1}}} +\newcommand{\fixme}{\rm{{\color{red}{FIXME!}}}} +\newcommand{\thetal}{\theta_l} +\newcommand{\thetak}{\theta_k} +\newcommand{\nn}{\nonumber} +\newcommand{\eq}[1]{\begin{equation} #1 \end{equation}} +%\newcommand{\eqn}[1]{\begin{displaymath} #1 \end{displaymath}} +\newcommand{\eqa}[1]{\begin{eqnarray} #1 \end{eqnarray}} +\newcommand{\apeL}{{A_\perp^L}} +\newcommand{\apeR}{{A_\perp^R}} +\newcommand{\ape}{{A_\perp}} +\newcommand{\apeLR}{{A_\perp^{L,R}}} +\newcommand{\apaL}{{A_\|^L}} +\newcommand{\apaR}{{A_\|^R}} +\newcommand{\apa}{{A_\|}} +\newcommand{\apaLR}{{A_\|^{L,R}}} +\newcommand{\azeL}{{A_0^L}} +\newcommand{\azeR}{{A_0^R}} +\newcommand{\aze}{{A_0}} + +\newcommand{\azeLR}{{A_0^{L,R}}} +\newcommand{\Real}{\ensuremath{\mathcal{R}e}\xspace} +\newcommand{\Imag}{\ensuremath{\mathcal{I}m}\xspace} + +\renewcommand{\C}[1]{{\cal C}_{#1}} +\newcommand{\Ceff}[1]{{\cal C}^{\rm eff}_{#1}} +\newcommand{\Cpeff}[1]{{\cal C}^{\rm eff\prime}_{#1}} +\newcommand{\Cp}[1]{{\cal C}^{\prime}_{#1}} +\def\FL {\ensuremath{F_{\mathrm{L}}}\xspace} +\def\ATDPH {\ensuremath{A_{\mathrm{T,PR}}^{(2)}}\xspace} +\def\ATImPH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Im}}}\xspace} +\def\ATRePH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Re}}}\xspace} +\def\FLPH {\ensuremath{F_{\mathrm{L,PR}}}\xspace} +\def\ATDKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{(2)}}\xspace} +\def\ATImKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Im}}}\xspace} +\def\ATReKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Re}}}\xspace} +\def\FLKG {\ensuremath{F_{\mathrm{L,\Kstarz \gamma}}}\xspace} +\def\ATD {\ensuremath{A_{\mathrm{T}}^{(2)}}\xspace} +\def\ATIm {\ensuremath{A_{\mathrm{T}}^{\mathrm{Im}}}\xspace} +\def\ATRe {\ensuremath{A_{\mathrm{T}}^{\mathrm{Re}}}\xspace} +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} + + + +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + + + +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\mathcal{B}}} + +\newcommand{\av}[1]{\langle #1 \rangle} +% particles +\def\LstFTTT {\ensuremath{\PLambda^{*}(1520)^{0}}\xspace} +\def\dll {\ensuremath{\mathrm{DLL}}\xspace} + \def\Lb {\ensuremath{\PLambda_b}} + + +% useful decays +\def\BdToKpimm {\decay{\Bd}{\Kp\pim\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsToJPsiKst {\decay{\Bs}{\jpsi\Kstarz}} +\def\BdTopsitwosKst {\decay{\Bd}{\psitwos\Kstarz}} +\def\LstFTTTT {\decay{\LstFTTT}{p\Km}} +%\def\LbToLstmm {\decay{\Lb}{\PLambda^{*}(1520)^{0} \mumu}} +\def\LbTopKmm {\decay{\Lb}{p\Km\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsTophimm {\decay{\Bs}{\Pphi\mumu}} + +% interesting variables +\def\mkpi {\ensuremath{m_{K\pi}}\xspace} +\def\mkpimm{\ensuremath{m_{K\pi\mu\mu}}\xspace} + +%% peaking background mass hypotheses +\def\mkmm {\ensuremath{m_{K\mu\mu}}\xspace} +\def\mSwappKmm {\ensuremath{m_{(\pi\to p)K\mu\mu}}\xspace} +\def\mSwappiK {\ensuremath{m_{(\pi\to K)K}}\xspace} +\def\mSwappiKmm {\ensuremath{m_{(\pi\to K)K\mu\mu}}\xspace} +\def\mSwappK {\ensuremath{m_{(\pi\to p)K}}\xspace} +\def\mDoubleSwappKmm {\ensuremath{m_{(K\to p)(\pi\to K)\mu\mu}}\xspace} +\def\mDoubleSwappK {\ensuremath{m_{(K\to p)(\pi\to K)}}\xspace} +\def\mSwapKst {\ensuremath{m_{K\leftrightarrow\pi}}\xspace} + +%% some other decays +\def\BsToPhimm {\decay{\Bs}{\phi\mumu}} +\def\BsToPhimmFULL {\decay{\Bs}{\phi(\to\!K^{+}K^{-})\mumu}} +\def\BsToKKmm {\decay{\Bs}{\Kp\Km\mumu}} + +\newcommand{\delC}[1]{\delta {\cal C}_{#1}} +\newcommand{\dC}[1]{{\cal C}_{#1}^{\rm NP}} +\newcommand{\dCp}[1]{{\cal C}_{#1^\prime}^{\rm NP}} + + + + +\definecolor{green}{rgb}{0.2,0.6,0.2} +\definecolor{lightgreen}{rgb}{0.4,1,0.4} +\definecolor{verylightgreen}{rgb}{0.7,1,0.7} +\def\cgreen{\color{green}} +\definecolor{brown}{rgb}{0.4,0.2,0.0} +\def\cbrown{\color{brown}} +\def\cred{\color{red}} +\definecolor{darkblue}{rgb}{0.0,0.0,1.0} +\def\cdarkblue{\color{darkblue}} +\definecolor{darkgrey}{rgb}{0.4,0.4,0.4} +\definecolor{lightgrey}{rgb}{0.7,0.7,0.7} +\definecolor{verylightblue}{rgb}{0.8,0.8,1.0} +\definecolor{lightblue}{rgb}{0.6,0.6,1.0} +\definecolor{verylightyellow}{rgb}{1.0,1.0,0.5} +\definecolor{lightyellow}{rgb}{1.0,0.7,0.3} +\definecolor{darkred}{rgb}{0.6,0.0,0.0} + +\definecolor{green}{rgb}{0.3,0.6,0.2} +\definecolor{green}{rgb}{0.3,0.7,0.4} + + + +\definecolor{indigo}{RGB}{100,0,100} +\definecolor{dgray}{RGB}{80,80,80} +\definecolor{lgray}{RGB}{220,220,220} +\definecolor{dred}{RGB}{190,0,0} +\definecolor{dgreen}{RGB}{0,110,0} +\definecolor{lyellow}{RGB}{245,245,210} +\definecolor{bblue}{RGB}{93,93,255} +\definecolor{bbrown}{RGB}{150,85,52} +\definecolor{llgray}{RGB}{230,230,230} + + + +\newcommand{\F}{\mathcal{F}} +\newcommand{\A}{\mathcal{A}} +\newcommand{\N}{\mathcal{N}} +\renewcommand{\H}{\mathcal{H}} +\newcommand{\Leff}{\mathcal{L}_{\rm eff}} +\newcommand{\heff}{\mathcal{H}_{\rm eff}} +\newcommand{\Lag}{\mathcal{L}} +\newcommand{\red}{\color{red}} +\newcommand{\blue}{\color{blue}} +\newcommand{\indigo}{\color{indigo}} +\newcommand{\brown}{\color{bbrown}} +\newcommand{\bs}{\mathbf} +\newcommand{\sss}{\scriptscriptstyle} +\newcommand{\btr}{{ $\blacktriangleright\ $}} + + +\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (CERN, IFJ PAN)} +\institute{UZH} +\title[Quo Vadis flavor anomalies?]{Quo Vadis flavor anomalies?} +\date{25 September 2014} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.9\textwidth} + \flushright\fontspec{Trebuchet MS}\bfseries \Huge {Quo Vadis flavor anomalies?} + \end{column} + \begin{column}{0.2\textwidth} + %\includegraphics[width=\textwidth]{SHiP-2} + \end{column} + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} {\fontspec{Trebuchet MS} \Large Marcin Chrząszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=1.3cm]{cern}{~}{~} +\includegraphics[height=1.1cm]{ifj.png} +\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + \textcolor{normal text.fg!50!Comment}{The Future of Particle Physics: A Quest for Guiding Principles \\October 2, 2018} +\end{center} +\end{frame} +} + + +\begin{frame}{Outline} + + \begin{minipage}{\textwidth} +{~}\\ + +\begin{enumerate} +\item The flavour anomalies: +\begin{itemize} +\item $R(\PDstar)$ +\item $R_K$ and $R_{\PKstar}$ +\item $P_5^{\prime}$ +\end{itemize} +\item Global fits results. +\item Conclusions. +\end{enumerate} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + +\begin{frame}\frametitle{Modern Flavour Physics} +\begin{center} +\only<1>{ +\includegraphics[width=1.05\textwidth]{1.png} +} +\only<2>{ +\includegraphics[width=1.05\textwidth]{2.png} + +} +\end{center} + + + + +\end{frame} + + +\begin{frame}\frametitle{Why semi-leptonic decays?} +\begin{large} +\ARROW A decay is semi-leptonic if its products are part leptons +and part hadrons. +\end{large} + +\begin{center} +\includegraphics[width=0.99\textwidth]{3.png} +\end{center} + +\begin{large} +\ARROW These decays can be factorised into the weak and +strong parts, greatly simplifying theoretical calculations. +\end{large} + + +\end{frame} + + + +\begin{frame}\frametitle{Types of semi-leptonic decays} + +\begin{center} +\includegraphics[width=1.05\textwidth]{4.png} +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Anomalies} + +\only<1>{ +\ARROW Today I will talk about three anomalies in $\PB$ +decays: +\begin{itemize} +\item $R(\PDstar)$ +\item $R_{\PK/\PKstar}$ +\item $P^{\prime}_5$ +\end{itemize} + +} + +\end{frame} + + + +\begin{frame} + +\begin{center} + +\begin{Huge}Anomaly 1\\ +\begin{align*} +R(\PDstar) = \frac{\Br (\PB \to \PDstar \tau \nu )}{\Br(\PB \to \PDstar \mu \nu)} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{$R(\PDstar) $} + +\begin{large} + +\ARROW Large rate of charged current decays allow for measurement +in semi-tauonic decays +\end{large} + +\begin{columns} +\column{0.5\textwidth} +\begin{align*} +R(\PDstar) = \frac{\Br (\PB \to \PDstar \tau \nu )}{\Br(\PB \to \PDstar \mu \nu)} +\end{align*} +\column{0.5\textwidth} +\begin{large} +\ARROW Form ratio of decays with different lepton generations.\\ +\ARROW Cancel QCD uncertainties. +\end{large} + +\end{columns} +~\\ +\begin{large} + +\ARROW $R(\PDstar)$ is sensitive to the NP with strong 3rd generation couplings. +\end{large} + +\includegraphics[width=0.8\textwidth]{images/7.png} + + +\end{frame} + +\begin{frame}\frametitle{The Rule of three} + +\begin{center} + +\includegraphics[width=1.\textwidth]{images/8.png} + +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Experimental challenges} +\begin{large} +\ARROW With the $\tau \to \mu \nu \nu$ decay we are missing 3 neutrinos!\\ +\ARROW No sharp peak in any distributions.\\ +\end{large} +{~}\\ +\begin{columns} +\column{0.5\textwidth} +\begin{large} +\ARROW At B-factories, can control this +using tagging technique.\\ +\end{large} + + +\includegraphics[width=0.9\textwidth]{9.png} + +\column{0.5\textwidth} + + +\includegraphics[width=0.9\textwidth]{10.png}\\ +\begin{large} +\ARROW More difficult at LHCb, compensate +using large boost (flight information) +and huge B production\\ +\end{large} +\end{columns} + +\end{frame} + +\iffalse + +\begin{frame}\frametitle{Signal fits} +\ARROW Three main backgrounds: +\begin{itemize} +\item $\PB \to \PDstar \ell \nu$. +\item $\PB \to \PD^{\ast \ast} \ell \nu$. +\item $\PB \to \PD \PDstar X$ +\end{itemize} +\begin{center} +\includegraphics[width=0.9\textwidth]{12.png} +\end{center} +\ARROW Fit variables which discriminate between the signal and background modes. + +\end{frame} + +\begin{frame}\frametitle{Results} +\ARROW All experiments see an access w.r.t. to SM prediction: +\begin{center} +\includegraphics[angle=-90,width=0.6\textwidth]{rdrds_winter2017.pdf} +\end{center} +\ARROW Theoretical uncertainties negligible.\\ +\ARROW The ball is on the experimental side. + +\end{frame} + + +\fi +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + + +\begin{frame}\frametitle{Introduction to anomaly 2 \& 3} + +\begin{columns} +\column{4in} +\begin{itemize} +\item The SM allows only the charged interactions to change flavour. +\begin{itemize} +\item Other interactions are flavour conserving. +\end{itemize} +\item One can escape this constraint and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. +\begin{itemize} +\item These kind of processes are suppressed in SM $\to$~Rare decays. +\item New Physics can enter in the loops. +\end{itemize} +\end{itemize} +\begin{center} +\includegraphics[scale=0.3]{lupa.png} +\includegraphics[scale=0.3]{example.png} +\end{center} +\column{1.5in} +\includegraphics[width=0.61\textwidth]{couplings.png} +\end{columns} + +\end{frame} + + +\begin{frame}{Analysis of Rare decays} +\begin{footnotesize} + +%{\Large Since a long time ago...} \\ \medskip +%\hspace*{1.4cm}$\Rightarrow$ $b \to s \gamma$ and $b \to s \ell\ell $ {\bf Flavour Changing Neutral Currents} have been used as {\bf \cred Our Portal} \\ to explore the fundamental theory beyond SM. \\ +%\medskip +%\medskip +%\hfill....... with not much success till 2013.\hspace*{1cm} +%\bigskip + +Analysis of FCNC in a model-independent approach, effective Hamiltonian: +\vspace*{-0.1cm} +\begin{columns} +\begin{column}{1cm} +~ +\end{column} +\begin{column}{8cm} +\begin{equation*} +b\to s\gamma(^*): {\mathcal H}^{SM}_{\Delta F=1} \propto + \sum_{i=1}^{10} V_{ts}^* V_{tb} {\cgreen \C{i}} \alert{ {\cal O}_i} + \ldots +\end{equation*} + +\vspace{-0.2cm} + +\begin{itemize} +\item $\alert{ {\cal O}_7} = \frac{e}{16 \pi^2}m_b\, + (\bar s\sigma^{\mu\nu} P_R b) F_{\mu\nu}\,$ %\quad [real or soft photon] +\item $\alert{ {\cal O}_9}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b)\ (\bar\ell\gamma_\mu\ell)$ + %\quad [$b\to s\mu\mu$ via $Z$/hard $\gamma$] +\item $\alert{ {\cal O}_{10}}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b) \ (\bar\ell\gamma_\mu\gamma_5\ell)$, ... +%\quad [$b\to s\mu\mu$ via $Z$] +\end{itemize} +\end{column} +\begin{column}{5.5cm} +\includegraphics[width=3.5cm]{images/qum1.png} +%\includegraphics[width=3cm]{bsll.pdf} +\end{column} +\end{columns} + +%\hspace*{5cm} with no clear success yet... +%\bigskip + + +%\centerline{{\bf Goal}: \underline{Decode the short distance physics to find a smoking gun of BSM}\hspace*{2cm}} + + +\bigskip +\hspace*{0.0cm} $\bullet$ {\bf SM} Wilson coefficients up to NNLO + e.m. corrections at $\mu_{ref}=4.8$ GeV [{\cgreen Misiak et al.}]: $${\cal C}_7^{\rm SM}=-0.29,\, {\cal C}_9^{\rm SM}=4.1,\, {\cal C}_{10}^{\rm SM}=-4.3$$ +%BUT, like in the film there is always the good, the bad and the ugly. +\bigskip +$\bullet$ {\bf NP} changes short distance ${\cal C}_i-{\cal C}_i^{\rm SM}={\cal C}_i^{\rm NP}$ and induce new operators, like ${\cal O}^\prime_{7,9,10}={\cal O}_{7,9,10}\,\, (P_L \leftrightarrow P_R)$ ... also scalars, pseudoescalar, tensor operators...%\bigskip + + +\end{footnotesize} + +\end{frame} + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 2\\ +\begin{align*} +R_{\PK/\PKstar} = \frac{\Br(\PB \to \PK/\PKstar \mu \mu)}{\Br(\PB \to \PK/\PKstar e e)} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + + + +\begin{frame}\frametitle{Measurement at LHCb} + +\ARROW Most precise measurements performed at LHCb.\\ +\ARROW Main challenge is due to electron Bremsstrahlung.\\ +\begin{center} +\includegraphics[width=0.99\textwidth]{13.png} +\end{center} +\ARROW To protect ourself from electron reconstruction issue we use double ratio: +\begin{align*} +R_K = \frac{ \Br(\PB \to \PK \mu \mu ) \times \Br(\PB \to \PK \PJpsi(\to e e)) }{ \Br(\PB \to \PK e e ) \times \Br(\PB \to \PK \PJpsi(\to \mu \mu)) } +\end{align*} + + +\end{frame} + + +\begin{frame}\frametitle{Result} + +\begin{center} +\begin{large} +\begin{align*} +R_K = 0.745^{+0.090}_{-0.074} ({\rm stat.}) \pm 0.036 ({\rm syst}) +\end{align*} +\end{large} + +\includegraphics[width=0.7\textwidth]{images/RK.png}\\ + +\end{center} +\ARROW $2.6~\sigma$ away from SM prediction. +\end{frame} + +\begin{frame}\frametitle{The continuation - $R_{\PKstar}$} +\ARROW The neutral continuation of the $R_K$ measurement is to measure its partner: +\begin{center} +\begin{align*} +R_{\PKstar} = \frac{\Br(\PB \to \PKstar \mu \mu)}{\Br(\PB \to \PKstar e e)} +\end{align*} +\end{center} + + +\begin{columns} +\column{0.4\textwidth} +\ARROW Measurement performed in two $q^2$ bins. \\ +\ARROW Normalized in double ratio to $\PB \to \PKstar \PJpsi$.\\ +\includegraphics[width=0.95\textwidth]{images/plot.png} + + +\column{0.6\textwidth} +\begin{center} +\includegraphics[width=0.95\textwidth]{Fig10a.pdf} +\end{center} + +\end{columns} + + + +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PB \to \PKstar^{\pm} \Pmu \Pmu$} +{~} +\includegraphics[width=0.5\textwidth]{images/ksmumu_BF.png} +\includegraphics[width=0.5\textwidth]{images/kmumu_BF.png} + +\begin{center} +\begin{columns} + +\column{0.4\textwidth} +\begin{itemize} +\item Despite large theoretical errors the results are consistently smaller than SM prediction. +\end{itemize} +\column{0.6\textwidth} +\includegraphics[width=0.87\textwidth]{images/bukst_BF.png} + + +\end{columns} + + + + + + + +\end{center} + \vspace*{2.1cm} +\end{frame} + + + + + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 3\\ +\begin{align*} +P_5^{\prime} = \sqrt{2} \frac{\Re (\apeL \apaL^{\ast} - \apeR \apaR^{\ast} )}{\sqrt{ |\aze|^2 ( |\ape|^2 + |\aze|^2 )}} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + + +%\azeLR +%\apaLR +%\apeLR + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{$\PBzero \to \PKstar \Pmuon \APmuon$ kinematics} +{~} + \begin{minipage}{\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ The kinematics of $\PBzero \to \PKstar \Pmuon \APmuon$ decay is described by three angles $\thetal$, $\thetak$, $\phi$ and invariant mass of the dimuon system ($q^2)$: +{\tiny{ +\eqa{\label{dist} +\frac{d^4\Gamma}{dq^2\,d\!\cos\theta_K\,d\!\cos\theta_l\,d\phi}&=&\frac9{32\pi} \bigg[ +J_{1s} \sin^2\theta_K + J_{1c} \cos^2\theta_K + (J_{2s} \sin^2\theta_K + J_{2c} \cos^2\theta_K) \cos 2\theta_l\nn\\[1.5mm] +&&\hspace{-2.7cm}+ J_3 \sin^2\theta_K \sin^2\theta_l \cos 2\phi + J_4 \sin 2\theta_K \sin 2\theta_l \cos\phi + J_5 \sin 2\theta_K \sin\theta_l \cos\phi \nn\\[1.5mm] +&&\hspace{-2.7cm}+ (J_{6s} \sin^2\theta_K + {J_{6c} \cos^2\theta_K}) \cos\theta_l ++ J_7 \sin 2\theta_K \sin\theta_l \sin\phi + J_8 \sin 2\theta_K \sin 2\theta_l \sin\phi \nn\\[1.5mm] +&&\hspace{-2.7cm}+ J_9 \sin^2\theta_K \sin^2\theta_l \sin 2\phi \bigg]\,, +\nonumber} +}} + + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +\fi + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Transversity amplitudes } +{~} + \begin{minipage}{\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ One can link the angular observables to transversity amplitudes +{\tiny{ +\eqa{ +J_{1s} & = & \frac{(2+\beta_\ell^2)}{4} \left[|\apeL|^2 + |\apaL|^2 +|\apeR|^2 + |\apaR|^2 \right] + + \frac{4 m_\ell^2}{q^2} \re\left(\apeL\apeR^* + \apaL\apaR^*\right)\,,\nn\\[1mm] +% +J_{1c} & = & |\azeL|^2 +|\azeR|^2 + \frac{4m_\ell^2}{q^2} \left[|A_t|^2 + 2\re(\azeL^{}\azeR^*) \right] + \beta_\ell^2\, |A_S|^2 \,,\nn\\[1mm] +% +J_{2s} & = & \frac{ \beta_\ell^2}{4}\left[ |\apeL|^2+ |\apaL|^2 + |\apeR|^2+ |\apaR|^2\right], +\hspace{0.92cm} J_{2c} = - \beta_\ell^2\left[|\azeL|^2 + |\azeR|^2 \right]\,,\nn\\[1mm] +% +J_3 & = & \frac{1}{2}\beta_\ell^2\left[ |\apeL|^2 - |\apaL|^2 + |\apeR|^2 - |\apaR|^2\right], +\qquad J_4 = \frac{1}{\sqrt{2}}\beta_\ell^2\left[\re (\azeL\apaL^* + \azeR\apaR^* )\right],\nn \\[1mm] +% +J_5 & = & \sqrt{2}\beta_\ell\,\Big[\re(\azeL\apeL^* - \azeR\apeR^* ) - \frac{m_\ell}{\sqrt{q^2}}\, +\re(\apaL A_S^*+ \apaR^* A_S) \Big]\,,\nn\\[1mm] +% +J_{6s} & = & 2\beta_\ell\left[\re (\apaL\apeL^* - \apaR\apeR^*) \right]\,, +\hspace{2.25cm} J_{6c} = 4\beta_\ell\, \frac{m_\ell}{\sqrt{q^2}}\, \re (\azeL A_S^*+ \azeR^* A_S)\,,\nn\\[1mm] +% +J_7 & = & \sqrt{2} \beta_\ell\, \Big[\im (\azeL\apaL^* - \azeR\apaR^* ) + +\frac{m_\ell}{\sqrt{q^2}}\, \im (\apeL A_S^* - \apeR^* A_S)) \Big]\,,\nn\\[1mm] +% +J_8 & = & \frac{1}{\sqrt{2}}\beta_\ell^2\left[\im(\azeL\apeL^* + \azeR\apeR^*)\right]\,, +% +\hspace{1.9cm} J_9 = \beta_\ell^2\left[\im (\apaL^{*}\apeL + \apaR^{*}\apeR)\right] \,, +\label{Js}\nonumber} +}} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Link to effective operators} +{~} + \begin{minipage}{\textwidth} +$\color{JungleGreen}{\Rrightarrow}$ So here is where the magic happens. At leading order the amplitudes can be written as: +{\tiny{ +\eqa{ +\apeLR &=&\sqrt{2} N m_B(1- \hat s)\bigg[ (\Ceff9 + \Cpeff9) \mp (\C{10} + \Cp{10}) ++\frac{2\hat{m}_b}{\hat s} (\Ceff7 + \Cpeff7) \bigg]\xi_{\bot}(E_{K^*}) \nn \\[2mm] +\apaLR &=& -\sqrt{2} N m_B (1-\hat s)\bigg[(\Ceff9 - \Cpeff9) \mp (\C{10} - \Cp{10}) ++\frac{2\hat{m}_b}{\hat s}(\Ceff7 - \Cpeff7) \bigg] \xi_{\bot}(E_{K^*}) \nn \\[2mm] +\azeLR &=& -\frac{N m_B (1-\hat s)^2}{2 \hat{m}_{K^*} \sqrt{\hat s}} \bigg[ (\Ceff9 - \Cpeff9) \mp (\C{10} - \Cp{10}) + 2\hat{m}_b (\Ceff7 - \Cpeff7) \bigg]\xi_{\|}(E_{K^*}), +\label{LargeRecoilAs}\nonumber} +}} +where $\hat s = q^2 /m_B^2$, $\hat{m}_i = m_i/m_B$. The $\xi_{\|,\bot }$ are the form factors. \\ +\pause +$\color{JungleGreen}{\Rrightarrow}$ Now we can construct observables that cancel the $\xi$ form factors at leading order: +\eq{P_5^{\prime} = \dfrac{J_5+\bar{J}_5}{2\sqrt{-(J_2^c+\bar{J}_2^c)(J_2^s+\bar{J}_2^s)} }\nonumber +} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + +\begin{frame}{Compatibility with SM} +{~} + + \begin{minipage}{\textwidth} + +\begin{columns} +\column{0.1in} +{~} +\column{2in} +\includegraphics[angle=-90,width=0.95\textwidth]{images/PBasis_P5pPad.pdf} + +\ARROW Use \texttt{EOS} software package to test compatibility with SM.\\ +\ARROW Perform the $\chi^2$ fit to the measured: +\begin{center} +\begin{align*} +F_L, A_{FB}, S_{3,..., 9} . +\end{align*} +\end{center} +\ARROW Float a vector coupling: $\Re(C_9)$.\\ + + +\column{3in} +\begin{align*} +\Delta \Re (C_9) \equiv \Re(C_9)^{{\rm fit}} - \Re(C_9)^{{\rm SM}} = -1.03 +\end{align*} +\includegraphics[angle=-90,width=0.95\textwidth]{images/wilsonchi2.pdf} \\ + +\ARROW Best fit is found to be $3.4~\sigma$ away from the SM. + +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}\frametitle{Global picture of $P_5^{\prime}$} + +\begin{columns} + +\column{0.4\textwidth} +\only<1>{{\color{gray}{\ARROW 2013 LHCb: \href{https://arxiv.org/pdf/1308.1707.pdf}{arXiv::1308.1707}}}\\} +\only<1>{\ARROW 2015 LHCb: \href{https://arxiv.org/abs/1512.04442}{arXiv::1512.0444}\\} +\only<1>{{\color{red}{\ARROW 2016 Belle: \href{https://arxiv.org/abs/1604.04042}{arXiv::1604.04042}}}\\} +\only<1>{\ARROW 2017: {\color{blue}{\href{https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2017-023/}{ATLAS-CONF-2017-023}}} $(20.5~\rm fb^{-1})$ and {\color{OliveGreen}{\href{http://cds.cern.ch/record/2256738?ln=en}{CMS-PAS-BPH-15-008}}} $(20.8~\rm fb^{-1})$} + + + +\column{0.6\textwidth} +\only<1>{ +\ARROW Theory: +~~DHMV: \href{https://arxiv.org/abs/1407.8526}{arXiv::1407.8526} +~~ASZB: \href{https://arxiv.org/abs/1411.3161}{arXiv::1411.3161} +} +%\includegraphics[width=0.95\textwidth]{images/P5p1.png} +\only<1>{ +\includegraphics[angle=-90,width=0.9\textwidth]{images/P5p.pdf} +} + + +\end{columns} +\only<1>{ + + +} + +\end{frame} + + + +\iffalse + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PLambdab \to \PLambda \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + + \begin{center} + \only<1>{ + \includegraphics[width=0.65\textwidth]{images/Lb_BR.png} +} + \only<2>{ + \includegraphics[width=0.45\textwidth]{images/Lblow.png} +\includegraphics[width=0.45\textwidth]{images/Lbhigh.png} + +} + + + \end{center} + + +\begin{itemize} +\item This years LHCb measurement [JHEP 06 (2015) 115]]. +\item In total $\sim 300$ candidates in data set. +\item Decay not present in the low $q^2$. + +\end{itemize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}{Angular analysis of $\PLambdab \to \PLambda \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item For the bins in which we have $>3~\sigma$ significance the forward backward asymmetry for the hadronic and leptonic system. +\end{itemize} +\begin{center} +\includegraphics[width=0.9\textwidth]{{images/AFB_Lb}.png} +\end{center} +\begin{itemize} +\item $A_{FB}^H$ is in good agreement with SM. +\item $A_{FB}^{\ell}$ always in above SM prediction. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Lepton universality test} +{~} + \begin{minipage}{\textwidth} +\begin{columns} +\column{3.0in} +\begin{itemize} +\item If $\PZprime$ is responsible for the $P'_5$ anomaly, does it couple equally to all flavours? +\includegraphics[width=0.9\textwidth]{images/uni2.png} +\item Challenging analysis due to bremsstrahlung. +\item Migration of events modeled by MC. +\item Correct for bremsstrahlung. +\item Take double ratio with $\PBplus \to \PJpsi \PKplus$ to cancel systematics. +\item In $3\invfb$, LHCb measures $R_K=0.745^{+0.090}_{-0.074}(stat.)^{+0.036}_{-0.036}(syst.)$ +\item Consistent with SM at $2.6\sigma$. + +\end{itemize} +\column{2.0in} +\includegraphics[width=0.99\textwidth]{images/RK.png}\\ +\begin{itemize} +\item \href{http://arxiv.org/abs/1406.6482}{Phys. Rev. Lett. 113, 151601 (2014)} +\end{itemize} +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Angular analysis of $\PBzero \to \PKstar \Pe \Pe$} +{~} +\only<1>{ + \begin{minipage}{\textwidth} + \begin{itemize} + \item With the full data set ($3\invfb$) we performed angular analysis in $0.0004 < q^2 <1~\GeV^2$. + \item Electrons channels are extremely challenging experimentally: + \begin{itemize} + \item Bremsstrahlung. + \item Trigger efficiencies. + \end{itemize} + \item Determine the angular observables: $\FL$, $\ATD$, $\ATRe$, $\ATIm$: + \end{itemize} +\begin{equation} + \label{eq:physPars} + \begin{split} + \FL &=\frac{|A_0|^2}{|A_0|^2+|A_{||}|^2 + |A_\perp|^2}\\ + \ATD &= \frac{|A_\perp|^2-|A_{||}|^2}{|A_\perp|^2+|A_{||}|^2}\\ + \ATRe &= \frac{2\Real(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}\\ + \ATIm &= \frac{2\Imag(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}, +\end{split}\nonumber +\end{equation} + +\end{minipage} +} +\only<2>{ +\begin{center} +\includegraphics[width=0.5\textwidth]{images/Kstee.png}\\ +\end{center} +\begin{itemize} +\item Results in full agreement with the SM. +\item Similar strength on $C_7$ Wilson coefficient as from $\Pbeauty \to \Pstrange \Pphoton$ decays. +\end{itemize} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/Kstee2.png} +\end{center} + +} + \vspace*{2.1cm} +\end{frame} + +\fi + +\begin{frame} +\begin{center} +\begin{Huge} +Global fit to $\Pbeauty \to \Pstrange \ell \ell$ measurements +\end{Huge} +\end{center} + + + + +\end{frame} + + + +\begin{frame}{Link the observables} +\begin{footnotesize} + +\ARROW Fits prepare by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}} + +\begin{itemize} + +\item Inclusive + +\begin{itemize} +\item $B\to X_s\gamma$ {\color{gray}($BR$) +.......................................................... } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} +\item $B\to X_s\ell^+\ell^-$ {\color{gray}($dBR/dq^2$) +............................................ } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} +\end{itemize} + +\item Exclusive leptonic + +\begin{itemize} +\item $B_s\to \ell^+\ell^-$ {\color{gray}($BR$) +........................................................ } {\color{red} $\C{10}^{(\prime)}$} +\end{itemize} + +\item Exclusive radiative/semileptonic +\begin{itemize} +\item $B\to K^*\gamma$ {\color{gray}($BR$, $S$, $A_I$) +................................................ } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $B\to K\ell^+\ell^-$ {\color{gray}($dBR/dq^2$) +.............................................. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $\bf \color{Red} B\to K^*\ell^+\ell^-$ {\color{gray}($dBR/dq^2$, {\bf Optimized Angular Obs.}) +.. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $B_s\to \phi \ell^+\ell^-$ {\color{gray}($dBR/dq^2$, Angular Observables) +.............. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $\Lambda_b\to \Lambda\ell^+\ell^-$ {\color{gray}(None so far)} +\item etc. +\end{itemize} + + + +\end{itemize} +\end{footnotesize} + +\end{frame} + +\frame{ \frametitle{Statistic details} + +\begin{footnotesize} + +\ARROW Frequentist approach: +\medskip + +$$\chi^2(C_i) = [O_\text{exp}- O_\text{th}(C_i)]_j \, [Cov^{-1}]_{jk}\, [O_\text{exp}- O_\text{th}(C_i)]_k$$ + + +\begin{itemize} +\item $\bf Cov = Cov^\text{exp} + Cov^\text{th}$. We have $Cov^\text{exp}$ for the first time +\item Calculate $Cov^\text{th}$: correlated multigaussian scan over all nuisance parameters +\item $Cov^\text{th}$ depends on $C_i$: Must check this dependence\\[5mm] +\end{itemize} +For the Fit: +\begin{itemize} +\item Minimise $\chi^2 \to \chi^2_\text{min} = \chi^2(C_i^0)\quad$ (Best Fit Point = $C_i^0$) +\item Confidence level regions: $\chi^2(C_i) - \chi^2_\text{min} < \Delta\chi_{\sigma,n}$ +%\item Compute pulls by inversion of the above formula +\end{itemize} +\medskip +\ARROW The results from 1D scans:{~}\\{~}\\ +\begin{tiny} +\begin{tabular}{crccc} +%\toprule[1.6pt] +Coefficient ${\cal C}_i^{NP}={\cal C}_i-{\cal C}_i^{SM}$ & Best fit & 1$\sigma$ & 3$\sigma$ & Pull$_{\rm SM}$ \\ \hspace{10mm} \\[5mm] +% \midrule + $\bf\cred\C9^{\rm NP}$ & $ -1.09 $ & $ [-1.29,-0.87] $ & $ [-1.67,-0.39] $ & $\,\,\,\,\,\,\bf 4.5 + \cred \Leftarrow$ \hspace{5mm} \\[3mm] + $\C9^{\rm NP}=-\C{10}^{\rm NP}$ & $ -0.68 $ & $ [-0.85,-0.50] $ & $ [-1.22,-0.18] $ & \bf \quad 4.2 + $\cred\Leftarrow$ \hspace{5mm} \\[3mm] + $\C9^{\rm NP}=-\C{9'}^{\rm NP}$ & $ -1.06 $ & $ [-1.25,-0.86] $ & $ [-1.60,-0.40] $ & \quad \quad \quad \,\,\quad 4.8 + $\cred\Leftarrow$ (no $R_K$)\hspace{5mm} \\[3mm] + + \hspace{5mm} \\[3mm] +% \bottomrule[1.6pt] +\end{tabular} +\end{tiny} +\end{footnotesize} + +} + + +\frame{ \frametitle{Where to look for more?} + +\begin{footnotesize} +\ARROW There are couple of models that can accommodate these (see next talk).\\ +\ARROW Usual models need high mass particle outside the reach of LHC.\\ + +\begin{exampleblock}{My opinion} +Before moving to high energy frontier to look for something we should explore more precisely the electroweak sector. + +We can get more clues about the underlying physics +\end{exampleblock} + +\begin{center} +\includegraphics[width=0.5\textwidth]{images/download.pdf} +\end{center} + + + + +\end{footnotesize} + +} + + + + + + + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} + + +\end{frame} + + + + + + + + +\begin{frame}{$B\to K^\ast \ell\ell\ $ Amplitudes} + +\small + +\mbox{ +\includegraphics[width=3cm,height=2cm]{bsg0.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2cm]{bsg1.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2.4cm]{bsg2.jpg} +} + +\vspace{3mm} + +\mbox{ +\hspace{-10mm} +\colorbox{llgray}{ +\hspace{1mm} +$\displaystyle +A_\lambda^{L,R} = N_\lambda\ \bigg\{ +(C_9 \mp C_{10}) {\blue \F_\lambda(q^2)} ++\frac{2m_b M_B}{q^2} \bigg[ C_7 {\blue \F_\lambda^{T}(q^2)} +- 16\pi^2 \frac{M_B}{m_b} {\red \H_\lambda(q^2)} \bigg] +\bigg\} +$ +\hspace{2mm} +} +} + +\vspace{5mm} +{\small + +\hspace{-8mm} \btr {\brown Local (Form Factors) :} \hspace{2mm} {\blue $ \F_\lambda^{(T)}(q^2) = \av{\bar M_\lambda(k)| \,\bar s\, \Gamma_\lambda^{(T)}\, b\, | \bar{ B}(k+q)}$} +\\[5mm] + +\mbox{ +\hspace{-9mm} +\btr {\brown Non-Local :} \hspace{0mm} {\red $\displaystyle \H_\lambda(q^2) = i \,{\cal P}_\mu^\lambda \int d^4 x\ e^{i q\cdot x}\, +\av{\bar{M}_\lambda(k)| +T\big\{ {\cal J}_{\rm em}^\mu(x), \C{i} \, \mathcal{O}(0) \big\} | \bar{B}(q+k)}$} +} + +\vspace{3mm} + +\hspace{-8mm} +\btr CKM structure : \hspace{2mm} $\displaystyle \H_\lambda = {\color{gray}- \frac{\lambda_u}{\lambda_t} \H_\lambda^{(u)}} - \frac{\lambda_c}{\lambda_t} \H_\lambda^{(c)}$ \hspace{5mm} $\Rightarrow\ \mathcal{O} \sim (\bar{ c} b)(\bar{ s} c)$ + +} + +\end{frame} + + + + + +\begin{frame}{Analytic structure of $\H_\lambda(q^2)$} + +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{3mm} + + +Neglecting OZI- and CKM-suppressed contributions : + +\begin{center} +\includegraphics[width=7.5cm]{Analyticq2.png} +\end{center} + + +$\displaystyle { \hat{\mathcal{H}}_\lambda(q^2)} = (q^2 - M_{J/\psi}^2)(q^2 -M_{\psi(2S)}^2) \,{ {\mathcal{H}}_\lambda(q^2)} \quad $ has no poles. + +\end{frame} + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} + +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{2mm} + +\btr Conformal mapping : \hspace{5mm} $q^2 \mapsto \ z\,(q^2) = \frac{\sqrt{t_+ - q^2} - \sqrt{t_+ - t_0}}{\sqrt{t_+ - q^2} + \sqrt{t_+ - t_0}}$ + +\mbox{ +\hspace{-10mm} +\raisebox{8mm}{\includegraphics[width=5.6cm]{Analyticq22.png}} +\hspace{1mm} +\includegraphics[width=6.5cm]{Analyticz.png} +} + +\vspace{-7mm} + +\btr ${\red \hat \H_\lambda (q^2(z))}$ is {\bf analytic in $|z|<1$}\\[3mm] + +\btr Taylor expand $\red \hat{\H}_\lambda(z)$ around $z=0$.\\[3mm] + +\btr Expansion needed for $|z| < 0.52\ $ ( $-7\,\GeV^2 \leq q^2 \leq 14 \GeV^2$ ) + + +\end{frame} + + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} + +\vspace{3mm} + + +\hspace{-5mm} {\bf \brown Some details for actual parametrisation :} + +\mbox{\hspace{-5mm} \btr Try to capture most features of the expansion (better convergence)} + +\mbox{\hspace{-5mm} \btr Parametrize the ratios $\H_\lambda(q^2)/\F_\lambda(q^2)$ instead} + +\mbox{\hspace{-5mm} \btr The poles should not modify the asymptotic behaviour at $|q^2|\to \infty$} + +\begin{eqnarray} +\H_\lambda(z) &=& +\frac{1-z\, z^*_{J/\psi}}{z-z_{J/\psi}} \frac{1-z\,z^*_{\psi(2S)}}{z-z_{\psi(2S)}} \ \hat\H_\lambda(z) +\nonumber\\[2mm] +% +\hat\H_\lambda(z) &=& \Big[ \sum_{k=0}^K \alpha_k^{(\lambda)} z^{k} \Big] \F_\lambda(z) +\nonumber +\end{eqnarray} + + +where $\alpha^{(\lambda)}_k$ are complex coefficients, and the expansion is truncated after the term $z^{K}$. +We will take $K=2$ ({\brown 16} real parameters). + + +\end{frame} + + + + +\begin{frame}{Experimental constraints on $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown Experimental constraints :} + +\mbox{\hspace{-5mm} \btr The residues of the poles are given by $B\to K^* \psi_n$ :} + +$$ +\H_\lambda(q^2 \to M_{\psi_n}^2) \sim +\frac{M_{\psi_n} f^{\,*}_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2 (q^2 - M_{\psi_n}^2)} + \cdots +$$ + +\mbox{\hspace{-5mm} \btr Angular analyses \Cite{Belle, Babar, LHCb} determine : } + +$$ +|r_\perp^{\psi_n}|,\, +|r_\|^{\psi_n}|,\, +|r_0^{\psi_n}|,\, +\arg\{r_\perp^{\psi_n} r_{0}^{\psi_n*}\},\, +\arg\{r_\|^{\psi_n} r_{0}^{\psi_n*}\}, +$$ + +where $\quad \displaystyle r_\lambda^{\psi_n} \equiv \operatorname*{Res}_{q^2\to M^2_{\psi_n}} \frac{\H_\lambda(q^2)}{\F_\lambda(q^2)} +\sim +\frac{M_{\psi_n} f^*_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2\, \F_\lambda(M_{\psi_n}^2)}$\\[3mm] + + +\mbox{\hspace{-5mm} \btr We produce correlated pseudo-observables from a fit (5+5).} + + + +\end{frame} + + + + +\begin{frame}{Prior Fit to $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown (Prior) Fit to Experimental and theoretical pseudo-observables :} + + + +\begin{table}[b] +% \resizebox{.85\textwidth}{!}{% +\centering +\renewcommand{\arraystretch}{1.5} +\renewcommand{\tabcolsep}{3.1mm} +\begin{tabular}{@{}crrr@{}} +\hline +$k$ & 0\hspace{7mm} & 1\hspace{7mm} & 2\hspace{7mm} \\ +\hline +%re perp +${\rm Re}[\alpha_{k}^{(\perp)}]$ & $-0.06 \pm 0.21$ & $-6.77 \pm 0.27$ & $18.96 \pm 0.59$ \\ +%re para +${\rm Re}[\alpha_{k}^{(\parallel)}]$ & $-0.35 \pm 0.62$ & $-3.13 \pm 0.41$ & $12.20 \pm 1.34$ \\ +%re long +${\rm Re}[\alpha_{k}^{(0)}]$ & $0.05 \pm 1.52$ & $17.26 \pm 1.64$ & -- \\ +%im perp +${\rm Im}[\alpha_{k}^{(\perp)}]$ & $-0.21 \pm 2.25$ & $1.17 \pm 3.58$ & $-0.08 \pm 2.24$ \\ +%im para +${\rm Im}[\alpha_{k}^{(\parallel)}]$ & $-0.04 \pm 3.67$ & $-2.14 \pm 2.46$ & $6.03 \pm 2.50$ \\ +%im long +${\rm Im}[\alpha_{k}^{(0)}]$ & $-0.05 \pm 4.99$ & $4.29 \pm 3.14$ & -- \\ +\hline +\end{tabular} +% } +\caption{Mean values and standard deviations (in units of $10^{-4}$) +of the prior PDF for the parameters $\alpha_k^{(\lambda)}$.} +\label{alphak} +\end{table} + +\end{frame} + +\begin{frame}{New Physics Analysis } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown SM predictions and Fit including $B\to K^* \mu^+\mu^-$ data and $\C{9}^{\rm NP}$ :}\\[4mm] + +\mbox{ +\hspace{-10mm} +\includegraphics[width=12cm]{NPFit.png} +} + +The NP hypothesis with {\red $\C{9}^{\bf NP}\sim -1$} is favored strongly in the global fit + +\end{frame} + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Scale of NP?} +{~} + \begin{minipage}{\textwidth} +\includegraphics[width=0.99\textwidth]{15.png} + +\ARROW Stolen from M. Nardecchia +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Conclusions} +{~} + \begin{minipage}{\textwidth} +\begin{itemize} +\item Clear tensions wrt. SM predictions! +\item Measurements cluster in the same direction. +\item We are not opening the champagne yet! +\item Still need improvement both on theory and experimental side. +\item Time will tell if this is QCD+fluctuations or new Physics: +\end{itemize} +\pause +''... when you have eliminated all the\\ +Standard Model explanations, whatever remains,\\ +however improbable, must be New Physics.''\\ +prof. Joaquim Matias + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +{~} + \begin{minipage}{\textwidth} +\begin{center} +\begin{LARGE} +Thank you for the attention! +\end{LARGE} +\includegraphics[width=0.8\textwidth]{images/Joke.jpg} + +\end{center} + + + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Amplitudes method} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + +\ARROW Fit for amplitudes as (continuous) functions of $q^2$ in the region: $q^2 \in \left[ 1.1. 6.0 \right]~\GeV^2/c^4$.\\ +\ARROW Needs some Ansatz: +\begin{align*} +A(q^2) = \alpha + \beta q^2+ \dfrac{\gamma}{q^2} +\end{align*} +\ARROW The assumption is tested extensively with toys.\\ +\ARROW Set of 3 complex parameters $ \alpha, \beta, \gamma $ per vector amplitude:\begin{itemize} +\item {\color{Magenta}{$L, ~R$}}, {\color{Cerulean}{$0 ,~\| ,~\bot$}}, {\color{PineGreen}{$\Re ,~\Im$}} $\rightarrowtail$~~ $3 \times {\color{PineGreen}{2}} \times {\color{Cerulean}{3}} \times {\color{Magenta}{2}} = 36$ DoF. +\item Scalar amplitudes: $+4$ DoF. +\item Symmetries of the amplitudes reduces the total budget to: $28$. +\end{itemize} +\ARROW The technique is described in \href{http://arxiv.org/pdf/1504.00574v2.pdf}{\color{blue}{JHEP06(2015)084}}.\\ +\ARROW Allows to build the observables as continuous functions of $q^2$: +\begin{itemize} +\item At current point the method is limited by statistics. +\item In the future the power of this method will increase. +\end{itemize} +\ARROW Allows to measure the zero-crossing points for free and with smaller errors than previous methods. +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Amplitudes - results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} +\begin{center} +\begin{columns} +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_AFBOverlay}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S4Overlay}.pdf} + +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S5Overlay}.pdf}\\ +{~}\\{~}\\{~}\\{~}\\ +\begin{large} +Zero crossing points: +\end{large} +\begin{align*} +q_0(S_4) & <2.65 & {\rm{~at~}} & 95\% ~CL \\ +q_0(S_5) & \in \left[ 2.49,3.95 \right] & {\rm{~at~}} & 68\% ~CL \\ +q_0(A_{FB}) & \in \left[ 3.40, 4.87 \right] & {\rm{~at~}} & 68\% ~CL +\end{align*} + + +\end{columns} +\end{center} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\backupend + +\end{document} diff --git a/KIT_2018/mchrzasz.toc b/KIT_2018/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/KIT_2018/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/KIT_2018/tikzfeynman.sty b/KIT_2018/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/KIT_2018/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Kstarmumu_Run2/Overlaps/Makefile b/Kstarmumu_Run2/Overlaps/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Kstarmumu_Run2/Overlaps/beamercolorthemeFlip.sty b/Kstarmumu_Run2/Overlaps/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Kstarmumu_Run2/Overlaps/beamerinnerthemeFlip.sty b/Kstarmumu_Run2/Overlaps/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Kstarmumu_Run2/Overlaps/beamerouterthemeFlip.sty b/Kstarmumu_Run2/Overlaps/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Kstarmumu_Run2/Overlaps/beamerouterthemedecolines.sty b/Kstarmumu_Run2/Overlaps/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Kstarmumu_Run2/Overlaps/beamerthemeFlip.sty b/Kstarmumu_Run2/Overlaps/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Kstarmumu_Run2/Overlaps/images/.DS_Store b/Kstarmumu_Run2/Overlaps/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/.DS_Store Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/B0_DiraAngle.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/B0_DiraAngle.pdf new file mode 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b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/J_psi_M.pdf new file mode 100644 index 0000000..f4c9ea2 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/J_psi_M.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..1c5c6f9 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_P.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_P.pdf new file mode 100644 index 0000000..f651416 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PIDK.pdf new file mode 100644 index 0000000..c837135 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PIDK.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PIDmu.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PIDmu.pdf new file mode 100644 index 0000000..b6052a8 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PIDmu.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PIDp.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PIDp.pdf new file mode 100644 index 0000000..158bfcf --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PIDp.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PT.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PT.pdf new file mode 100644 index 0000000..bc77fda --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/K_PT.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Kstar_M.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Kstar_M.pdf new file mode 100644 index 0000000..9749eab --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Kstar_M.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/NEW.root b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/NEW.root new file mode 100644 index 0000000..08dafbf --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/NEW.root Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/OLD.root b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/OLD.root new file mode 100644 index 0000000..dfab327 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/OLD.root Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..4a89bf9 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_P.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_P.pdf new file mode 100644 index 0000000..012fd0c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PIDK.pdf new file mode 100644 index 0000000..207c260 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PIDK.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PIDmu.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PIDmu.pdf new file mode 100644 index 0000000..a2f582e --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PIDmu.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PIDp.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PIDp.pdf new file mode 100644 index 0000000..31ea568 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PIDp.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PT.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PT.pdf new file mode 100644 index 0000000..aab6600 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/Pi_PT.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/compare.cc b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/compare.cc new file mode 100644 index 0000000..6b8180d --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/compare.cc @@ -0,0 +1,104 @@ +void compare() +{ + + gROOT->ProcessLine(".L lhcbStyle.C"); + + TCanvas *c1= new TCanvas("c1", "c1", 800,600); + + TChain *ch_S21= new TChain(); + TChain *ch_S21_unique= new TChain(); + TChain *ch_S20_unique= new TChain(); + + ch_S21->Add("/storage4/ntuples/lhcb/KstarMuMu/data_reduced/Run1/Kstarmumu_Data_Run1.root/Reduced"); + ch_S21_unique->Add("NEW.root/NEW"); + ch_S20_unique->Add("OLD.root/OLD"); + + + TString cutnew= "B0_M>5370 && B0_M<5700 && Kstar_M>795.9 && Kstar_M < 995.9 && K_TRACK_GhostProb<0.4 && Pi_TRACK_GhostProb<0.4 && mu_plus_TRACK_GhostProb<0.4 && mu_minus_TRACK_GhostProb<0.4 && (!((B0_ID>0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID<0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID>0)&&(B0_kmuswapMass>3626)&&(B0_kmuswapMass<3746)&&(K_PIDmu>5||K_isMuon==1)))" ; + TString fiducial_new="q2>0.1 && q2<19. && !( J_psi_M>3626 && J_psi_M <3746.) && !( J_psi_M>3037 && J_psi_M <3157. )"; + + + + TString cut = cutnew + "&&"+fiducial_new; + + vector variables={"B0_M", "Kstar_M", "J_psi_M", "B0_DiraAngle", "B0_ENDVERTEX_CHI2", "B0_IP_OWNPV", "B0_IPCHI2_OWNPV", "B0_P", "B0_PT", + "K_IPCHI2_OWNPV", "K_P", "K_PT", "K_PIDmu", "K_PIDK", "K_PIDp", + "Pi_IPCHI2_OWNPV", "Pi_P", "Pi_PT", "Pi_PIDmu", "Pi_PIDK", "Pi_PIDp", + "mu_plus_IPCHI2_OWNPV", "mu_plus_P", "mu_plus_PT", "mu_plus_PIDmu", "mu_plus_PIDK", "mu_plus_PIDp", + "mu_minus_IPCHI2_OWNPV", "mu_minus_P", "mu_minus_PT", "mu_minus_PIDmu", "mu_minus_PIDK", "mu_minus_PIDp" }; + + + + vector range={ "(100,5060,6000)", "(100,795.9, 995.9)","(100,100,4000)", "(100,0,0.014)", "(100,0,30)", "(100,0,0.12)", "(100,0., 16.)", "(100,10000, 300000)", "(100,100, 30000)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-5,80)", "(100,-40,50)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-80,20)", "(100,-80,20)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)", + "(100,0,200)","(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)"}; + + + if(variables.size() != range.size()) + { + cout<<"Wrong number of arguments!"<< variables.size()<<" "<< range.size()<Draw(variables[i]+">>"+variables[i]+range[i], cut); + ch_S21_unique->Draw(variables[i]+">>"+variables[i]+"1"+range[i]); + ch_S20_unique->Draw(variables[i]+">>"+variables[i]+"2"+range[i]); + + TH1D* hist= (TH1D*)gROOT->FindObject(variables[i]); + TH1D* hist1= (TH1D*)gROOT->FindObject(variables[i] +"1"); + TH1D* hist2= (TH1D*)gROOT->FindObject(variables[i]+"2"); + + hist->SetFillColor(0); + hist1->SetFillColor(0); + hist2->SetFillColor(0); + + hist->SetLineColor(kRed); + hist1->SetLineColor(kBlue+2); + hist2->SetLineColor(kGreen+2); + + + hist->GetXaxis()->SetTitle(variables[i]); + hist1->GetXaxis()->SetTitle(variables[i]); + hist2->GetXaxis()->SetTitle(variables[i]); + + hist->SetMaximum(hist->GetMaximum()*1.5); + hist1->SetMaximum(hist1->GetMaximum()*1.5); + hist2->SetMaximum(hist2->GetMaximum()*1.5); + + + hist->DrawNormalized(); + hist1->DrawNormalized("SAME"); + hist2->DrawNormalized("SAME"); + + + //if(i==0) + // { + TLegend *leg= new TLegend(0.6, 0.8, 0.9, 0.9); + leg->AddEntry(hist, "S21", "f"); + leg->AddEntry(hist1, "Unique in S21" ,"f"); + leg->AddEntry(hist2, "Unique in S20" ,"f"); + + leg->Draw(); + + // } + + c1->SaveAs(variables[i]+".pdf"); + + } + + + + + + + + + + + +} diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/compare.cc~ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/compare.cc~ new file mode 100644 index 0000000..1c68936 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/compare.cc~ @@ -0,0 +1,104 @@ +void compare() +{ + + gROOT->ProcessLine(".L lhcbStyle.C"); + + TCanvas *c1= new TCanvas("c1", "c1", 800,600); + + TChain *ch_S21= new TChain(); + TChain *ch_S21_unique= new TChain(); + TChain *ch_S20_unique= new TChain(); + + ch_S21->Add("/storage4/ntuples/lhcb/KstarMuMu/data_reduced/Run1/Kstarmumu_Data_Run1.root/Reduced"); + ch_S21_unique->Add("NEW.root/NEW"); + ch_S20_unique->Add("OLD.root/OLD"); + + + TString cutnew= "B0_M>5050 && B0_M<5700 && Kstar_M>795.9 && Kstar_M < 995.9 && K_TRACK_GhostProb<0.4 && Pi_TRACK_GhostProb<0.4 && mu_plus_TRACK_GhostProb<0.4 && mu_minus_TRACK_GhostProb<0.4 && (!((B0_ID>0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID<0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID>0)&&(B0_kmuswapMass>3626)&&(B0_kmuswapMass<3746)&&(K_PIDmu>5||K_isMuon==1)))" ; + TString fiducial_new="q2>0.1 && q2<19. && !( J_psi_M>3626 && J_psi_M <3746.) && !( J_psi_M>3037 && J_psi_M <3157. )"; + + + + TString cut = cutnew + "&&"+fiducial_new; + + vector variables={"B0_M", "Kstar_M", "J_psi_M", "B0_DiraAngle", "B0_ENDVERTEX_CHI2", "B0_IP_OWNPV", "B0_IPCHI2_OWNPV", "B0_P", "B0_PT", + "K_IPCHI2_OWNPV", "K_P", "K_PT", "K_PIDmu", "K_PIDK", "K_PIDp", + "Pi_IPCHI2_OWNPV", "Pi_P", "Pi_PT", "Pi_PIDmu", "Pi_PIDK", "Pi_PIDp", + "mu_plus_IPCHI2_OWNPV", "mu_plus_P", "mu_plus_PT", "mu_plus_PIDmu", "mu_plus_PIDK", "mu_plus_PIDp", + "mu_minus_IPCHI2_OWNPV", "mu_minus_P", "mu_minus_PT", "mu_minus_PIDmu", "mu_minus_PIDK", "mu_minus_PIDp" }; + + + + vector range={ "(100,5060,6000)", "(100,795.9, 995.9)","(100,100,4000)", "(100,0,0.014)", "(100,0,30)", "(100,0,0.12)", "(100,0., 16.)", "(100,10000, 300000)", "(100,100, 30000)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-5,80)", "(100,-40,50)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-80,20)", "(100,-80,20)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)", + "(100,0,200)","(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)"}; + + + if(variables.size() != range.size()) + { + cout<<"Wrong number of arguments!"<< variables.size()<<" "<< range.size()<Draw(variables[i]+">>"+variables[i]+range[i], cut); + ch_S21_unique->Draw(variables[i]+">>"+variables[i]+"1"+range[i]); + ch_S20_unique->Draw(variables[i]+">>"+variables[i]+"2"+range[i]); + + TH1D* hist= (TH1D*)gROOT->FindObject(variables[i]); + TH1D* hist1= (TH1D*)gROOT->FindObject(variables[i] +"1"); + TH1D* hist2= (TH1D*)gROOT->FindObject(variables[i]+"2"); + + hist->SetFillColor(0); + hist1->SetFillColor(0); + hist2->SetFillColor(0); + + hist->SetLineColor(kRed); + hist1->SetLineColor(kBlue+2); + hist2->SetLineColor(kGreen+2); + + + hist->GetXaxis()->SetTitle(variables[i]); + hist1->GetXaxis()->SetTitle(variables[i]); + hist2->GetXaxis()->SetTitle(variables[i]); + + hist->SetMaximum(hist->GetMaximum()*1.5); + hist1->SetMaximum(hist1->GetMaximum()*1.5); + hist2->SetMaximum(hist2->GetMaximum()*1.5); + + + hist->DrawNormalized(); + hist1->DrawNormalized("SAME"); + hist2->DrawNormalized("SAME"); + + + //if(i==0) + // { + TLegend *leg= new TLegend(0.6, 0.8, 0.9, 0.9); + leg->AddEntry(hist, "S21", "f"); + leg->AddEntry(hist1, "Unique in S21" ,"f"); + leg->AddEntry(hist2, "Unique in S20" ,"f"); + + leg->Draw(); + + // } + + c1->SaveAs(variables[i]+".pdf"); + + } + + + + + + + + + + + +} diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/lhcbStyle.C b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/lhcbStyle.C new file mode 100644 index 0000000..5d8a70c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/lhcbStyle.C @@ -0,0 +1,196 @@ +// all users - please change the name of this file to lhcbStyle.C +// Commits to lhcbdocs svn of .C files are not allowed +{ + + // define names for colours + Int_t black = 1; + Int_t red = 2; + Int_t green = 3; + Int_t blue = 4; + Int_t yellow = 5; + Int_t magenta= 6; + Int_t cyan = 7; + Int_t purple = 9; + + +//////////////////////////////////////////////////////////////////// +// PURPOSE: +// +// This macro defines a standard style for (black-and-white) +// "publication quality" LHCb ROOT plots. +// +// USAGE: +// +// Include the lines +// gROOT->ProcessLine(".L lhcbstyle.C"); +// lhcbStyle(); +// at the beginning of your root macro. +// +// Example usage is given in myPlot.C +// +// COMMENTS: +// +// Font: +// +// The font is chosen to be 132, this is Times New Roman (like the text of +// your document) with precision 2. +// +// "Landscape histograms": +// +// The style here is designed for more or less square plots. +// For longer histograms, or canvas with many pads, adjustements are needed. +// For instance, for a canvas with 1x5 histograms: +// TCanvas* c1 = new TCanvas("c1", "L0 muons", 600, 800); +// c1->Divide(1,5); +// Adaptions like the following will be needed: +// gStyle->SetTickLength(0.05,"x"); +// gStyle->SetTickLength(0.01,"y"); +// gStyle->SetLabelSize(0.15,"x"); +// gStyle->SetLabelSize(0.1,"y"); +// gStyle->SetStatW(0.15); +// gStyle->SetStatH(0.5); +// +// Authors: Thomas Schietinger, Andrew Powell, Chris Parkes, Niels Tuning +// Maintained by Editorial board member (currently Niels) +/////////////////////////////////////////////////////////////////// + + // Use times new roman, precision 2 + Int_t lhcbFont = 132; // Old LHCb style: 62; + // Line thickness + Double_t lhcbWidth = 2.00; // Old LHCb style: 3.00; + // Text size + Double_t lhcbTSize = 0.06; + + // use plain black on white colors + gROOT->SetStyle("Plain"); + TStyle *lhcbStyle= new TStyle("lhcbStyle","LHCb plots style"); + + //lhcbStyle->SetErrorX(0); // don't suppress the error bar along X + + lhcbStyle->SetFillColor(1); + lhcbStyle->SetFillStyle(1001); // solid + lhcbStyle->SetFrameFillColor(0); + lhcbStyle->SetFrameBorderMode(0); + lhcbStyle->SetPadBorderMode(0); + lhcbStyle->SetPadColor(0); + lhcbStyle->SetCanvasBorderMode(0); + lhcbStyle->SetCanvasColor(0); + lhcbStyle->SetStatColor(0); + lhcbStyle->SetLegendBorderSize(0); + lhcbStyle->SetLegendFont(132); + + // If you want the usual gradient palette (blue -> red) + lhcbStyle->SetPalette(1); + // If you want colors that correspond to gray scale in black and white: + int colors[8] = {0,5,7,3,6,2,4,1}; + lhcbStyle->SetPalette(8,colors); + + // set the paper & margin sizes + lhcbStyle->SetPaperSize(20,26); + lhcbStyle->SetPadTopMargin(0.05); + lhcbStyle->SetPadRightMargin(0.05); // increase for colz plots + lhcbStyle->SetPadBottomMargin(0.16); + lhcbStyle->SetPadLeftMargin(0.14); + + // use large fonts + lhcbStyle->SetTextFont(lhcbFont); + lhcbStyle->SetTextSize(lhcbTSize); + lhcbStyle->SetLabelFont(lhcbFont,"x"); + lhcbStyle->SetLabelFont(lhcbFont,"y"); + lhcbStyle->SetLabelFont(lhcbFont,"z"); + lhcbStyle->SetLabelSize(lhcbTSize,"x"); + lhcbStyle->SetLabelSize(lhcbTSize,"y"); + lhcbStyle->SetLabelSize(lhcbTSize,"z"); + lhcbStyle->SetTitleFont(lhcbFont); + lhcbStyle->SetTitleFont(lhcbFont,"x"); + lhcbStyle->SetTitleFont(lhcbFont,"y"); + lhcbStyle->SetTitleFont(lhcbFont,"z"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"x"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"y"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"z"); + + // use medium bold lines and thick markers + lhcbStyle->SetLineWidth(lhcbWidth); + lhcbStyle->SetFrameLineWidth(lhcbWidth); + lhcbStyle->SetHistLineWidth(lhcbWidth); + lhcbStyle->SetFuncWidth(lhcbWidth); + lhcbStyle->SetGridWidth(lhcbWidth); + lhcbStyle->SetLineStyleString(2,"[12 12]"); // postscript dashes + lhcbStyle->SetMarkerStyle(20); + lhcbStyle->SetMarkerSize(1.0); + + // label offsets + lhcbStyle->SetLabelOffset(0.010,"X"); + lhcbStyle->SetLabelOffset(0.010,"Y"); + + // by default, do not display histogram decorations: + lhcbStyle->SetOptStat(0); + //lhcbStyle->SetOptStat("emr"); // show only nent -e , mean - m , rms -r + // full opts at http://root.cern.ch/root/html/TStyle.html#TStyle:SetOptStat + lhcbStyle->SetStatFormat("6.3g"); // specified as c printf options + lhcbStyle->SetOptTitle(0); + lhcbStyle->SetOptFit(0); + //lhcbStyle->SetOptFit(1011); // order is probability, Chi2, errors, parameters + //titles + lhcbStyle->SetTitleOffset(0.95,"X"); + lhcbStyle->SetTitleOffset(0.95,"Y"); + lhcbStyle->SetTitleOffset(1.2,"Z"); + lhcbStyle->SetTitleFillColor(0); + lhcbStyle->SetTitleStyle(0); + lhcbStyle->SetTitleBorderSize(0); + lhcbStyle->SetTitleFont(lhcbFont,"title"); + lhcbStyle->SetTitleX(0.0); + lhcbStyle->SetTitleY(1.0); + lhcbStyle->SetTitleW(1.0); + lhcbStyle->SetTitleH(0.05); + + // look of the statistics box: + lhcbStyle->SetStatBorderSize(0); + lhcbStyle->SetStatFont(lhcbFont); + lhcbStyle->SetStatFontSize(0.05); + lhcbStyle->SetStatX(0.9); + lhcbStyle->SetStatY(0.9); + lhcbStyle->SetStatW(0.25); + lhcbStyle->SetStatH(0.15); + + // put tick marks on top and RHS of plots + lhcbStyle->SetPadTickX(1); + lhcbStyle->SetPadTickY(1); + + // histogram divisions: only 5 in x to avoid label overlaps + lhcbStyle->SetNdivisions(505,"x"); + lhcbStyle->SetNdivisions(510,"y"); + + gROOT->SetStyle("lhcbStyle"); + gROOT->ForceStyle(); + + // add LHCb label + TPaveText* lhcbName = new TPaveText(gStyle->GetPadLeftMargin() + 0.05, + 0.87 - gStyle->GetPadTopMargin(), + gStyle->GetPadLeftMargin() + 0.20, + 0.95 - gStyle->GetPadTopMargin(), + "BRNDC"); + lhcbName->AddText("LHCb"); + lhcbName->SetFillColor(0); + lhcbName->SetTextAlign(12); + lhcbName->SetBorderSize(0); + + TText *lhcbLabel = new TText(); + lhcbLabel->SetTextFont(lhcbFont); + lhcbLabel->SetTextColor(1); + lhcbLabel->SetTextSize(lhcbTSize); + lhcbLabel->SetTextAlign(12); + + TLatex *lhcbLatex = new TLatex(); + lhcbLatex->SetTextFont(lhcbFont); + lhcbLatex->SetTextColor(1); + lhcbLatex->SetTextSize(lhcbTSize); + lhcbLatex->SetTextAlign(12); + + cout << "-------------------------" << endl; + cout << "Set LHCb Style - Feb 2012" << endl; + cout << "-------------------------" << endl; + +} + + diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/log b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/log new file mode 100644 index 0000000..1a9de86 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/log @@ -0,0 +1,16 @@ +OLD: + +Processing 18156 events from 18158 +Processing 18157 events from 18158 +Processing 18158 events from 18158 +Finished filling ntuple 31.2662627697 sec +Finished writing ntuple 31.281359911 sec + + +NEW: + +Processing 18221 events from 18223 +Processing 18222 events from 18223 +Processing 18223 events from 18223 +Finished filling ntuple 32.35283494 sec +Finished writing ntuple 32.3865230083 sec diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/log~ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/log~ new file mode 100644 index 0000000..5c7bde5 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/log~ @@ -0,0 +1,7 @@ +OLD: + +Processing 18156 events from 18158 +Processing 18157 events from 18158 +Processing 18158 events from 18158 +Finished filling ntuple 31.2662627697 sec +Finished writing ntuple 31.281359911 sec diff --git a/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/mu_minus_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/mu_minus_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..de79c2c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/BACKGROUNDREGION/mu_minus_IPCHI2_OWNPV.pdf Binary files differ diff --git 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b/Kstarmumu_Run2/Overlaps/images/B_PT.png new file mode 100644 index 0000000..1097473 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/B_PT.png Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_DiraAngle.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_DiraAngle.pdf new file mode 100644 index 0000000..6d811c2 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_DiraAngle.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_ENDVERTEX_CHI2.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_ENDVERTEX_CHI2.pdf new file mode 100644 index 0000000..5e0db82 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_ENDVERTEX_CHI2.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..7cb9063 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_IP_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_IP_OWNPV.pdf new file mode 100644 index 0000000..f74f02c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_IP_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_M.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_M.pdf new file mode 100644 index 0000000..215e5ae --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_M.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_P.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_P.pdf new file mode 100644 index 0000000..b00cce7 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_PT.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_PT.pdf new file mode 100644 index 0000000..d07a60c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/B0_PT.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/J_psi_M.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/J_psi_M.pdf new file mode 100644 index 0000000..cf22342 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/J_psi_M.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/K_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/K_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..fda53d4 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/K_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/K_P.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/K_P.pdf new file mode 100644 index 0000000..40cba8c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/K_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/K_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/K_PIDK.pdf new file mode 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b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Kstar_M.pdf new file mode 100644 index 0000000..7084c63 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Kstar_M.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/NEW.root b/Kstarmumu_Run2/Overlaps/images/FULLREGION/NEW.root new file mode 100644 index 0000000..88c16f2 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/NEW.root Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/OLD.root b/Kstarmumu_Run2/Overlaps/images/FULLREGION/OLD.root new file mode 100644 index 0000000..e1361f2 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/OLD.root Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..b9a8282 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_P.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_P.pdf new file mode 100644 index 0000000..1151e2a --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PIDK.pdf new file mode 100644 index 0000000..a09006e --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PIDK.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PIDmu.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PIDmu.pdf new file mode 100644 index 0000000..016c7d5 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PIDmu.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PIDp.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PIDp.pdf new file mode 100644 index 0000000..ffc776e --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PIDp.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PT.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PT.pdf new file mode 100644 index 0000000..073af3a --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/Pi_PT.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/compare.cc b/Kstarmumu_Run2/Overlaps/images/FULLREGION/compare.cc new file mode 100644 index 0000000..a9c705b --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/compare.cc @@ -0,0 +1,103 @@ +void compare() +{ + + gROOT->ProcessLine(".L lhcbStyle.C"); + + TCanvas *c1= new TCanvas("c1", "c1", 800,600); + + TChain *ch_S21= new TChain(); + TChain *ch_S21_unique= new TChain(); + TChain *ch_S20_unique= new TChain(); + + ch_S21->Add("/storage4/ntuples/lhcb/KstarMuMu/data_reduced/Run1/Kstarmumu_Data_Run1.root/Reduced"); + ch_S21_unique->Add("NEW.root/NEW"); + ch_S20_unique->Add("OLD.root/OLD"); + + + TString cutnew= "B0_M>5050 && B0_M<5700 && Kstar_M>795.9 && Kstar_M < 995.9 && K_TRACK_GhostProb<0.4 && Pi_TRACK_GhostProb<0.4 && mu_plus_TRACK_GhostProb<0.4 && mu_minus_TRACK_GhostProb<0.4 && (!((B0_ID>0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID<0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID>0)&&(B0_kmuswapMass>3626)&&(B0_kmuswapMass<3746)&&(K_PIDmu>5||K_isMuon==1)))" ; + TString fiducial_new="q2>0.1 & q2<19"; + + + TString cut = cutnew + "&&"+fiducial_new; + + vector variables={"B0_M", "Kstar_M", "J_psi_M", "B0_DiraAngle", "B0_ENDVERTEX_CHI2", "B0_IP_OWNPV", "B0_IPCHI2_OWNPV", "B0_P", "B0_PT", + "K_IPCHI2_OWNPV", "K_P", "K_PT", "K_PIDmu", "K_PIDK", "K_PIDp", + "Pi_IPCHI2_OWNPV", "Pi_P", "Pi_PT", "Pi_PIDmu", "Pi_PIDK", "Pi_PIDp", + "mu_plus_IPCHI2_OWNPV", "mu_plus_P", "mu_plus_PT", "mu_plus_PIDmu", "mu_plus_PIDK", "mu_plus_PIDp", + "mu_minus_IPCHI2_OWNPV", "mu_minus_P", "mu_minus_PT", "mu_minus_PIDmu", "mu_minus_PIDK", "mu_minus_PIDp" }; + + + + vector range={ "(100,5060,6000)", "(100,795.9, 995.9)","(100,100,4000)", "(100,0,0.014)", "(100,0,30)", "(100,0,0.12)", "(100,0., 16.)", "(100,10000, 300000)", "(100,100, 30000)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-5,80)", "(100,-40,50)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-80,20)", "(100,-80,20)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)", + "(100,0,200)","(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)"}; + + + if(variables.size() != range.size()) + { + cout<<"Wrong number of arguments!"<< variables.size()<<" "<< range.size()<Draw(variables[i]+">>"+variables[i]+range[i], cut); + ch_S21_unique->Draw(variables[i]+">>"+variables[i]+"1"+range[i]); + ch_S20_unique->Draw(variables[i]+">>"+variables[i]+"2"+range[i]); + + TH1D* hist= (TH1D*)gROOT->FindObject(variables[i]); + TH1D* hist1= (TH1D*)gROOT->FindObject(variables[i] +"1"); + TH1D* hist2= (TH1D*)gROOT->FindObject(variables[i]+"2"); + + hist->SetFillColor(0); + hist1->SetFillColor(0); + hist2->SetFillColor(0); + + hist->SetLineColor(kRed); + hist1->SetLineColor(kBlue+2); + hist2->SetLineColor(kGreen+2); + + + hist->GetXaxis()->SetTitle(variables[i]); + hist1->GetXaxis()->SetTitle(variables[i]); + hist2->GetXaxis()->SetTitle(variables[i]); + + hist->SetMaximum(hist->GetMaximum()*1.5); + hist1->SetMaximum(hist1->GetMaximum()*1.5); + hist2->SetMaximum(hist2->GetMaximum()*1.5); + + + hist->DrawNormalized(); + hist1->DrawNormalized("SAME"); + hist2->DrawNormalized("SAME"); + + + //if(i==0) + // { + TLegend *leg= new TLegend(0.6, 0.8, 0.9, 0.9); + leg->AddEntry(hist, "S21", "f"); + leg->AddEntry(hist1, "Unique in S21" ,"f"); + leg->AddEntry(hist2, "Unique in S20" ,"f"); + + leg->Draw(); + + // } + + c1->SaveAs(variables[i]+".pdf"); + + } + + + + + + + + + + + +} diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/compare.cc~ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/compare.cc~ new file mode 100644 index 0000000..3240e33 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/compare.cc~ @@ -0,0 +1,103 @@ +void compare() +{ + + gROOT->ProcessLine(".L lhcbStyle.C"); + + TCanvas *c1= new TCanvas("c1", "c1", 800,600); + + TChain *ch_S21_full= new TChain(); + TChain *ch_S21_unique= new TChain(); + TChain *ch_S20_unique= new TChain(); + + ch_S21->Add("/storage4/ntuples/lhcb/KstarMuMu/data_reduced/Run1/Kstarmumu_Data_Run1.root/Reduced"); + ch_S21_unique->Add("NEW.root/NEW"); + ch_S20_unique->Add("OLD.root/OLD"); + + + TString cutnew= "B0_M>5050 && B0_M<5700 && Kstar_M>795.9 && Kstar_M < 995.9 && K_TRACK_GhostProb<0.4 && Pi_TRACK_GhostProb<0.4 && mu_plus_TRACK_GhostProb<0.4 && mu_minus_TRACK_GhostProb<0.4 && (!((B0_ID>0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID<0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID>0)&&(B0_kmuswapMass>3626)&&(B0_kmuswapMass<3746)&&(K_PIDmu>5||K_isMuon==1)))" ; + TString fiducial_new="q2>0.1 & q2<19"; + + + TString cut = cutnew + "&&"+fiducial_new; + + vector variables={"B0_M", "Kstar_M", "J_psi_M", "B0_DiraAngle", "B0_ENDVERTEX_CHI2", "B0_IP_OWNPV", "B0_IPCHI2_OWNPV", "B0_P", "B0_PT", + "K_IPCHI2_OWNPV", "K_P", "K_PT", "K_PIDmu", "K_PIDK", "K_PIDp", + "Pi_IPCHI2_OWNPV", "Pi_P", "Pi_PT", "Pi_PIDmu", "Pi_PIDK", "Pi_PIDp", + "mu_plus_IPCHI2_OWNPV", "mu_plus_P", "mu_plus_PT", "mu_plus_PIDmu", "mu_plus_PIDK", "mu_plus_PIDp", + "mu_minus_IPCHI2_OWNPV", "mu_minus_P", "mu_minus_PT", "mu_minus_PIDmu", "mu_minus_PIDK", "mu_minus_PIDp" }; + + + + vector range={ "(100,5060,6000)", "(100,795.9, 995.9)","(100,100,4000)", "(100,0,0.014)", "(100,0,30)", "(100,0,0.12)", "(100,0., 16.)", "(100,10000, 300000)", "(100,100, 30000)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-5,80)", "(100,-40,50)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-80,20)", "(100,-80,20)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)", + "(100,0,200)","(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)"}; + + + if(variables.size() != range.size()) + { + cout<<"Wrong number of arguments!"<< variables.size()<<" "<< range.size()<Draw(variables[i]+">>"+variables[i]+range[i], cut); + ch_S21_unique->Draw(variables[i]+">>"+variables[i]+"1"+range[i]); + ch_S20_unique->Draw(variables[i]+">>"+variables[i]+"2"+range[i]); + + TH1D* hist= (TH1D*)gROOT->FindObject(variables[i]); + TH1D* hist1= (TH1D*)gROOT->FindObject(variables[i] +"1"); + TH1D* hist2= (TH1D*)gROOT->FindObject(variables[i]+"2"); + + hist->SetFillColor(0); + hist1->SetFillColor(0); + hist2->SetFillColor(0); + + hist->SetLineColor(kRed); + hist1->SetLineColor(kBlue+2); + hist2->SetLineColor(kGreen+2); + + + hist->GetXaxis()->SetTitle(variables[i]); + hist1->GetXaxis()->SetTitle(variables[i]); + hist2->GetXaxis()->SetTitle(variables[i]); + + hist->SetMaximum(hist->GetMaximum()*1.5); + hist1->SetMaximum(hist1->GetMaximum()*1.5); + hist2->SetMaximum(hist2->GetMaximum()*1.5); + + + hist->DrawNormalized(); + hist1->DrawNormalized("SAME"); + hist2->DrawNormalized("SAME"); + + + //if(i==0) + // { + TLegend *leg= new TLegend(0.6, 0.8, 0.9, 0.9); + leg->AddEntry(hist, "S21", "f"); + leg->AddEntry(hist1, "Unique in S21" ,"f"); + leg->AddEntry(hist2, "Unique in S20" ,"f"); + + leg->Draw(); + + // } + + c1->SaveAs(variables[i]+".pdf"); + + } + + + + + + + + + + + +} diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/lhcbStyle.C b/Kstarmumu_Run2/Overlaps/images/FULLREGION/lhcbStyle.C new file mode 100644 index 0000000..5d8a70c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/lhcbStyle.C @@ -0,0 +1,196 @@ +// all users - please change the name of this file to lhcbStyle.C +// Commits to lhcbdocs svn of .C files are not allowed +{ + + // define names for colours + Int_t black = 1; + Int_t red = 2; + Int_t green = 3; + Int_t blue = 4; + Int_t yellow = 5; + Int_t magenta= 6; + Int_t cyan = 7; + Int_t purple = 9; + + +//////////////////////////////////////////////////////////////////// +// PURPOSE: +// +// This macro defines a standard style for (black-and-white) +// "publication quality" LHCb ROOT plots. +// +// USAGE: +// +// Include the lines +// gROOT->ProcessLine(".L lhcbstyle.C"); +// lhcbStyle(); +// at the beginning of your root macro. +// +// Example usage is given in myPlot.C +// +// COMMENTS: +// +// Font: +// +// The font is chosen to be 132, this is Times New Roman (like the text of +// your document) with precision 2. +// +// "Landscape histograms": +// +// The style here is designed for more or less square plots. +// For longer histograms, or canvas with many pads, adjustements are needed. +// For instance, for a canvas with 1x5 histograms: +// TCanvas* c1 = new TCanvas("c1", "L0 muons", 600, 800); +// c1->Divide(1,5); +// Adaptions like the following will be needed: +// gStyle->SetTickLength(0.05,"x"); +// gStyle->SetTickLength(0.01,"y"); +// gStyle->SetLabelSize(0.15,"x"); +// gStyle->SetLabelSize(0.1,"y"); +// gStyle->SetStatW(0.15); +// gStyle->SetStatH(0.5); +// +// Authors: Thomas Schietinger, Andrew Powell, Chris Parkes, Niels Tuning +// Maintained by Editorial board member (currently Niels) +/////////////////////////////////////////////////////////////////// + + // Use times new roman, precision 2 + Int_t lhcbFont = 132; // Old LHCb style: 62; + // Line thickness + Double_t lhcbWidth = 2.00; // Old LHCb style: 3.00; + // Text size + Double_t lhcbTSize = 0.06; + + // use plain black on white colors + gROOT->SetStyle("Plain"); + TStyle *lhcbStyle= new TStyle("lhcbStyle","LHCb plots style"); + + //lhcbStyle->SetErrorX(0); // don't suppress the error bar along X + + lhcbStyle->SetFillColor(1); + lhcbStyle->SetFillStyle(1001); // solid + lhcbStyle->SetFrameFillColor(0); + lhcbStyle->SetFrameBorderMode(0); + lhcbStyle->SetPadBorderMode(0); + lhcbStyle->SetPadColor(0); + lhcbStyle->SetCanvasBorderMode(0); + lhcbStyle->SetCanvasColor(0); + lhcbStyle->SetStatColor(0); + lhcbStyle->SetLegendBorderSize(0); + lhcbStyle->SetLegendFont(132); + + // If you want the usual gradient palette (blue -> red) + lhcbStyle->SetPalette(1); + // If you want colors that correspond to gray scale in black and white: + int colors[8] = {0,5,7,3,6,2,4,1}; + lhcbStyle->SetPalette(8,colors); + + // set the paper & margin sizes + lhcbStyle->SetPaperSize(20,26); + lhcbStyle->SetPadTopMargin(0.05); + lhcbStyle->SetPadRightMargin(0.05); // increase for colz plots + lhcbStyle->SetPadBottomMargin(0.16); + lhcbStyle->SetPadLeftMargin(0.14); + + // use large fonts + lhcbStyle->SetTextFont(lhcbFont); + lhcbStyle->SetTextSize(lhcbTSize); + lhcbStyle->SetLabelFont(lhcbFont,"x"); + lhcbStyle->SetLabelFont(lhcbFont,"y"); + lhcbStyle->SetLabelFont(lhcbFont,"z"); + lhcbStyle->SetLabelSize(lhcbTSize,"x"); + lhcbStyle->SetLabelSize(lhcbTSize,"y"); + lhcbStyle->SetLabelSize(lhcbTSize,"z"); + lhcbStyle->SetTitleFont(lhcbFont); + lhcbStyle->SetTitleFont(lhcbFont,"x"); + lhcbStyle->SetTitleFont(lhcbFont,"y"); + lhcbStyle->SetTitleFont(lhcbFont,"z"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"x"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"y"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"z"); + + // use medium bold lines and thick markers + lhcbStyle->SetLineWidth(lhcbWidth); + lhcbStyle->SetFrameLineWidth(lhcbWidth); + lhcbStyle->SetHistLineWidth(lhcbWidth); + lhcbStyle->SetFuncWidth(lhcbWidth); + lhcbStyle->SetGridWidth(lhcbWidth); + lhcbStyle->SetLineStyleString(2,"[12 12]"); // postscript dashes + lhcbStyle->SetMarkerStyle(20); + lhcbStyle->SetMarkerSize(1.0); + + // label offsets + lhcbStyle->SetLabelOffset(0.010,"X"); + lhcbStyle->SetLabelOffset(0.010,"Y"); + + // by default, do not display histogram decorations: + lhcbStyle->SetOptStat(0); + //lhcbStyle->SetOptStat("emr"); // show only nent -e , mean - m , rms -r + // full opts at http://root.cern.ch/root/html/TStyle.html#TStyle:SetOptStat + lhcbStyle->SetStatFormat("6.3g"); // specified as c printf options + lhcbStyle->SetOptTitle(0); + lhcbStyle->SetOptFit(0); + //lhcbStyle->SetOptFit(1011); // order is probability, Chi2, errors, parameters + //titles + lhcbStyle->SetTitleOffset(0.95,"X"); + lhcbStyle->SetTitleOffset(0.95,"Y"); + lhcbStyle->SetTitleOffset(1.2,"Z"); + lhcbStyle->SetTitleFillColor(0); + lhcbStyle->SetTitleStyle(0); + lhcbStyle->SetTitleBorderSize(0); + lhcbStyle->SetTitleFont(lhcbFont,"title"); + lhcbStyle->SetTitleX(0.0); + lhcbStyle->SetTitleY(1.0); + lhcbStyle->SetTitleW(1.0); + lhcbStyle->SetTitleH(0.05); + + // look of the statistics box: + lhcbStyle->SetStatBorderSize(0); + lhcbStyle->SetStatFont(lhcbFont); + lhcbStyle->SetStatFontSize(0.05); + lhcbStyle->SetStatX(0.9); + lhcbStyle->SetStatY(0.9); + lhcbStyle->SetStatW(0.25); + lhcbStyle->SetStatH(0.15); + + // put tick marks on top and RHS of plots + lhcbStyle->SetPadTickX(1); + lhcbStyle->SetPadTickY(1); + + // histogram divisions: only 5 in x to avoid label overlaps + lhcbStyle->SetNdivisions(505,"x"); + lhcbStyle->SetNdivisions(510,"y"); + + gROOT->SetStyle("lhcbStyle"); + gROOT->ForceStyle(); + + // add LHCb label + TPaveText* lhcbName = new TPaveText(gStyle->GetPadLeftMargin() + 0.05, + 0.87 - gStyle->GetPadTopMargin(), + gStyle->GetPadLeftMargin() + 0.20, + 0.95 - gStyle->GetPadTopMargin(), + "BRNDC"); + lhcbName->AddText("LHCb"); + lhcbName->SetFillColor(0); + lhcbName->SetTextAlign(12); + lhcbName->SetBorderSize(0); + + TText *lhcbLabel = new TText(); + lhcbLabel->SetTextFont(lhcbFont); + lhcbLabel->SetTextColor(1); + lhcbLabel->SetTextSize(lhcbTSize); + lhcbLabel->SetTextAlign(12); + + TLatex *lhcbLatex = new TLatex(); + lhcbLatex->SetTextFont(lhcbFont); + lhcbLatex->SetTextColor(1); + lhcbLatex->SetTextSize(lhcbTSize); + lhcbLatex->SetTextAlign(12); + + cout << "-------------------------" << endl; + cout << "Set LHCb Style - Feb 2012" << endl; + cout << "-------------------------" << endl; + +} + + diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/log b/Kstarmumu_Run2/Overlaps/images/FULLREGION/log new file mode 100644 index 0000000..63f080b --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/log @@ -0,0 +1,15 @@ +OLD: +Processing 646780 events from 646782 +Processing 646781 events from 646782 +Processing 646782 events from 646782 +Finished filling ntuple 167.544130087 sec +Finished writing ntuple 167.572943926 sec + + +NEW: + +Processing 642625 events from 642627 +Processing 642626 events from 642627 +Processing 642627 events from 642627 +Finished filling ntuple 112.242563963 sec +Finished writing ntuple 112.281162024 sec diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/log~ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/log~ new file mode 100644 index 0000000..a376e9a --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/log~ @@ -0,0 +1,8 @@ +OLD: +Processing 646780 events from 646782 +Processing 646781 events from 646782 +Processing 646782 events from 646782 +Finished filling ntuple 167.544130087 sec +Finished writing ntuple 167.572943926 sec + + diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..7ac418b --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_P.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_P.pdf new file mode 100644 index 0000000..6d9a958 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PIDK.pdf new file mode 100644 index 0000000..b9e3ccb --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PIDK.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PIDmu.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PIDmu.pdf new file mode 100644 index 0000000..3cd0483 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PIDmu.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PIDp.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PIDp.pdf new file mode 100644 index 0000000..64fbbd1 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PIDp.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PT.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PT.pdf new file mode 100644 index 0000000..31761eb --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_minus_PT.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..1c95ffa --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_P.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_P.pdf new file mode 100644 index 0000000..6e59a19 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PIDK.pdf new file mode 100644 index 0000000..93df7bd --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PIDK.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PIDmu.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PIDmu.pdf new file mode 100644 index 0000000..4153099 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PIDmu.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PIDp.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PIDp.pdf new file mode 100644 index 0000000..403012d --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PIDp.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PT.pdf b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PT.pdf new file mode 100644 index 0000000..b656077 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/FULLREGION/mu_plus_PT.pdf Binary files differ diff --git "a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/\043compare.cc\043" "b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/\043compare.cc\043" new file mode 100644 index 0000000..bdc0276 --- /dev/null +++ "b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/\043compare.cc\043" @@ -0,0 +1,108 @@ +void compare() +{ + + gROOT->ProcessLine(".L lhcbStyle.C"); + + TCanvas *c1= new TCanvas("c1", "c1", 800,600); + + TChain *ch_S21= new TChain(); + TChain *ch_S21_unique= new TChain(); + TChain *ch_S20_unique= new TChain(); + + ch_S21->Add("/storage4/ntuples/lhcb/KstarMuMu/data_reduced/Run1/Kstarmumu_Data_Run1.root/Reduced"); + ch_S21_unique->Add("NEW.root/NEW"); + ch_S20_unique->Add("OLD.root/OLD"); + + + TString cutnew= "B0_M>5050 && B0_M<5700 && Kstar_M>795.9 && Kstar_M < 995.9 && K_TRACK_GhostProb<0.4 && Pi_TRACK_GhostProb<0.4 && mu_plus_TRACK_GhostProb<0.4 && mu_minus_TRACK_GhostProb<0.4 && (!((B0_ID>0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID<0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID>0)&&(B0_kmuswapMass>3626)&&(B0_kmuswapMass<3746)&&(K_PIDmu>5||K_isMuon==1Processing 532067 events from 532068 +Processing 532068 events from 532068 +Finished filling ntuple 122.167264938 sec +Finished writing ntuple 122.21688509 sec +)))" ; + + TString fiducial_new="q2>0.1 & q2<19"; + + + TString cut = cutnew + "&&"+fiducial_new; + + vector variables={"B0_M", "Kstar_M", "J_psi_M", "B0_DiraAngle", "B0_ENDVERTEX_CHI2", "B0_IP_OWNPV", "B0_IPCHI2_OWNPV", "B0_P", "B0_PT", + "K_IPCHI2_OWNPV", "K_P", "K_PT", "K_PIDmu", "K_PIDK", "K_PIDp", + "Pi_IPCHI2_OWNPV", "Pi_P", "Pi_PT", "Pi_PIDmu", "Pi_PIDK", "Pi_PIDp", + "mu_plus_IPCHI2_OWNPV", "mu_plus_P", "mu_plus_PT", "mu_plus_PIDmu", "mu_plus_PIDK", "mu_plus_PIDp", + "mu_minus_IPCHI2_OWNPV", "mu_minus_P", "mu_minus_PT", "mu_minus_PIDmu", "mu_minus_PIDK", "mu_minus_PIDp" }; + + + + vector range={ "(100,5060,6000)", "(100,795.9, 995.9)","(100,100,4000)", "(100,0,0.014)", "(100,0,30)", "(100,0,0.12)", "(100,0., 16.)", "(100,10000, 300000)", "(100,100, 30000)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-5,80)", "(100,-40,50)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-80,20)", "(100,-80,20)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)", + "(100,0,200)","(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)"}; + + + if(variables.size() != range.size()) + { + cout<<"Wrong number of arguments!"<< variables.size()<<" "<< range.size()<Draw(variables[i]+">>"+variables[i]+range[i], cut); + ch_S21_unique->Draw(variables[i]+">>"+variables[i]+"1"+range[i]); + ch_S20_unique->Draw(variables[i]+">>"+variables[i]+"2"+range[i]); + + TH1D* hist= (TH1D*)gROOT->FindObject(variables[i]); + TH1D* hist1= (TH1D*)gROOT->FindObject(variables[i] +"1"); + TH1D* hist2= (TH1D*)gROOT->FindObject(variables[i]+"2"); + + hist->SetFillColor(0); + hist1->SetFillColor(0); + hist2->SetFillColor(0); + + hist->SetLineColor(kRed); + hist1->SetLineColor(kBlue+2); + hist2->SetLineColor(kGreen+2); + + + hist->GetXaxis()->SetTitle(variables[i]); + hist1->GetXaxis()->SetTitle(variables[i]); + hist2->GetXaxis()->SetTitle(variables[i]); + + hist->SetMaximum(hist->GetMaximum()*1.5); + hist1->SetMaximum(hist1->GetMaximum()*1.5); + hist2->SetMaximum(hist2->GetMaximum()*1.5); + + + hist->DrawNormalized(); + hist1->DrawNormalized("SAME"); + hist2->DrawNormalized("SAME"); + + + //if(i==0) + // { + TLegend *leg= new TLegend(0.6, 0.8, 0.9, 0.9); + leg->AddEntry(hist, "S21", "f"); + leg->AddEntry(hist1, "Unique in S21" ,"f"); + leg->AddEntry(hist2, "Unique in S20" ,"f"); + + leg->Draw(); + + // } + + c1->SaveAs(variables[i]+".pdf"); + + } + + + + + + + + + + + +} diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_DiraAngle.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_DiraAngle.pdf new file mode 100644 index 0000000..8e4f105 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_DiraAngle.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_ENDVERTEX_CHI2.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_ENDVERTEX_CHI2.pdf new file mode 100644 index 0000000..6d40423 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_ENDVERTEX_CHI2.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..0767c42 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_IP_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_IP_OWNPV.pdf new file mode 100644 index 0000000..49792af --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_IP_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_M.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_M.pdf new file mode 100644 index 0000000..027414e --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_M.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_P.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_P.pdf new file mode 100644 index 0000000..faa195e --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_PT.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_PT.pdf new file mode 100644 index 0000000..5ad5f75 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/B0_PT.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/J_psi_M.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/J_psi_M.pdf new file mode 100644 index 0000000..0e29897 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/J_psi_M.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..768a609 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_P.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_P.pdf new file mode 100644 index 0000000..b6fbccc --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PIDK.pdf new file mode 100644 index 0000000..42d6357 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PIDK.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PIDmu.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PIDmu.pdf new file mode 100644 index 0000000..02efc6a --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PIDmu.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PIDp.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PIDp.pdf new file mode 100644 index 0000000..294c59e --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PIDp.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PT.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PT.pdf new file mode 100644 index 0000000..98dfff6 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/K_PT.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Kstar_M.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Kstar_M.pdf new file mode 100644 index 0000000..f94299b --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Kstar_M.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/NEW.root b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/NEW.root new file mode 100644 index 0000000..9c03ba4 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/NEW.root Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/OLD.root b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/OLD.root new file mode 100644 index 0000000..d4366e6 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/OLD.root Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..9fe63fa --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_P.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_P.pdf new file mode 100644 index 0000000..3dcedd7 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PIDK.pdf new file mode 100644 index 0000000..35b71b4 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PIDK.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PIDmu.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PIDmu.pdf new file mode 100644 index 0000000..13d1e8c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PIDmu.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PIDp.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PIDp.pdf new file mode 100644 index 0000000..231853c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PIDp.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PT.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PT.pdf new file mode 100644 index 0000000..5cea8ee --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/Pi_PT.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/compare.cc b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/compare.cc new file mode 100644 index 0000000..abdf68a --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/compare.cc @@ -0,0 +1,104 @@ +void compare() +{ + + gROOT->ProcessLine(".L lhcbStyle.C"); + + TCanvas *c1= new TCanvas("c1", "c1", 800,600); + + TChain *ch_S21= new TChain(); + TChain *ch_S21_unique= new TChain(); + TChain *ch_S20_unique= new TChain(); + + ch_S21->Add("/storage4/ntuples/lhcb/KstarMuMu/data_reduced/Run1/Kstarmumu_Data_Run1.root/Reduced"); + ch_S21_unique->Add("NEW.root/NEW"); + ch_S20_unique->Add("OLD.root/OLD"); + + + TString cutnew= "B0_M>5050 && B0_M<5700 && Kstar_M>795.9 && Kstar_M < 995.9 && K_TRACK_GhostProb<0.4 && Pi_TRACK_GhostProb<0.4 && mu_plus_TRACK_GhostProb<0.4 && mu_minus_TRACK_GhostProb<0.4 && (!((B0_ID>0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID<0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID>0)&&(B0_kmuswapMass>3626)&&(B0_kmuswapMass<3746)&&(K_PIDmu>5||K_isMuon==1)))" ; + TString fiducial_new="J_psi_M>3037 && J_psi_M <3157."; + + + + TString cut = cutnew + "&&"+fiducial_new; + + vector variables={"B0_M", "Kstar_M", "J_psi_M", "B0_DiraAngle", "B0_ENDVERTEX_CHI2", "B0_IP_OWNPV", "B0_IPCHI2_OWNPV", "B0_P", "B0_PT", + "K_IPCHI2_OWNPV", "K_P", "K_PT", "K_PIDmu", "K_PIDK", "K_PIDp", + "Pi_IPCHI2_OWNPV", "Pi_P", "Pi_PT", "Pi_PIDmu", "Pi_PIDK", "Pi_PIDp", + "mu_plus_IPCHI2_OWNPV", "mu_plus_P", "mu_plus_PT", "mu_plus_PIDmu", "mu_plus_PIDK", "mu_plus_PIDp", + "mu_minus_IPCHI2_OWNPV", "mu_minus_P", "mu_minus_PT", "mu_minus_PIDmu", "mu_minus_PIDK", "mu_minus_PIDp" }; + + + + vector range={ "(100,5060,6000)", "(100,795.9, 995.9)","(100,100,4000)", "(100,0,0.014)", "(100,0,30)", "(100,0,0.12)", "(100,0., 16.)", "(100,10000, 300000)", "(100,100, 30000)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-5,80)", "(100,-40,50)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-80,20)", "(100,-80,20)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)", + "(100,0,200)","(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)"}; + + + if(variables.size() != range.size()) + { + cout<<"Wrong number of arguments!"<< variables.size()<<" "<< range.size()<Draw(variables[i]+">>"+variables[i]+range[i], cut); + ch_S21_unique->Draw(variables[i]+">>"+variables[i]+"1"+range[i]); + ch_S20_unique->Draw(variables[i]+">>"+variables[i]+"2"+range[i]); + + TH1D* hist= (TH1D*)gROOT->FindObject(variables[i]); + TH1D* hist1= (TH1D*)gROOT->FindObject(variables[i] +"1"); + TH1D* hist2= (TH1D*)gROOT->FindObject(variables[i]+"2"); + + hist->SetFillColor(0); + hist1->SetFillColor(0); + hist2->SetFillColor(0); + + hist->SetLineColor(kRed); + hist1->SetLineColor(kBlue+2); + hist2->SetLineColor(kGreen+2); + + + hist->GetXaxis()->SetTitle(variables[i]); + hist1->GetXaxis()->SetTitle(variables[i]); + hist2->GetXaxis()->SetTitle(variables[i]); + + hist->SetMaximum(hist->GetMaximum()*1.5); + hist1->SetMaximum(hist1->GetMaximum()*1.5); + hist2->SetMaximum(hist2->GetMaximum()*1.5); + + + hist->DrawNormalized(); + hist1->DrawNormalized("SAME"); + hist2->DrawNormalized("SAME"); + + + //if(i==0) + // { + TLegend *leg= new TLegend(0.6, 0.8, 0.9, 0.9); + leg->AddEntry(hist, "S21", "f"); + leg->AddEntry(hist1, "Unique in S21" ,"f"); + leg->AddEntry(hist2, "Unique in S20" ,"f"); + + leg->Draw(); + + // } + + c1->SaveAs(variables[i]+".pdf"); + + } + + + + + + + + + + + +} diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/compare.cc~ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/compare.cc~ new file mode 100644 index 0000000..a9c705b --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/compare.cc~ @@ -0,0 +1,103 @@ +void compare() +{ + + gROOT->ProcessLine(".L lhcbStyle.C"); + + TCanvas *c1= new TCanvas("c1", "c1", 800,600); + + TChain *ch_S21= new TChain(); + TChain *ch_S21_unique= new TChain(); + TChain *ch_S20_unique= new TChain(); + + ch_S21->Add("/storage4/ntuples/lhcb/KstarMuMu/data_reduced/Run1/Kstarmumu_Data_Run1.root/Reduced"); + ch_S21_unique->Add("NEW.root/NEW"); + ch_S20_unique->Add("OLD.root/OLD"); + + + TString cutnew= "B0_M>5050 && B0_M<5700 && Kstar_M>795.9 && Kstar_M < 995.9 && K_TRACK_GhostProb<0.4 && Pi_TRACK_GhostProb<0.4 && mu_plus_TRACK_GhostProb<0.4 && mu_minus_TRACK_GhostProb<0.4 && (!((B0_ID>0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID<0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID>0)&&(B0_kmuswapMass>3626)&&(B0_kmuswapMass<3746)&&(K_PIDmu>5||K_isMuon==1)))" ; + TString fiducial_new="q2>0.1 & q2<19"; + + + TString cut = cutnew + "&&"+fiducial_new; + + vector variables={"B0_M", "Kstar_M", "J_psi_M", "B0_DiraAngle", "B0_ENDVERTEX_CHI2", "B0_IP_OWNPV", "B0_IPCHI2_OWNPV", "B0_P", "B0_PT", + "K_IPCHI2_OWNPV", "K_P", "K_PT", "K_PIDmu", "K_PIDK", "K_PIDp", + "Pi_IPCHI2_OWNPV", "Pi_P", "Pi_PT", "Pi_PIDmu", "Pi_PIDK", "Pi_PIDp", + "mu_plus_IPCHI2_OWNPV", "mu_plus_P", "mu_plus_PT", "mu_plus_PIDmu", "mu_plus_PIDK", "mu_plus_PIDp", + "mu_minus_IPCHI2_OWNPV", "mu_minus_P", "mu_minus_PT", "mu_minus_PIDmu", "mu_minus_PIDK", "mu_minus_PIDp" }; + + + + vector range={ "(100,5060,6000)", "(100,795.9, 995.9)","(100,100,4000)", "(100,0,0.014)", "(100,0,30)", "(100,0,0.12)", "(100,0., 16.)", "(100,10000, 300000)", "(100,100, 30000)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-5,80)", "(100,-40,50)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-80,20)", "(100,-80,20)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)", + "(100,0,200)","(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)"}; + + + if(variables.size() != range.size()) + { + cout<<"Wrong number of arguments!"<< variables.size()<<" "<< range.size()<Draw(variables[i]+">>"+variables[i]+range[i], cut); + ch_S21_unique->Draw(variables[i]+">>"+variables[i]+"1"+range[i]); + ch_S20_unique->Draw(variables[i]+">>"+variables[i]+"2"+range[i]); + + TH1D* hist= (TH1D*)gROOT->FindObject(variables[i]); + TH1D* hist1= (TH1D*)gROOT->FindObject(variables[i] +"1"); + TH1D* hist2= (TH1D*)gROOT->FindObject(variables[i]+"2"); + + hist->SetFillColor(0); + hist1->SetFillColor(0); + hist2->SetFillColor(0); + + hist->SetLineColor(kRed); + hist1->SetLineColor(kBlue+2); + hist2->SetLineColor(kGreen+2); + + + hist->GetXaxis()->SetTitle(variables[i]); + hist1->GetXaxis()->SetTitle(variables[i]); + hist2->GetXaxis()->SetTitle(variables[i]); + + hist->SetMaximum(hist->GetMaximum()*1.5); + hist1->SetMaximum(hist1->GetMaximum()*1.5); + hist2->SetMaximum(hist2->GetMaximum()*1.5); + + + hist->DrawNormalized(); + hist1->DrawNormalized("SAME"); + hist2->DrawNormalized("SAME"); + + + //if(i==0) + // { + TLegend *leg= new TLegend(0.6, 0.8, 0.9, 0.9); + leg->AddEntry(hist, "S21", "f"); + leg->AddEntry(hist1, "Unique in S21" ,"f"); + leg->AddEntry(hist2, "Unique in S20" ,"f"); + + leg->Draw(); + + // } + + c1->SaveAs(variables[i]+".pdf"); + + } + + + + + + + + + + + +} diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/lhcbStyle.C b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/lhcbStyle.C new file mode 100644 index 0000000..5d8a70c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/lhcbStyle.C @@ -0,0 +1,196 @@ +// all users - please change the name of this file to lhcbStyle.C +// Commits to lhcbdocs svn of .C files are not allowed +{ + + // define names for colours + Int_t black = 1; + Int_t red = 2; + Int_t green = 3; + Int_t blue = 4; + Int_t yellow = 5; + Int_t magenta= 6; + Int_t cyan = 7; + Int_t purple = 9; + + +//////////////////////////////////////////////////////////////////// +// PURPOSE: +// +// This macro defines a standard style for (black-and-white) +// "publication quality" LHCb ROOT plots. +// +// USAGE: +// +// Include the lines +// gROOT->ProcessLine(".L lhcbstyle.C"); +// lhcbStyle(); +// at the beginning of your root macro. +// +// Example usage is given in myPlot.C +// +// COMMENTS: +// +// Font: +// +// The font is chosen to be 132, this is Times New Roman (like the text of +// your document) with precision 2. +// +// "Landscape histograms": +// +// The style here is designed for more or less square plots. +// For longer histograms, or canvas with many pads, adjustements are needed. +// For instance, for a canvas with 1x5 histograms: +// TCanvas* c1 = new TCanvas("c1", "L0 muons", 600, 800); +// c1->Divide(1,5); +// Adaptions like the following will be needed: +// gStyle->SetTickLength(0.05,"x"); +// gStyle->SetTickLength(0.01,"y"); +// gStyle->SetLabelSize(0.15,"x"); +// gStyle->SetLabelSize(0.1,"y"); +// gStyle->SetStatW(0.15); +// gStyle->SetStatH(0.5); +// +// Authors: Thomas Schietinger, Andrew Powell, Chris Parkes, Niels Tuning +// Maintained by Editorial board member (currently Niels) +/////////////////////////////////////////////////////////////////// + + // Use times new roman, precision 2 + Int_t lhcbFont = 132; // Old LHCb style: 62; + // Line thickness + Double_t lhcbWidth = 2.00; // Old LHCb style: 3.00; + // Text size + Double_t lhcbTSize = 0.06; + + // use plain black on white colors + gROOT->SetStyle("Plain"); + TStyle *lhcbStyle= new TStyle("lhcbStyle","LHCb plots style"); + + //lhcbStyle->SetErrorX(0); // don't suppress the error bar along X + + lhcbStyle->SetFillColor(1); + lhcbStyle->SetFillStyle(1001); // solid + lhcbStyle->SetFrameFillColor(0); + lhcbStyle->SetFrameBorderMode(0); + lhcbStyle->SetPadBorderMode(0); + lhcbStyle->SetPadColor(0); + lhcbStyle->SetCanvasBorderMode(0); + lhcbStyle->SetCanvasColor(0); + lhcbStyle->SetStatColor(0); + lhcbStyle->SetLegendBorderSize(0); + lhcbStyle->SetLegendFont(132); + + // If you want the usual gradient palette (blue -> red) + lhcbStyle->SetPalette(1); + // If you want colors that correspond to gray scale in black and white: + int colors[8] = {0,5,7,3,6,2,4,1}; + lhcbStyle->SetPalette(8,colors); + + // set the paper & margin sizes + lhcbStyle->SetPaperSize(20,26); + lhcbStyle->SetPadTopMargin(0.05); + lhcbStyle->SetPadRightMargin(0.05); // increase for colz plots + lhcbStyle->SetPadBottomMargin(0.16); + lhcbStyle->SetPadLeftMargin(0.14); + + // use large fonts + lhcbStyle->SetTextFont(lhcbFont); + lhcbStyle->SetTextSize(lhcbTSize); + lhcbStyle->SetLabelFont(lhcbFont,"x"); + lhcbStyle->SetLabelFont(lhcbFont,"y"); + lhcbStyle->SetLabelFont(lhcbFont,"z"); + lhcbStyle->SetLabelSize(lhcbTSize,"x"); + lhcbStyle->SetLabelSize(lhcbTSize,"y"); + lhcbStyle->SetLabelSize(lhcbTSize,"z"); + lhcbStyle->SetTitleFont(lhcbFont); + lhcbStyle->SetTitleFont(lhcbFont,"x"); + lhcbStyle->SetTitleFont(lhcbFont,"y"); + lhcbStyle->SetTitleFont(lhcbFont,"z"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"x"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"y"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"z"); + + // use medium bold lines and thick markers + lhcbStyle->SetLineWidth(lhcbWidth); + lhcbStyle->SetFrameLineWidth(lhcbWidth); + lhcbStyle->SetHistLineWidth(lhcbWidth); + lhcbStyle->SetFuncWidth(lhcbWidth); + lhcbStyle->SetGridWidth(lhcbWidth); + lhcbStyle->SetLineStyleString(2,"[12 12]"); // postscript dashes + lhcbStyle->SetMarkerStyle(20); + lhcbStyle->SetMarkerSize(1.0); + + // label offsets + lhcbStyle->SetLabelOffset(0.010,"X"); + lhcbStyle->SetLabelOffset(0.010,"Y"); + + // by default, do not display histogram decorations: + lhcbStyle->SetOptStat(0); + //lhcbStyle->SetOptStat("emr"); // show only nent -e , mean - m , rms -r + // full opts at http://root.cern.ch/root/html/TStyle.html#TStyle:SetOptStat + lhcbStyle->SetStatFormat("6.3g"); // specified as c printf options + lhcbStyle->SetOptTitle(0); + lhcbStyle->SetOptFit(0); + //lhcbStyle->SetOptFit(1011); // order is probability, Chi2, errors, parameters + //titles + lhcbStyle->SetTitleOffset(0.95,"X"); + lhcbStyle->SetTitleOffset(0.95,"Y"); + lhcbStyle->SetTitleOffset(1.2,"Z"); + lhcbStyle->SetTitleFillColor(0); + lhcbStyle->SetTitleStyle(0); + lhcbStyle->SetTitleBorderSize(0); + lhcbStyle->SetTitleFont(lhcbFont,"title"); + lhcbStyle->SetTitleX(0.0); + lhcbStyle->SetTitleY(1.0); + lhcbStyle->SetTitleW(1.0); + lhcbStyle->SetTitleH(0.05); + + // look of the statistics box: + lhcbStyle->SetStatBorderSize(0); + lhcbStyle->SetStatFont(lhcbFont); + lhcbStyle->SetStatFontSize(0.05); + lhcbStyle->SetStatX(0.9); + lhcbStyle->SetStatY(0.9); + lhcbStyle->SetStatW(0.25); + lhcbStyle->SetStatH(0.15); + + // put tick marks on top and RHS of plots + lhcbStyle->SetPadTickX(1); + lhcbStyle->SetPadTickY(1); + + // histogram divisions: only 5 in x to avoid label overlaps + lhcbStyle->SetNdivisions(505,"x"); + lhcbStyle->SetNdivisions(510,"y"); + + gROOT->SetStyle("lhcbStyle"); + gROOT->ForceStyle(); + + // add LHCb label + TPaveText* lhcbName = new TPaveText(gStyle->GetPadLeftMargin() + 0.05, + 0.87 - gStyle->GetPadTopMargin(), + gStyle->GetPadLeftMargin() + 0.20, + 0.95 - gStyle->GetPadTopMargin(), + "BRNDC"); + lhcbName->AddText("LHCb"); + lhcbName->SetFillColor(0); + lhcbName->SetTextAlign(12); + lhcbName->SetBorderSize(0); + + TText *lhcbLabel = new TText(); + lhcbLabel->SetTextFont(lhcbFont); + lhcbLabel->SetTextColor(1); + lhcbLabel->SetTextSize(lhcbTSize); + lhcbLabel->SetTextAlign(12); + + TLatex *lhcbLatex = new TLatex(); + lhcbLatex->SetTextFont(lhcbFont); + lhcbLatex->SetTextColor(1); + lhcbLatex->SetTextSize(lhcbTSize); + lhcbLatex->SetTextAlign(12); + + cout << "-------------------------" << endl; + cout << "Set LHCb Style - Feb 2012" << endl; + cout << "-------------------------" << endl; + +} + + diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/log b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/log new file mode 100644 index 0000000..ce1bfa8 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/log @@ -0,0 +1,14 @@ +OLD: + +Processing 532067 events from 532068 +Processing 532068 events from 532068 +Finished filling ntuple 122.167264938 sec +Finished writing ntuple 122.21688509 sec + + +NEW: + +Processing 528063 events from 528064 +Processing 528064 events from 528064 +Finished filling ntuple 75.038364172 sec +Finished writing ntuple 75.0701282024 sec diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/log~ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/log~ new file mode 100644 index 0000000..603277d --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/log~ @@ -0,0 +1,9 @@ +OLD: + +Processing 532067 events from 532068 +Processing 532068 events from 532068 +Finished filling ntuple 122.167264938 sec +Finished writing ntuple 122.21688509 sec + + +NEW: diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..98ab4b0 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_P.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_P.pdf new file mode 100644 index 0000000..f2a373a --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_PIDK.pdf new file mode 100644 index 0000000..e7158c7 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_PIDK.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/JPSIREGION/mu_minus_PIDmu.pdf 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a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/OLD.root b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/OLD.root new file mode 100644 index 0000000..9ae2e38 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/OLD.root Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..285b028 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_IPCHI2_OWNPV.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_P.pdf b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_P.pdf new file mode 100644 index 0000000..6c2dc81 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_P.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PIDK.pdf b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PIDK.pdf new file mode 100644 index 0000000..1510281 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PIDK.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PIDmu.pdf b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PIDmu.pdf new file mode 100644 index 0000000..4039d3e --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PIDmu.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PIDp.pdf b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PIDp.pdf new file mode 100644 index 0000000..b3b426a --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PIDp.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PT.pdf b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PT.pdf new file mode 100644 index 0000000..7438fce --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/Pi_PT.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/compare.cc b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/compare.cc new file mode 100644 index 0000000..7a75e1e --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/compare.cc @@ -0,0 +1,104 @@ +void compare() +{ + + gROOT->ProcessLine(".L lhcbStyle.C"); + + TCanvas *c1= new TCanvas("c1", "c1", 800,600); + + TChain *ch_S21= new TChain(); + TChain *ch_S21_unique= new TChain(); + TChain *ch_S20_unique= new TChain(); + + ch_S21->Add("/storage4/ntuples/lhcb/KstarMuMu/data_reduced/Run1/Kstarmumu_Data_Run1.root/Reduced"); + ch_S21_unique->Add("NEW.root/NEW"); + ch_S20_unique->Add("OLD.root/OLD"); + + + TString cutnew= "B0_M>5050 && B0_M<5700 && Kstar_M>795.9 && Kstar_M < 995.9 && K_TRACK_GhostProb<0.4 && Pi_TRACK_GhostProb<0.4 && mu_plus_TRACK_GhostProb<0.4 && mu_minus_TRACK_GhostProb<0.4 && (!((B0_ID>0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID<0)&&(B0_swapMass>3626)&&(B0_swapMass<3746)&&(Pi_PIDmu>5||Pi_isMuon==1))&&!((B0_ID>0)&&(B0_kmuswapMass>3626)&&(B0_kmuswapMass<3746)&&(K_PIDmu>5||K_isMuon==1)))" ; + TString fiducial_new="J_psi_M>3625 && J_psi_M <3746."; + + + + TString cut = cutnew + "&&"+fiducial_new; + + vector variables={"B0_M", "Kstar_M", "J_psi_M", "B0_DiraAngle", "B0_ENDVERTEX_CHI2", "B0_IP_OWNPV", "B0_IPCHI2_OWNPV", "B0_P", "B0_PT", + "K_IPCHI2_OWNPV", "K_P", "K_PT", "K_PIDmu", "K_PIDK", "K_PIDp", + "Pi_IPCHI2_OWNPV", "Pi_P", "Pi_PT", "Pi_PIDmu", "Pi_PIDK", "Pi_PIDp", + "mu_plus_IPCHI2_OWNPV", "mu_plus_P", "mu_plus_PT", "mu_plus_PIDmu", "mu_plus_PIDK", "mu_plus_PIDp", + "mu_minus_IPCHI2_OWNPV", "mu_minus_P", "mu_minus_PT", "mu_minus_PIDmu", "mu_minus_PIDK", "mu_minus_PIDp" }; + + + + vector range={ "(100,5060,6000)", "(100,795.9, 995.9)","(100,100,4000)", "(100,0,0.014)", "(100,0,30)", "(100,0,0.12)", "(100,0., 16.)", "(100,10000, 300000)", "(100,100, 30000)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-5,80)", "(100,-40,50)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-15,15)", "(100,-80,20)", "(100,-80,20)", + "(100,0,200)", "(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)", + "(100,0,200)","(100,1000, 150000)", "(100,100, 5000)", "(100,-3,15)", "(100,-80,15)", "(100,-100,20)"}; + + + if(variables.size() != range.size()) + { + cout<<"Wrong number of arguments!"<< variables.size()<<" "<< range.size()<Draw(variables[i]+">>"+variables[i]+range[i], cut); + ch_S21_unique->Draw(variables[i]+">>"+variables[i]+"1"+range[i]); + ch_S20_unique->Draw(variables[i]+">>"+variables[i]+"2"+range[i]); + + TH1D* hist= (TH1D*)gROOT->FindObject(variables[i]); + TH1D* hist1= (TH1D*)gROOT->FindObject(variables[i] +"1"); + TH1D* hist2= (TH1D*)gROOT->FindObject(variables[i]+"2"); + + hist->SetFillColor(0); + hist1->SetFillColor(0); + hist2->SetFillColor(0); + + hist->SetLineColor(kRed); + hist1->SetLineColor(kBlue+2); + hist2->SetLineColor(kGreen+2); + + + hist->GetXaxis()->SetTitle(variables[i]); + hist1->GetXaxis()->SetTitle(variables[i]); + hist2->GetXaxis()->SetTitle(variables[i]); + + hist->SetMaximum(hist->GetMaximum()*1.5); + hist1->SetMaximum(hist1->GetMaximum()*1.5); + hist2->SetMaximum(hist2->GetMaximum()*1.5); + + + hist->DrawNormalized(); + hist1->DrawNormalized("SAME"); + hist2->DrawNormalized("SAME"); + + + //if(i==0) + // { + TLegend *leg= new TLegend(0.6, 0.8, 0.9, 0.9); + leg->AddEntry(hist, "S21", "f"); + leg->AddEntry(hist1, "Unique in S21" ,"f"); + leg->AddEntry(hist2, "Unique in S20" ,"f"); + + leg->Draw(); + + // } + + c1->SaveAs(variables[i]+".pdf"); + + } + + + + + + + + + + + +} diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/lhcbStyle.C b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/lhcbStyle.C new file mode 100644 index 0000000..5d8a70c --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/lhcbStyle.C @@ -0,0 +1,196 @@ +// all users - please change the name of this file to lhcbStyle.C +// Commits to lhcbdocs svn of .C files are not allowed +{ + + // define names for colours + Int_t black = 1; + Int_t red = 2; + Int_t green = 3; + Int_t blue = 4; + Int_t yellow = 5; + Int_t magenta= 6; + Int_t cyan = 7; + Int_t purple = 9; + + +//////////////////////////////////////////////////////////////////// +// PURPOSE: +// +// This macro defines a standard style for (black-and-white) +// "publication quality" LHCb ROOT plots. +// +// USAGE: +// +// Include the lines +// gROOT->ProcessLine(".L lhcbstyle.C"); +// lhcbStyle(); +// at the beginning of your root macro. +// +// Example usage is given in myPlot.C +// +// COMMENTS: +// +// Font: +// +// The font is chosen to be 132, this is Times New Roman (like the text of +// your document) with precision 2. +// +// "Landscape histograms": +// +// The style here is designed for more or less square plots. +// For longer histograms, or canvas with many pads, adjustements are needed. +// For instance, for a canvas with 1x5 histograms: +// TCanvas* c1 = new TCanvas("c1", "L0 muons", 600, 800); +// c1->Divide(1,5); +// Adaptions like the following will be needed: +// gStyle->SetTickLength(0.05,"x"); +// gStyle->SetTickLength(0.01,"y"); +// gStyle->SetLabelSize(0.15,"x"); +// gStyle->SetLabelSize(0.1,"y"); +// gStyle->SetStatW(0.15); +// gStyle->SetStatH(0.5); +// +// Authors: Thomas Schietinger, Andrew Powell, Chris Parkes, Niels Tuning +// Maintained by Editorial board member (currently Niels) +/////////////////////////////////////////////////////////////////// + + // Use times new roman, precision 2 + Int_t lhcbFont = 132; // Old LHCb style: 62; + // Line thickness + Double_t lhcbWidth = 2.00; // Old LHCb style: 3.00; + // Text size + Double_t lhcbTSize = 0.06; + + // use plain black on white colors + gROOT->SetStyle("Plain"); + TStyle *lhcbStyle= new TStyle("lhcbStyle","LHCb plots style"); + + //lhcbStyle->SetErrorX(0); // don't suppress the error bar along X + + lhcbStyle->SetFillColor(1); + lhcbStyle->SetFillStyle(1001); // solid + lhcbStyle->SetFrameFillColor(0); + lhcbStyle->SetFrameBorderMode(0); + lhcbStyle->SetPadBorderMode(0); + lhcbStyle->SetPadColor(0); + lhcbStyle->SetCanvasBorderMode(0); + lhcbStyle->SetCanvasColor(0); + lhcbStyle->SetStatColor(0); + lhcbStyle->SetLegendBorderSize(0); + lhcbStyle->SetLegendFont(132); + + // If you want the usual gradient palette (blue -> red) + lhcbStyle->SetPalette(1); + // If you want colors that correspond to gray scale in black and white: + int colors[8] = {0,5,7,3,6,2,4,1}; + lhcbStyle->SetPalette(8,colors); + + // set the paper & margin sizes + lhcbStyle->SetPaperSize(20,26); + lhcbStyle->SetPadTopMargin(0.05); + lhcbStyle->SetPadRightMargin(0.05); // increase for colz plots + lhcbStyle->SetPadBottomMargin(0.16); + lhcbStyle->SetPadLeftMargin(0.14); + + // use large fonts + lhcbStyle->SetTextFont(lhcbFont); + lhcbStyle->SetTextSize(lhcbTSize); + lhcbStyle->SetLabelFont(lhcbFont,"x"); + lhcbStyle->SetLabelFont(lhcbFont,"y"); + lhcbStyle->SetLabelFont(lhcbFont,"z"); + lhcbStyle->SetLabelSize(lhcbTSize,"x"); + lhcbStyle->SetLabelSize(lhcbTSize,"y"); + lhcbStyle->SetLabelSize(lhcbTSize,"z"); + lhcbStyle->SetTitleFont(lhcbFont); + lhcbStyle->SetTitleFont(lhcbFont,"x"); + lhcbStyle->SetTitleFont(lhcbFont,"y"); + lhcbStyle->SetTitleFont(lhcbFont,"z"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"x"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"y"); + lhcbStyle->SetTitleSize(1.2*lhcbTSize,"z"); + + // use medium bold lines and thick markers + lhcbStyle->SetLineWidth(lhcbWidth); + lhcbStyle->SetFrameLineWidth(lhcbWidth); + lhcbStyle->SetHistLineWidth(lhcbWidth); + lhcbStyle->SetFuncWidth(lhcbWidth); + lhcbStyle->SetGridWidth(lhcbWidth); + lhcbStyle->SetLineStyleString(2,"[12 12]"); // postscript dashes + lhcbStyle->SetMarkerStyle(20); + lhcbStyle->SetMarkerSize(1.0); + + // label offsets + lhcbStyle->SetLabelOffset(0.010,"X"); + lhcbStyle->SetLabelOffset(0.010,"Y"); + + // by default, do not display histogram decorations: + lhcbStyle->SetOptStat(0); + //lhcbStyle->SetOptStat("emr"); // show only nent -e , mean - m , rms -r + // full opts at http://root.cern.ch/root/html/TStyle.html#TStyle:SetOptStat + lhcbStyle->SetStatFormat("6.3g"); // specified as c printf options + lhcbStyle->SetOptTitle(0); + lhcbStyle->SetOptFit(0); + //lhcbStyle->SetOptFit(1011); // order is probability, Chi2, errors, parameters + //titles + lhcbStyle->SetTitleOffset(0.95,"X"); + lhcbStyle->SetTitleOffset(0.95,"Y"); + lhcbStyle->SetTitleOffset(1.2,"Z"); + lhcbStyle->SetTitleFillColor(0); + lhcbStyle->SetTitleStyle(0); + lhcbStyle->SetTitleBorderSize(0); + lhcbStyle->SetTitleFont(lhcbFont,"title"); + lhcbStyle->SetTitleX(0.0); + lhcbStyle->SetTitleY(1.0); + lhcbStyle->SetTitleW(1.0); + lhcbStyle->SetTitleH(0.05); + + // look of the statistics box: + lhcbStyle->SetStatBorderSize(0); + lhcbStyle->SetStatFont(lhcbFont); + lhcbStyle->SetStatFontSize(0.05); + lhcbStyle->SetStatX(0.9); + lhcbStyle->SetStatY(0.9); + lhcbStyle->SetStatW(0.25); + lhcbStyle->SetStatH(0.15); + + // put tick marks on top and RHS of plots + lhcbStyle->SetPadTickX(1); + lhcbStyle->SetPadTickY(1); + + // histogram divisions: only 5 in x to avoid label overlaps + lhcbStyle->SetNdivisions(505,"x"); + lhcbStyle->SetNdivisions(510,"y"); + + gROOT->SetStyle("lhcbStyle"); + gROOT->ForceStyle(); + + // add LHCb label + TPaveText* lhcbName = new TPaveText(gStyle->GetPadLeftMargin() + 0.05, + 0.87 - gStyle->GetPadTopMargin(), + gStyle->GetPadLeftMargin() + 0.20, + 0.95 - gStyle->GetPadTopMargin(), + "BRNDC"); + lhcbName->AddText("LHCb"); + lhcbName->SetFillColor(0); + lhcbName->SetTextAlign(12); + lhcbName->SetBorderSize(0); + + TText *lhcbLabel = new TText(); + lhcbLabel->SetTextFont(lhcbFont); + lhcbLabel->SetTextColor(1); + lhcbLabel->SetTextSize(lhcbTSize); + lhcbLabel->SetTextAlign(12); + + TLatex *lhcbLatex = new TLatex(); + lhcbLatex->SetTextFont(lhcbFont); + lhcbLatex->SetTextColor(1); + lhcbLatex->SetTextSize(lhcbTSize); + lhcbLatex->SetTextAlign(12); + + cout << "-------------------------" << endl; + cout << "Set LHCb Style - Feb 2012" << endl; + cout << "-------------------------" << endl; + +} + + diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/log b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/log new file mode 100644 index 0000000..6cf5c1f --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/log @@ -0,0 +1,17 @@ +OLD: + +Processing 41585 events from 41587 +Processing 41586 events from 41587 +Processing 41587 events from 41587 +Finished filling ntuple 32.4889957905 sec +Finished writing ntuple 32.5045368671 sec + + +NEW: + +Processing 41392 events from 41393 +Processing 41393 events from 41393 +Finished filling ntuple 32.8871917725 sec +Finished writing ntuple 32.91405797 sec + + diff --git a/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/mu_minus_IPCHI2_OWNPV.pdf b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/mu_minus_IPCHI2_OWNPV.pdf new file mode 100644 index 0000000..bab69d1 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/PSI2SREGION/mu_minus_IPCHI2_OWNPV.pdf Binary files differ 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new file mode 100644 index 0000000..4cb7f24 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/d.png Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/derotate.sh b/Kstarmumu_Run2/Overlaps/images/derotate.sh new file mode 100755 index 0000000..ba653b9 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/derotate.sh @@ -0,0 +1,13 @@ +#!/bin/bash +#FILES=*.pdf +FILES="$(find . -name '*.pdf')" +for f in $FILES +do + echo "Processing $f ..." + gs -sDEVICE=pdfwrite -dCompatibilityLevel=1.4 -dUseCIEColor -dPDFSETTINGS=/printer -dSAFER -dNOPAUSE -dQUIET -dBATCH -sOutputFile="temp.pdf" "$f" + mv temp.pdf "$f" +# pdf2ps "$f" temp.ps +# ps2pdf temp.ps "$f" +# rm temp.ps +done +#rm temp.pdf diff --git a/Kstarmumu_Run2/Overlaps/images/dirac.png b/Kstarmumu_Run2/Overlaps/images/dirac.png new file mode 100644 index 0000000..6757d18 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/dirac.png Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/espen1.png b/Kstarmumu_Run2/Overlaps/images/espen1.png new file mode 100644 index 0000000..1cf559b --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/espen1.png Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/espen2.png b/Kstarmumu_Run2/Overlaps/images/espen2.png new file mode 100644 index 0000000..ed9a9b8 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/espen2.png Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/espen3.png b/Kstarmumu_Run2/Overlaps/images/espen3.png new file mode 100644 index 0000000..419cc5f --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/espen3.png Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/images/getFromAFS.sh b/Kstarmumu_Run2/Overlaps/images/getFromAFS.sh new file mode 100644 index 0000000..7d73a4a --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/images/getFromAFS.sh @@ -0,0 +1,4 @@ +kinit egraveri@CERN.CH +aklog +cp -r /afs/cern.ch/user/e/egraveri/cmtuser/STMonitoring/NewTTAlignment/Out/Plots/AlignVSSimCond-D0Align ./img/ +cp -r 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It will be recreated as +required. + +@Control{biblatex-control, + options = {2.6:0:0:1:0:0:1:1:0:0:0:0:1:1:3:1:79:+}, +} diff --git a/Kstarmumu_Run2/Overlaps/mchrzasz.aux b/Kstarmumu_Run2/Overlaps/mchrzasz.aux new file mode 100644 index 0000000..d15a4bc --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/mchrzasz.aux @@ -0,0 +1,216 @@ +\relax +\providecommand\hyper@newdestlabel[2]{} +\providecommand\zref@newlabel[2]{} +\providecommand\HyperFirstAtBeginDocument{\AtBeginDocument} +\HyperFirstAtBeginDocument{\ifx\hyper@anchor\@undefined +\global\let\oldcontentsline\contentsline +\gdef\contentsline#1#2#3#4{\oldcontentsline{#1}{#2}{#3}} +\global\let\oldnewlabel\newlabel +\gdef\newlabel#1#2{\newlabelxx{#1}#2} +\gdef\newlabelxx#1#2#3#4#5#6{\oldnewlabel{#1}{{#2}{#3}}} +\AtEndDocument{\ifx\hyper@anchor\@undefined +\let\contentsline\oldcontentsline +\let\newlabel\oldnewlabel +\fi} +\fi} +\global\let\hyper@last\relax +\gdef\HyperFirstAtBeginDocument#1{#1} +\providecommand*\HyPL@Entry[1]{} 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\inserttotalframenumber {29}} diff --git a/Kstarmumu_Run2/Overlaps/mchrzasz.out b/Kstarmumu_Run2/Overlaps/mchrzasz.out new file mode 100644 index 0000000..e69de29 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/mchrzasz.out diff --git a/Kstarmumu_Run2/Overlaps/mchrzasz.pdf b/Kstarmumu_Run2/Overlaps/mchrzasz.pdf new file mode 100644 index 0000000..2e4d713 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/mchrzasz.pdf Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/mchrzasz.run.xml b/Kstarmumu_Run2/Overlaps/mchrzasz.run.xml new file mode 100644 index 0000000..4d0e3ba --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/mchrzasz.run.xml @@ -0,0 +1,91 @@ + + + + + + + + + + + + + + + + + + + + + + + + +]> + + + latex + + mchrzasz.aux + mchrzasz-blx.bib + + + mchrzasz.bbl + + + blx-compat.def + biblatex_legacy.def + numeric-comp.bbx + numeric.bbx + standard.bbx + numeric-comp.cbx + biblatex.cfg + english.lbx + + + + bibtex + + bibtex + + mchrzasz + + + mchrzasz.aux + + + mchrzasz.bbl + + + mchrzasz.bbl + + + mchrzasz.aux + mchrzasz-blx.bib + + + bib.bib + + + biblatex.bst + + + diff --git a/Kstarmumu_Run2/Overlaps/mchrzasz.snm b/Kstarmumu_Run2/Overlaps/mchrzasz.snm new file mode 100644 index 0000000..e69de29 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/mchrzasz.snm diff --git a/Kstarmumu_Run2/Overlaps/mchrzasz.synctex.gz b/Kstarmumu_Run2/Overlaps/mchrzasz.synctex.gz new file mode 100644 index 0000000..c603861 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/mchrzasz.synctex.gz Binary files differ diff --git a/Kstarmumu_Run2/Overlaps/mchrzasz.tex b/Kstarmumu_Run2/Overlaps/mchrzasz.tex new file mode 100644 index 0000000..007c515 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/mchrzasz.tex @@ -0,0 +1,879 @@ +\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} + +\usepackage[english]{babel} +\usepackage{polski} + + +\usetheme[ + bullet=circle, % Other option: square + bigpagenumber, % circled page number on lower right + topline=true, % colored bar at the top of the frame + shadow=false, % Shading for beamer blocks + watermark=BG_lower, % png file for the watermark + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +%\usepackage{emerald} +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} %for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + +\author{ {Marcin Chrzaszcz} (CERN)} +\institute{UZH} +\title[$\PBzero \to \PKstar \Pmuon \APmuon$ Update]{$\PBzero \to \PKstar \Pmuon \APmuon$ Update} +\date{14 February 2018} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright\bfseries \Huge {$\PBzero \to \PKstar \Pmuon \APmuon$\\ Finalization} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} { \Large Marcin Chrzaszcz } + +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=1.3cm]{cern} + +\end{column} +\end{columns} + +\vspace{1em} + +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{$\PBzero \to \PKstar \Pmuon \APmuon$ meeting, CERN\\February 14, 2018} +\end{center} +\end{frame} +} + + +\begin{frame}[c]{Reminder} + + \begin{minipage}{\textwidth} + +\ARROW Last week we saw a $4\%$ difference between the S20 and S21.\\ +\ARROW Most of the events were located in S21. \\ +\ARROW Many theories why... and if this is dangerous... + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\begin{frame}[c]{Overlap} + \begin{minipage}{\textwidth} + +\ARROW I have matched the S20 with S21 ntuples by \texttt{EventNumber} + +\begin{center} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/BEFOREBUGFIX/B0_M}.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/BEFOREBUGFIX/Pi_PIDp}.pdf} +\end{center} + + +\ARROW We have protons unique to S21. + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + +\begin{frame}[c]{Overlap} + \begin{minipage}{\textwidth} + +\begin{columns} + +\column{0.45\textwidth} +\begin{exampleblock}{S21:} +\includegraphics[angle=-90,width=0.99\textwidth]{{images/BEFOREBUGFIX/NEW}.pdf} +\end{exampleblock} +\column{0.45\textwidth} + +\begin{alertblock}{S20:} +\includegraphics[angle=-90,width=0.99\textwidth]{{images/BEFOREBUGFIX/OLD}.pdf} +\end{alertblock} + +\end{columns} + + +{~}\\{~}\\ +\ARROW Got the nasty bugger + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in \in (0.1, 19)$\\ +\ARROW Difference in number of events: $0.6\%$.\\ +\ARROW I have check and there are no unique RunNumbers in each of the set. + +\begin{center} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/FULLREGION/B0_DiraAngle}.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/FULLREGION/B0_ENDVERTEX_CHI2}.pdf} +\end{center} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in (0.1, 19)$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/B0_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/B0_IP_OWNPV}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/B0_M}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/B0_P}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in (0.1, 19)$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/B0_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/B0_IP_OWNPV}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/B0_M}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/B0_P}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in (0.1, 19)$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/B0_PT}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/J_psi_M}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/K_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/K_PIDK}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in (0.1, 19)$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/K_PIDmu}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/K_PIDp}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/K_P}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/K_PT}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in (0.1, 19)$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/Kstar_M}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/mu_minus_IPCHI2_OWNPV}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/mu_minus_PIDK}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/mu_minus_PIDmu}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in (0.1, 19)$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/mu_minus_P}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/mu_minus_PT}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/Pi_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/Pi_PIDK}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in (0.1, 19)$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/Pi_PIDmu}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/Pi_PIDp}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/Pi_P}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/FULLREGION/Pi_PT}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%% + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in \PJpsi \pm 60 \rm MeV/c^{2}s$\\ +\ARROW Difference in number of events: $0.7\%$.\\ + +\begin{center} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/JPSIREGION/B0_DiraAngle}.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/JPSIREGION/B0_ENDVERTEX_CHI2}.pdf} +\end{center} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in \PJpsi \pm 60 \rm MeV/c^{2}s$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/B0_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/B0_IP_OWNPV}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/B0_M}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/B0_P}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in \PJpsi \pm 60 \rm MeV/c^{2}s$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/B0_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/B0_IP_OWNPV}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/B0_M}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/B0_P}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in \PJpsi \pm 60 \rm MeV/c^{2}s$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/B0_PT}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/J_psi_M}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/K_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/K_PIDK}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in \PJpsi \pm 60 \rm MeV/c^{2}s$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/K_PIDmu}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/K_PIDp}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/K_P}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/K_PT}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in \PJpsi \pm 60 \rm MeV/c^{2}s$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/Kstar_M}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/mu_minus_IPCHI2_OWNPV}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/mu_minus_PIDK}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/mu_minus_PIDmu}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in \PJpsi \pm 60 \rm MeV/c^{2}s$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/mu_minus_P}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/mu_minus_PT}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/Pi_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/Pi_PIDK}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5050,5700)$ and $q^2 \in \PJpsi \pm 60 \rm MeV/c^{2}s$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/Pi_PIDmu}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/Pi_PIDp}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/Pi_P}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/JPSIREGION/Pi_PT}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + + + + + + + +%%%%%%%%%%%%%%%%%%% + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5370,5700)$ and $q^2 \in [0.1,19] -c\bar{c}$\\ +\ARROW Difference in number of events: $0.4\%$.\\ + +\begin{center} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/BACKGROUNDREGION/B0_DiraAngle}.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{{images/BACKGROUNDREGION/B0_ENDVERTEX_CHI2}.pdf} +\end{center} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5370,5700)$ and $q^2 \in [0.1,19] -c\bar{c}$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/B0_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/B0_IP_OWNPV}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/B0_M}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/B0_P}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5370,5700)$ and $q^2 \in [0.1,19] -c\bar{c}$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/B0_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/B0_IP_OWNPV}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/B0_M}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/B0_P}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5370,5700)$ and $q^2 \in [0.1,19] -c\bar{c}$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/B0_PT}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/J_psi_M}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/K_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/K_PIDK}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5370,5700)$ and $q^2 \in [0.1,19] -c\bar{c}$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/K_PIDmu}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/K_PIDp}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/K_P}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/K_PT}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5370,5700)$ and $q^2 \in [0.1,19] -c\bar{c}$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/Kstar_M}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/mu_minus_IPCHI2_OWNPV}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/mu_minus_PIDK}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/mu_minus_PIDmu}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5370,5700)$ and $q^2 \in [0.1,19] -c\bar{c}$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/mu_minus_P}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/mu_minus_PT}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/Pi_IPCHI2_OWNPV}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/Pi_PIDK}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}[c]{Overlap, after aligning} + \begin{minipage}{\textwidth} +\ARROW Fiducial cut: $m_{\PK \Ppi \mu \mu} \in ( 5370,5700)$ and $q^2 \in [0.1,19] -c\bar{c}$\\ + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/Pi_PIDmu}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/Pi_PIDp}.pdf} +\end{center} + + +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/Pi_P}.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{{images/BACKGROUNDREGION/Pi_PT}.pdf} +\end{center} + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + + + +\begin{frame}[c]{Conclusions} + \begin{minipage}{\textwidth} + +\ARROW There is a sub percent difference between the two samples.\\ +\ARROW The difference is constatish in different phase space regions.\\ +\ARROW No obvious cut missing the distributions look ok. + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Kstarmumu_Run2/Overlaps/mchrzasz.toc b/Kstarmumu_Run2/Overlaps/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Kstarmumu_Run2/Overlaps/tikzfeynman.sty b/Kstarmumu_Run2/Overlaps/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Kstarmumu_Run2/Overlaps/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Kstarmumu_Run2/Selection2/images/MagDown_2011_slices.pdf b/Kstarmumu_Run2/Selection2/images/MagDown_2011_slices.pdf new file mode 100644 index 0000000..394ed63 --- /dev/null +++ b/Kstarmumu_Run2/Selection2/images/MagDown_2011_slices.pdf Binary files differ diff --git a/Kstarmumu_Run2/Selection2/images/distr_pipt.pdf b/Kstarmumu_Run2/Selection2/images/distr_pipt.pdf new file mode 100644 index 0000000..83f1be7 --- /dev/null +++ b/Kstarmumu_Run2/Selection2/images/distr_pipt.pdf Binary files differ diff --git a/Kstarmumu_Run2/Selection3/Makefile b/Kstarmumu_Run2/Selection3/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Kstarmumu_Run2/Selection3/beamercolorthemeFlip.sty b/Kstarmumu_Run2/Selection3/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Kstarmumu_Run2/Selection3/beamerinnerthemeFlip.sty b/Kstarmumu_Run2/Selection3/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Kstarmumu_Run2/Selection3/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Kstarmumu_Run2/Selection3/beamerouterthemeFlip.sty b/Kstarmumu_Run2/Selection3/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Kstarmumu_Run2/Selection3/beamerouterthemedecolines.sty b/Kstarmumu_Run2/Selection3/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Kstarmumu_Run2/Selection3/beamerthemeFlip.sty b/Kstarmumu_Run2/Selection3/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Kstarmumu_Run2/Selection3/images/.DS_Store b/Kstarmumu_Run2/Selection3/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/.DS_Store Binary files differ diff --git a/Kstarmumu_Run2/Selection3/images/B0_BsMassCut_Pwave_Rez.png b/Kstarmumu_Run2/Selection3/images/B0_BsMassCut_Pwave_Rez.png new file mode 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a/Kstarmumu_Run2/Selection3/images/costhetal_q2_SimpleHLT_LODiMuon.png b/Kstarmumu_Run2/Selection3/images/costhetal_q2_SimpleHLT_LODiMuon.png new file mode 100644 index 0000000..89bb80a --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/costhetal_q2_SimpleHLT_LODiMuon.png Binary files differ diff --git a/Kstarmumu_Run2/Selection3/images/d.png b/Kstarmumu_Run2/Selection3/images/d.png new file mode 100644 index 0000000..4cb7f24 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/d.png Binary files differ diff --git a/Kstarmumu_Run2/Selection3/images/derotate.sh b/Kstarmumu_Run2/Selection3/images/derotate.sh new file mode 100755 index 0000000..ba653b9 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/derotate.sh @@ -0,0 +1,13 @@ +#!/bin/bash +#FILES=*.pdf +FILES="$(find . -name '*.pdf')" +for f in $FILES +do + echo "Processing $f ..." + gs -sDEVICE=pdfwrite -dCompatibilityLevel=1.4 -dUseCIEColor -dPDFSETTINGS=/printer -dSAFER -dNOPAUSE -dQUIET -dBATCH -sOutputFile="temp.pdf" "$f" + mv temp.pdf "$f" +# pdf2ps "$f" temp.ps +# ps2pdf temp.ps "$f" +# rm temp.ps +done +#rm temp.pdf diff --git a/Kstarmumu_Run2/Selection3/images/dirac.png b/Kstarmumu_Run2/Selection3/images/dirac.png new file mode 100644 index 0000000..6757d18 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/dirac.png Binary files differ diff --git a/Kstarmumu_Run2/Selection3/images/distr_pipt.pdf b/Kstarmumu_Run2/Selection3/images/distr_pipt.pdf new file mode 100644 index 0000000..83f1be7 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/distr_pipt.pdf Binary files differ diff --git a/Kstarmumu_Run2/Selection3/images/effPsi2S.png b/Kstarmumu_Run2/Selection3/images/effPsi2S.png new file mode 100644 index 0000000..e683700 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/effPsi2S.png Binary files differ diff --git a/Kstarmumu_Run2/Selection3/images/effPsi2S2.png b/Kstarmumu_Run2/Selection3/images/effPsi2S2.png new file mode 100644 index 0000000..7ac4da9 --- /dev/null +++ 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differ diff --git a/Kstarmumu_Run2/Selection3/images/espen3.png b/Kstarmumu_Run2/Selection3/images/espen3.png new file mode 100644 index 0000000..419cc5f --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/espen3.png Binary files differ diff --git a/Kstarmumu_Run2/Selection3/images/getFromAFS.sh b/Kstarmumu_Run2/Selection3/images/getFromAFS.sh new file mode 100644 index 0000000..7d73a4a --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/getFromAFS.sh @@ -0,0 +1,4 @@ +kinit egraveri@CERN.CH +aklog +cp -r /afs/cern.ch/user/e/egraveri/cmtuser/STMonitoring/NewTTAlignment/Out/Plots/AlignVSSimCond-D0Align ./img/ +cp -r /afs/cern.ch/user/e/egraveri/cmtuser/STMonitoring/NewTTAlignment/Out/Plots/AlignVSSimCond-D0AlignNoTT ./img/ diff --git a/Kstarmumu_Run2/Selection3/images/index.png b/Kstarmumu_Run2/Selection3/images/index.png new file mode 100644 index 0000000..f51cd9d --- /dev/null +++ b/Kstarmumu_Run2/Selection3/images/index.png Binary files differ diff --git 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+%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} %for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +%\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} +\usepackage{hepparticles} +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + +\author{ {M.Chrzaszcz~A.Mauri~R.Coutinho} (UZH)} +\institute{UZH} +\title[$\PBzero \to \PKstar \Pmuon \APmuon$ Update]{$\PBzero \to \PKstar \Pmuon \APmuon$ Update} +\date{30 January 2017} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright\bfseries \Huge {$\PBzero \to \PKstar \Pmuon \APmuon$\\ Selection Update} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} { \large Marcin Chrzaszcz\\\vspace{-0.1em} \large Andrea Mauri\\\vspace{-0.1em} \large Rafael Silva Coutinho\\\vspace{-0.1em} } + +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=1.3cm]{uzh-transp} +\end{column} +\end{columns} +\vspace{0.2em} +with input from Eluned Anne Smith\\ + +\vspace{1em} + +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{$\PBzero \to \PKstar \Pmuon \APmuon$ meeting, CERN\\February 28, 2017} +\end{center} +\end{frame} +} + +\begin{frame}\frametitle{Topics on discussion} + +\begin{enumerate} +\item Trigger +\item Data/MC corrections +\item BDT training +\item PID re sampling +\item Exotic pollutions to $\PB \to \PKstar \PJpsi$. + +\item VARIA +\end{enumerate} + + + +\end{frame} + + + + + + + + + + + +\begin{frame}\frametitle{Trigger efficiencies \texttt{L0Muon}} + +\ARROW We studied the trigger efficiency on Run2 MC.\\ + +\begin{tabular}{l||c|c} +\hline +Name & Absolute $\epsilon$ & Relative $\epsilon$\\ \hline +\texttt{L0Muon} & $78.1065~\%$ & -------- \\ \hline \hline +\texttt{Hlt1TrackMVA} & $74.5579\%$ & $95.4568\%$\\ +\texttt{Hlt1TwoTrackMVA} & $76.7186\%$ & $98.2231\%$\\ +\texttt{Hlt1TrackMuon} & $77.2776\%$ & $98.9388\%$\\ +\texttt{Hlt1DiMuonLowMass} & $77.4331\%$ & $99.1379\%$ \\ +\texttt{Hlt1SingleMuonHighPT } & $77.4436\%$ & $99.1513\%$ \\ +\texttt{Hlt1DiMuonHighMass} & $ 77.4518\%$ & $99.1619\%$\\ +\texttt{Hlt1TrackMVALoose} & $ 77.4518\%$ & $99.1619\%$\\ +\texttt{Hlt1TwoTrackMVALoose} & $ 77.4518\%$ & $99.1619\%$\\ \hline \hline + + +\end{tabular} + + +\end{frame} + + + + +\begin{frame}\frametitle{Trigger efficiencies \texttt{L0Muon}} + +\ARROW We studied the trigger efficiency on Run2 MC.\\ + +\begin{tabular}{l||c|c} +\hline +Name & Absolute $\epsilon$ & Relative $\epsilon$\\ \hline + +\texttt{Hlt2TopoMu2BodyBBDT} & $70.296\%$ & $90.7609\%$\\ +\texttt{Hlt2DiMuonDetached} & $73.9044\%$ & $95.4198\%$\\ +\texttt{Hlt2Topo3BodyBBDT} & $75.2972\%$ & $97.2181\%$\\ +\texttt{Hlt2SingleMuon} & $75.9356\%$ & $98.0424\%$\\ +\texttt{Hlt2Topo2BodyBBDT} & $76.0233 \%$ & $98.1556\%$\\ +\texttt{Hlt2TopoMuMu2BodyBBDT} & $76.0794 \%$ & $98.228\%$\\ +\texttt{Hlt2TopoMu3BodyBBDT } & $76.0986 \%$ & $98.2528\%$\\ +\texttt{Hlt2TopoMuMu4BodyBBDT} & $76.1101 \%$ & $98.2677\%$\\ +\texttt{Hlt2TopoMuMu3BodyBBDT} & $76.1156 \%$ & $98.2748\%$\\ +\texttt{Hlt2SingleMuonHighPT} & $76.125 \%$ & $98.2869\%$\\ +\texttt{Hlt2SingleMuonRare} & $76.1288 \%$ & $98.2918\%$\\ +\texttt{Hlt2Topo4BodyBBDT } & $76.1291 \%$ & $98.2922\%$\\ +\texttt{Hlt2TopoMu4BodyBBDT } & $76.1291\%$ & $98.2922\%$\\ +\texttt{Hlt2SingleMuonLowPT } & $76.1291\%$ & $98.2922\%$\\ + + +\end{tabular} + + +\end{frame} + +%%%%% Here we put flatness + +\begin{frame}\frametitle{Trigger efficiencies \texttt{L0Muon}} + + +\includegraphics[width=0.45\textwidth]{images/costhetak_LOMuon.png} +\includegraphics[width=0.45\textwidth]{images/costhetal_LOMuon.png}\\ +\includegraphics[width=0.45\textwidth]{images/phi_LOMuon.png} +\includegraphics[width=0.45\textwidth]{images/q2_LOMuon.png}\\ + +\end{frame} + + + +\begin{frame}\frametitle{Trigger efficiencies \texttt{L0Muon}$\Vert $\texttt{L0DiMuon}} + +\ARROW We studied the trigger efficiency on Run2 MC.\\ + +\begin{tabular}{l||c|c} +\hline +Name & Absolute $\epsilon$ & Relative $\epsilon$\\ \hline +\texttt{L0Muon}$\Vert $\texttt{L0DiMuon} & $81.5517~\%$ & -------- \\ \hline \hline + +\texttt{Hlt1TrackMVA} & $77.7613\%$ & $95.3522\%$\\ +\texttt{Hlt1TwoTrackMVA} & $80.0632\%$ & $98.1748\%$\\ +\texttt{Hlt1TrackMuon} & $80.6849\%$ & $98.9371\%$\\ +\texttt{Hlt1SingleMuonHighPT} & $80.7013\%$ & $98.9573\%$ \\ +\texttt{Hlt1DiMuonLowMass } & $80.8558\%$ & $99.1467\%$ \\ +\texttt{Hlt1DiMuonHighMass } & $80.864\%$ & $99.1568\%$ \\ +\texttt{Hlt1TrackMVALoose} & $ 80.864 \%$ & $99.1568\%$\\ +\texttt{Hlt1TwoTrackMVALoose} & $ 80.864\%$ & $99.1568\%$\\ + +\end{tabular} + + +\end{frame} + + +\begin{frame}\frametitle{Trigger efficiencies \texttt{L0Muon}$\Vert $\texttt{L0DiMuon}} + +\ARROW We studied the trigger efficiency on Run2 MC.\\ + +\begin{tabular}{l||c|c} +\hline +Name & Absolute $\epsilon$ & Relative $\epsilon$\\ \hline + +\texttt{Hlt2TopoMu2BodyBBDT} & $73.269\%$ & $90.6077\%$\\ +\texttt{Hlt2DiMuonDetached} & $77.1023\%$ & $95.348\%$\\ +\texttt{Hlt2Topo3BodyBBDT} & $78.5627 \%$ & $97.154\%$\\ +\texttt{Hlt2SingleMuon} & $79.2459\%$ & $97.9989\%$\\ +\texttt{Hlt2Topo2BodyBBDT} & $79.3382\%$ & $98.1131\%$\\ +\texttt{Hlt2TopoMuMu2BodyBBDT}& $ 79.3965\%$ & $98.1852\%$\\ +\texttt{Hlt2TopoMu3BodyBBDT} & $79.4168\%$ & $98.2103\%$\\ +\texttt{Hlt2TopoMuMu4BodyBBDT} & $79.43\%$ & $98.2266\%$\\ +\texttt{Hlt2SingleMuonHighPT} & $79.4394\%$ & $98.2382\%$\\ +\texttt{Hlt2TopoMuMu3BodyBBDT} & $79.4454 \%$ & $98.2456\%$\\ +\texttt{Hlt2SingleMuonRare} & $79.4493 \%$ & $98.2504\%$\\ +\texttt{Hlt2Topo4BodyBBDT} & $79.4495 \%$ & $98.2507\%$\\ +\texttt{Hlt2TopoMu4BodyBBDT} & $79.4495 \%$ & $98.2507\%$\\ +\texttt{Hlt2SingleMuonLowPT} & $79.4496 \%$ & $98.2508\%$\\ + + + + +\end{tabular} + + +\end{frame} + + +\begin{frame}\frametitle{Trigger efficiencies \texttt{L0Muon}$\Vert $\texttt{L0DiMuon}} + + +\includegraphics[width=0.45\textwidth]{images/costhetak_LODiMuon.png} +\includegraphics[width=0.45\textwidth]{images/costhetal_LODiMuon.png}\\ +\includegraphics[width=0.45\textwidth]{images/phi_LODiMuon.png} +\includegraphics[width=0.45\textwidth]{images/q2_LODiMuon.png}\\ + +\end{frame} + + + + + + +\begin{frame}\frametitle{Trigger validation on the $\PB \to \PKstar \PJpsi$} + +\includegraphics[width=0.95\textwidth]{images/effjpsi.png} + + + + + +\end{frame} + + + +\begin{frame}\frametitle{Trigger validation on the $\PB \to \PKstar \PJpsi$} + +\includegraphics[width=0.95\textwidth]{images/effjpsi2.png} + + + + + +\end{frame} + + + + +\begin{frame}\frametitle{Trigger validation on the $\PB \to \PKstar \Ppsi(2S)$} + + +\includegraphics[width=0.95\textwidth]{images/effPsi2S.png} + + + +\end{frame} + +\begin{frame}\frametitle{Trigger validation on the $\PB \to \PKstar \Ppsi(2S)$} + + +\includegraphics[width=0.95\textwidth]{images/effPsi2S.png} + + + +\end{frame} + + +\begin{frame}\frametitle{Trigger Summary} + +\ARROW We propose: +\texttt{L0Muon} $\Vert$ \texttt{L0DiMuon}\\ +\texttt{Hlt1TrackMVA}, \texttt{Hlt1TwoTrackMVA}, \texttt{Hlt1TrackMuon}\\ +\texttt{Hlt2TopoMu2BodyBBDT}, \texttt{Hlt2DiMuonDetached}, \texttt{Hlt2Topo3BodyBBDT}, \texttt{Hlt2SingleMuon}, \texttt{Hlt2Topo2BodyBBDT}\\ +\ARROW Simplifies life, unifies the selection for 2015 and 2016 and keeps the same efficiency.\\ +\ARROW Eluned found same results with her independent studies. \\ +\ARROW Total numbers: +\begin{tabular}{|l|c|c|} + \hline +L0 & Simple HLT & Full HLT\\ \hline \hline +\texttt{L0Muon} & $76.41\%$ & $76.64\%$\\ +\texttt{L0Muon} & $79.77\%$ & $80.00\%$\\ \hline +\end{tabular} + + + + + +\end{frame} + +\iffalse + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}\frametitle{Data MC corrections} + +\ARROW There are now two standard ways how to correct the MC: +\begin{enumerate} +\item Adaptive reweighing. +\item N-dim histogram reweighing. +\item BDT - reweighing. +\end{enumerate} + + + +\end{frame} + +\fi +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +\begin{frame}\frametitle{Data/MC corrections 2} + +\ARROW Our biggest systematic came from the $\Ppi$ $p_T$ spectrum.\\ +\ARROW Lets get rid of this issue:)\\ +\ARROW The idea is the following: we compare our p-wave MC with what we have in data.\\ +\ARROW What I did is to compute the weight: real model / pwave model.\\ +\ARROW I then apply the weight to our MC and compare with data.\\ +\end{frame} + + +\begin{frame}\frametitle{Data/MC corrections 2} + +\begin{center} +\includegraphics[width=0.99\textwidth]{images/Pi_PT.png} +\end{center} + +\end{frame} + +\begin{frame}\frametitle{Data/MC corrections 2} + +\begin{center} +\includegraphics[width=0.99\textwidth]{images/K_PT.png} +\end{center} + +\end{frame} + +\begin{frame}\frametitle{Data/MC corrections 2} + +\begin{center} +\includegraphics[width=0.45\textwidth]{images/mu_minus_PT.png}\\ +\includegraphics[width=0.45\textwidth]{images/mu_plus_PT.png} + +\end{center} + +\end{frame} + + + + +\begin{frame}\frametitle{Meerkat- PID corrections} + +\ARROW We have made first PID corrections using Meerkat:\\ +\begin{center} +\includegraphics[width=0.45\textwidth]{images/Pi_PIDK.png} +\includegraphics[width=0.45\textwidth]{images/K_PIDK.png}\\ +\includegraphics[width=0.45\textwidth]{images/Pi_PIDp.png} +\includegraphics[width=0.45\textwidth]{images/K_PIDp.png} + +\end{center} +\ARROW We are still missing the muon re sampling(ongoing).\\ +\ARROW We will cross check with old re sampling. +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +\begin{frame}\frametitle{Angle separation} + +\ARROW Let's see the angle separation between the two tracks: +\begin{center} +\includegraphics[width=0.45\textwidth]{images/angle/phi.png} +\includegraphics[width=0.45\textwidth]{images/angle/phin.png}\\ +\includegraphics[width=0.45\textwidth]{images/angle/q2.png}\includegraphics[width=0.45\textwidth]{images/angle/q2n.png} + +\end{center} + + +\end{frame} + + + +\begin{frame}\frametitle{Angle separation} + +\ARROW Let's see the angle separation between the two tracks: +\begin{center} +\includegraphics[width=0.45\textwidth]{images/angle/costhetak.png} +\includegraphics[width=0.45\textwidth]{images/angle/costhetakn.png}\\ +\includegraphics[width=0.45\textwidth]{images/angle/costhetal.png}\includegraphics[width=0.45\textwidth]{images/angle/costhetaln.png} + +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Angle separation} + +\ARROW Release the $\PK$ $\Ppi$ angle: +\begin{center} +\includegraphics[width=0.45\textwidth]{images/angle2/costhetak.png} +\includegraphics[width=0.45\textwidth]{images/angle2/costhetakn.png}\\ +\includegraphics[width=0.45\textwidth]{images/angle2/costhetal.png}\includegraphics[width=0.45\textwidth]{images/angle2/costhetaln.png} + +\end{center} + + +\end{frame} + + + +\begin{frame}\frametitle{Angle separation} + +\ARROW Release the $\PK$ $\Ppi$ angle and tighter the other angles: +\begin{center} +\includegraphics[width=0.45\textwidth]{images/angle3/costhetak.png} +\includegraphics[width=0.45\textwidth]{images/angle3/costhetakn.png}\\ +\includegraphics[width=0.45\textwidth]{images/angle3/costhetal.png}\includegraphics[width=0.45\textwidth]{images/angle3/costhetaln.png} + +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Angle separation} + +\ARROW Release the $\PK$ $\Ppi$ angle and tighting the other angles: +\begin{center} +\includegraphics[width=0.45\textwidth]{images/angle3/phi.png} +\includegraphics[width=0.45\textwidth]{images/angle3/phin.png}\\ +\includegraphics[width=0.45\textwidth]{images/angle3/q2.png}\includegraphics[width=0.45\textwidth]{images/angle3/q2n.png} + +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{Angle separation} + +\ARROW Everything tighting: +\begin{center} +\includegraphics[width=0.45\textwidth]{images/angle4/costhetak.png} +\includegraphics[width=0.45\textwidth]{images/angle4/costhetakn.png}\\ +\includegraphics[width=0.45\textwidth]{images/angle4/costhetal.png}\includegraphics[width=0.45\textwidth]{images/angle4/costhetaln.png} + +\end{center} + + +\end{frame} +\begin{frame}\frametitle{Angle separation} + +\ARROW Everything tighting: +\begin{center} +\includegraphics[width=0.45\textwidth]{images/angle4/phi.png} +\includegraphics[width=0.45\textwidth]{images/angle4/phin.png}\\ +\includegraphics[width=0.45\textwidth]{images/angle4/q2.png}\includegraphics[width=0.45\textwidth]{images/angle4/q2n.png} + +\end{center} + + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +\begin{frame}\frametitle{BDT} + +\ARROW We have started to train the BDT.\\ +\ARROW For now we used MC PHSP as signal and side-bands.\\ +\ARROW Variables: +\begin{itemize} +\item \texttt{B0\_ENDVERTEX\_CHI2} +\item \texttt{B0\_IP\_OWNPV} +\item \texttt{B0\_IPCHI2\_OWNPV} +\item \texttt{B0\_FD\_OWNPV} +\item \texttt{B0\_FDCHI2\_OWNPV} +\item \texttt{B0\_P} +\item \texttt{B0\_PT} +\item \texttt{B0\_relinfo\_VTXISOBDTHARDFIRSTVALUE} +\end{itemize} + + + +\end{frame} + + +\begin{frame}\frametitle{BDT ROC} + + +\begin{center} +\includegraphics[width=0.95\textwidth]{images/roc.png} +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{BDT ranking} + + +\begin{center} +\includegraphics[width=0.95\textwidth]{images/index.png} +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Conclusions} + + +\begin{itemize} +\item PID works reasonably well, but still needs a bit of work. +\item To fully test the BDT we need the re sampled MC. +\item I think we can fix the preselection today. +\item Trigger study performed. +\item Discrepancy on the \texttt{Pi\_PT} fixed and others are under control. +\end{itemize} + +\end{frame} + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Kstarmumu_Run2/Selection3/mchrzasz.toc b/Kstarmumu_Run2/Selection3/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Kstarmumu_Run2/Selection3/tikzfeynman.sty b/Kstarmumu_Run2/Selection3/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Kstarmumu_Run2/Selection3/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Kstarmumu_Run2/SelectionFINAL/Makefile b/Kstarmumu_Run2/SelectionFINAL/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Kstarmumu_Run2/SelectionFINAL/beamercolorthemeFlip.sty b/Kstarmumu_Run2/SelectionFINAL/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Kstarmumu_Run2/SelectionFINAL/beamerinnerthemeFlip.sty b/Kstarmumu_Run2/SelectionFINAL/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Kstarmumu_Run2/SelectionFINAL/beamerouterthemeFlip.sty b/Kstarmumu_Run2/SelectionFINAL/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Kstarmumu_Run2/SelectionFINAL/beamerouterthemedecolines.sty b/Kstarmumu_Run2/SelectionFINAL/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Kstarmumu_Run2/SelectionFINAL/beamerthemeFlip.sty b/Kstarmumu_Run2/SelectionFINAL/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Kstarmumu_Run2/SelectionFINAL/images/.DS_Store b/Kstarmumu_Run2/SelectionFINAL/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/images/.DS_Store Binary files differ diff --git a/Kstarmumu_Run2/SelectionFINAL/images/BG_both.png b/Kstarmumu_Run2/SelectionFINAL/images/BG_both.png new file mode 100755 index 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http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. 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+\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + +\author{ {Eluned Smith,Marcin Chrzaszcz} (RWTH, CERN)} +\institute{UZH} +\title[$\PBzero \to \PKstar \Pmuon \APmuon$ Update]{$\PBzero \to \PKstar \Pmuon \APmuon$ Update} +\date{30 January 2017} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright\bfseries \Huge {$\PBzero \to \PKstar \Pmuon \APmuon$\\ Finalization} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} { \Large Eluned Smith\\ Marcin Chrzaszcz } + +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=0.7cm]{RWTH.png}\vspace{0.8em} +\includegraphics[height=1.3cm]{cern} + +\end{column} +\end{columns} + +\vspace{1em} + +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{$\PBzero \to \PKstar \Pmuon \APmuon$ meeting, CERN\\January 30, 2018} +\end{center} +\end{frame} +} + + +\begin{frame}[c]{Selection Run1} + + \begin{minipage}{\textwidth} +\ARROW We have independently implemented Run1 selection.\\ +\ARROW Our implementation agrees between us (independent check).\\ +\ARROW There is slightly issue when running the same selection on S21: + +\begin{center} + + +\begin{tabular}{|c|c|} +\hline +S20 $N.~\PBd \to \PKstar \PJpsi$ & $442315$\\ +S21 $N.~\PBd \to \PKstar \PJpsi$ & $429258$\\ \hline +Difference & $2.95~\%$\\ \hline +\end{tabular} +~\\ +{~}\\{~}\\{~}\\ +\begin{exampleblock}{} +We thing the $3\%$ is fine giving that S20 and S21 even having the same cuts have different DDB etc. We saw that this things can cause difference much much higher in previous round. +\end{exampleblock} + + +\end{center} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + +\begin{frame}[c]{The need for MC - improvements} + \begin{minipage}{\textwidth} +\ARROW If you recall in Run1 we had PHSP MC: + \begin{columns} +\column{0.5\textwidth} +\includegraphics[width=0.99\textwidth]{images/q2PHSP.png} + + +\column{0.5\textwidth} + \includegraphics[width=0.99\textwidth]{images/q2.png} + +\end{columns} + +\ARROW More flat makes our life easier and less dirty in terms of reweighing :)\\ +\ARROW Produced 20M events so we can get the correction for small ''nonflatness''. (will give you links at the end). + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\begin{frame}[c]{Selection} + \begin{minipage}{\textwidth} + +\ARROW Normally we have the swap for $J/\psi$:\\ +\texttt{"!((B0\_swapMass>3036) and (B0\_swapMass<3156) and (Pi\_PIDmu>5||Pi\_isMuon==1)) and !((B0\_kmuswapMass>3036) and (B0\_kmuswapMass<3156) or (K\_PIDmu>5||K\_isMuon==1))”} +\ARROW For Run2 we added the same for the $\psi(2S)$:\\{~}\\ +\begin{columns} +\column{0.33\textwidth} +\includegraphics[width=0.95\textwidth]{images/espen1.png} +\column{0.33\textwidth} +\includegraphics[width=0.95\textwidth]{images/espen2.png} +\column{0.33\textwidth} +\includegraphics[width=0.95\textwidth]{images/espen3.png} + +\end{columns} + + +\ARROW Impact for the Pwave analysis minimal but let's veto just to be sure :)\\ + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + +\begin{frame}[c]{Location} + \begin{minipage}{\textwidth} + +\ARROW the ntuples after the selection can be found:\\ +\url{/eos/lhcb/wg/RD/Bd2Kstmumu/data_reduced} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} + + + + + + + + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Kstarmumu_Run2/SelectionFINAL/mchrzasz.toc b/Kstarmumu_Run2/SelectionFINAL/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Kstarmumu_Run2/SelectionFINAL/overlaps.pdf b/Kstarmumu_Run2/SelectionFINAL/overlaps.pdf new file mode 100644 index 0000000..600dbe3 --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/overlaps.pdf Binary files differ diff --git a/Kstarmumu_Run2/SelectionFINAL/tikzfeynman.sty b/Kstarmumu_Run2/SelectionFINAL/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Kstarmumu_Run2/SelectionFINAL/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Magnet_Stations/11_10_2018_OPG/ClosedOT_halffield.eps 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119 786 m -5 -1 d -3 -5 d -1 -7 d -5 Y 1 -7 d 3 -5 d 5 -1 d 3 X 4 1 d + 3 5 d 2 7 d 5 Y -2 7 d -3 5 d -4 1 d -3 X cl s 120 788 m -4 -2 d -3 -4 d -2 -8 + d -5 Y 2 -7 d 3 -5 d 4 -1 d 3 X 5 1 d 3 5 d 1 7 d 5 Y -1 8 d -3 4 d -5 2 d -3 X + cl s 118 786 m -4 -1 d -3 -5 d -2 -8 d -4 Y 2 -8 d 3 -4 d 4 -2 d 4 X 4 2 d 3 4 + d 2 8 d 4 Y -2 8 d -3 5 d -4 1 d -4 X cl s 120 788 m -4 -2 d -3 -4 d -2 -8 d -4 + Y 2 -8 d 3 -4 d 4 -2 d 3 X 5 2 d 3 4 d 1 8 d 4 Y -1 8 d -3 4 d -5 2 d -3 X cl s + 118 786 m -4 -2 d -3 -4 d -2 -8 d -4 Y 2 -8 d 3 -5 d 4 -1 d 3 X 5 1 d 3 5 d 1 8 + d 4 Y -1 8 d -3 4 d -5 2 d -3 X cl s 121 788 m -5 -1 d -3 -5 d -1 -7 d -5 Y 1 + -7 d 3 -5 d 5 -1 d 3 X 4 1 d 3 5 d 2 7 d 5 Y -2 7 d -3 5 d -4 1 d -3 X cl s 144 + 758 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 143 758 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl + s 144 759 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 143 758 m -2 -2 d 2 -1 d 2 1 d -2 + 2 d cl s 144 759 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 143 757 m -2 -1 d 2 -2 d 1 + 2 d -1 1 d cl s 145 759 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 142 757 m -1 -2 d 1 + -1 d 2 1 d -2 2 d cl s 145 760 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 163 787 m -4 + -2 d -2 -3 d -3 Y 2 -3 d 3 -1 d 6 -2 d 4 -1 d 3 -3 d 2 -3 d -5 Y -2 -3 d -1 -1 + d -5 -2 d -6 X -4 2 d -2 1 d -1 3 d 5 Y 1 3 d 3 3 d 5 1 d 6 2 d 3 1 d 1 3 d 3 Y + -1 3 d -5 2 d -6 X cl s 163 787 m -5 -2 d -1 -3 d -3 Y 1 -3 d 3 -1 d 7 -2 d 4 + -1 d 3 -3 d 2 -3 d -5 Y -2 -3 d -1 -2 d -5 -1 d -6 X -5 1 d -1 2 d -2 3 d 5 Y 2 + 3 d 3 3 d 4 1 d 7 2 d 3 1 d 1 3 d 3 Y -1 3 d -5 2 d -6 X cl s 164 787 m -5 -1 d + -1 -3 d -3 Y 1 -3 d 3 -2 d 6 -1 d 5 -2 d 3 -3 d 1 -3 d -4 Y -1 -3 d -2 -2 d -4 + -1 d -6 X -5 1 d -1 2 d -2 3 d 4 Y 2 3 d 3 3 d 4 2 d 6 1 d 3 2 d 2 3 d 3 Y -2 3 + d -4 1 d -6 X cl s 163 786 m -5 -1 d -1 -3 d -3 Y 1 -3 d 3 -2 d 6 -1 d 5 -2 d 3 + -3 d 1 -3 d -4 Y -1 -3 d -2 -2 d -4 -1 d -6 X -5 1 d -1 2 d -2 3 d 4 Y 2 3 d 3 + 3 d 4 2 d 6 1 d 3 2 d 2 3 d 3 Y -2 3 d -4 1 d -6 X cl s 164 788 m -5 -2 d -1 -3 + d -3 Y 1 -3 d 3 -1 d 6 -2 d 5 -1 d 3 -4 d 2 -3 d -4 Y -2 -3 d -1 -2 d -5 -1 d + -6 X -5 1 d -1 2 d -2 3 d 4 Y 2 3 d 3 4 d 4 1 d 6 2 d 4 1 d 1 3 d 3 Y -1 3 d -5 + 2 d -6 X cl s 162 786 m -4 -1 d -2 -3 d -4 Y 2 -3 d 3 -1 d 6 -2 d 4 -1 d 3 -3 d + 2 -3 d -5 Y -2 -3 d -1 -1 d -5 -2 d -6 X -4 2 d -2 1 d -1 3 d 5 Y 1 3 d 3 3 d 5 + 1 d 6 2 d 3 1 d 1 3 d 4 Y -1 3 d -5 1 d -6 X cl s 164 788 m -4 -2 d -2 -3 d -3 + Y 2 -3 d 3 -1 d 6 -2 d 4 -1 d 3 -3 d 2 -3 d -5 Y -2 -3 d -1 -1 d -5 -2 d -6 X + -4 2 d -2 1 d -1 3 d 5 Y 1 3 d 3 3 d 5 1 d 6 2 d 3 1 d 1 3 d 3 Y -1 3 d -5 2 d + -6 X cl s 162 786 m -5 -2 d -1 -3 d -3 Y 1 -3 d 4 -1 d 6 -2 d 4 -1 d 3 -3 d 2 + -3 d -5 Y -2 -3 d -1 -2 d -5 -1 d -6 X -5 1 d -1 2 d -2 3 d 5 Y 2 3 d 3 3 d 5 1 + d 6 2 d 3 1 d 1 3 d 3 Y -1 3 d -5 2 d -6 X cl s 165 788 m -5 -1 d -1 -3 d -3 Y + 1 -3 d 3 -2 d 6 -1 d 5 -2 d 3 -3 d 1 -3 d -4 Y -1 -3 d -2 -2 d -4 -1 d -6 X -5 + 1 d -1 2 d -2 3 d 4 Y 2 3 d 3 3 d 4 2 d 6 1 d 3 2 d 2 3 d 3 Y -2 3 d -4 1 d -6 + X cl s 160 988 m 3 2 d 5 4 d -31 Y s 160 988 m 3 2 d 5 4 d -32 Y s 161 989 m 3 + 1 d 4 5 d -32 Y s 160 988 m 3 1 d 4 5 d -32 Y s 161 989 m 3 1 d 4 5 d -32 Y s + 159 987 m 3 2 d 5 4 d -31 Y s 161 989 m 3 2 d 5 4 d -31 Y s 159 987 m 3 2 d 5 4 + d -32 Y s 162 990 m 3 1 d 4 5 d -32 Y s 115 1196 m 3 1 d 4 5 d -32 Y s 115 1195 + m 3 2 d 4 4 d -31 Y s 115 1196 m 3 1 d 5 5 d -32 Y s 114 1195 m 3 2 d 5 4 d -32 + Y s 116 1196 m 3 2 d 4 4 d -31 Y s 114 1195 m 3 1 d 5 5 d -32 Y s 116 1197 m 3 + 1 d 4 5 d -32 Y s 114 1194 m 3 2 d 4 4 d -31 Y s 116 1197 m 3 1 d 5 5 d -32 Y s + 144 1173 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 143 1173 m -1 -2 d 1 -1 d 2 1 d -2 + 2 d cl s 144 1173 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 143 1172 m -2 -1 d 2 -2 d + 2 2 d -2 1 d cl s 144 1174 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 143 1172 m -2 -1 + d 2 -2 d 1 2 d -1 1 d cl s 145 1174 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 142 1172 + m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 145 1174 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s + 157 1194 m 2 Y 2 3 d 1 1 d 3 2 d 6 X 3 -2 d 2 -1 d 1 -3 d -3 Y -1 -3 d -3 -5 d + -15 -15 d 21 X s 157 1194 m 1 Y 1 3 d 2 2 d 3 1 d 6 X 3 -1 d 2 -2 d 1 -3 d -3 Y + -1 -3 d -3 -4 d -16 -15 d 22 X s 158 1194 m 2 Y 1 3 d 2 2 d 3 1 d 6 X 3 -1 d 1 + -2 d 2 -3 d -3 Y -2 -3 d -3 -5 d -15 -15 d 21 X s 157 1194 m 1 Y 1 3 d 2 2 d 3 + 1 d 6 X 3 -1 d 1 -2 d 2 -3 d -3 Y -2 -3 d -3 -5 d -15 -15 d 21 X s 158 1195 m 1 + Y 1 3 d 2 2 d 3 1 d 6 X 3 -1 d 2 -2 d 1 -3 d -3 Y -1 -3 d -4 -4 d -15 -15 d 22 + X s 156 1193 m 2 Y 2 3 d 1 1 d 3 2 d 6 X 3 -2 d 2 -1 d 1 -3 d -3 Y -1 -3 d -3 + -5 d -15 -15 d 21 X s 158 1195 m 2 Y 2 3 d 1 1 d 3 2 d 6 X 3 -2 d 2 -1 d 1 -3 d + -3 Y -1 -3 d -3 -5 d -15 -15 d 21 X s 156 1193 m 1 Y 1 3 d 2 2 d 3 1 d 6 X 3 -1 + d 2 -2 d 1 -3 d -3 Y -1 -3 d -3 -4 d -16 -15 d 22 X s 159 1195 m 2 Y 1 3 d 2 1 + d 3 2 d 6 X 3 -2 d 1 -1 d 2 -3 d -3 Y -2 -3 d -3 -5 d -15 -15 d 21 X s 115 1403 + m 3 2 d 4 4 d -32 Y s 115 1403 m 3 1 d 4 5 d -32 Y s 115 1403 m 3 2 d 5 4 d -31 + Y s 114 1402 m 3 2 d 5 4 d -31 Y s 116 1404 m 3 1 d 4 5 d -32 Y s 114 1402 m 3 + 2 d 5 4 d -32 Y s 116 1404 m 3 1 d 4 5 d -32 Y s 114 1402 m 3 1 d 4 5 d -32 Y s + 116 1404 m 3 2 d 5 4 d -31 Y s 144 1380 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 143 + 1380 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 144 1381 m -2 -2 d 2 -1 d 1 1 d -1 2 d + cl s 143 1380 m -2 -2 d 2 -1 d 2 1 d -2 2 d cl s 144 1381 m -1 -2 d 1 -1 d 2 1 + d -2 2 d cl s 143 1379 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 145 1381 m -2 -1 d 2 + -2 d 1 2 d -1 1 d cl s 142 1379 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 145 1382 m + -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 171 1409 m -15 -21 d 22 X s 171 1409 m -16 -21 + d 23 X s 171 1409 m -15 -21 d 23 X s 170 1408 m -15 -21 d 23 X s 171 1410 m -15 + -21 d 23 X s 170 1408 m -15 -21 d 22 X s 172 1410 m -15 -21 d 22 X s 170 1408 m + -16 -21 d 23 X s 172 1410 m -15 -21 d 23 X s 171 1409 m -32 Y s 171 1409 m -32 + Y s 171 1409 m -31 Y s 170 1408 m -31 Y s 171 1410 m -32 Y s 170 1408 m -32 Y s + 172 1410 m -32 Y s 170 1408 m -32 Y s 172 1410 m -31 Y s 115 1610 m 3 2 d 4 4 d + -31 Y s 115 1610 m 3 2 d 4 4 d -32 Y s 115 1611 m 3 1 d 5 5 d -32 Y s 114 1610 + m 3 1 d 5 5 d -32 Y s 116 1611 m 3 2 d 4 4 d -32 Y s 114 1609 m 3 2 d 5 4 d -31 + Y s 116 1611 m 3 2 d 4 4 d -31 Y s 114 1609 m 3 2 d 4 4 d -32 Y s 116 1612 m 3 + 1 d 5 5 d -32 Y s 144 1588 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 143 1587 m -1 -1 + d 1 -2 d 2 2 d -2 1 d cl s 144 1588 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 143 1587 + m -2 -1 d 2 -2 d 2 2 d -2 1 d cl s 144 1588 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s + 143 1587 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 145 1589 m -2 -2 d 2 -1 d 1 1 d -1 + 2 d cl s 142 1586 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 145 1589 m -2 -2 d 2 -1 d + 1 1 d -1 2 d cl s 175 1612 m -1 3 d -5 1 d -3 X -4 -1 d -3 -5 d -2 -7 d -8 Y 2 + -6 d 3 -3 d 4 -1 d 2 X 4 1 d 3 3 d 2 5 d 1 Y -2 5 d -3 3 d -4 1 d -2 X -4 -1 d + -3 -3 d -2 -5 d s 175 1612 m -1 3 d -5 1 d -3 X -5 -1 d -3 -5 d -1 -7 d -8 Y 1 + -6 d 3 -3 d 5 -2 d 2 X 4 2 d 3 3 d 2 4 d 2 Y -2 4 d -3 4 d -4 1 d -2 X -5 -1 d + -3 -4 d -1 -4 d s 176 1612 m -2 3 d -4 2 d -3 X -5 -2 d -3 -4 d -1 -8 d -7 Y 1 + -6 d 3 -3 d 5 -2 d 1 X 5 2 d 3 3 d 1 4 d 2 Y -1 4 d -3 3 d -5 2 d -1 X -5 -2 d + -3 -3 d -1 -4 d s 175 1611 m -2 3 d -4 2 d -3 X -5 -2 d -3 -4 d -1 -8 d -7 Y 1 + -6 d 3 -3 d 5 -2 d 1 X 5 2 d 3 3 d 1 4 d 2 Y -1 4 d -3 3 d -5 2 d -1 X -5 -2 d + -3 -3 d -1 -4 d s 176 1613 m -1 3 d -5 1 d -3 X -5 -1 d -3 -5 d -1 -8 d -7 Y 1 + -6 d 3 -3 d 5 -2 d 1 X 5 2 d 3 3 d 2 4 d 2 Y -2 4 d -3 3 d -5 2 d -1 X -5 -2 d + -3 -3 d -1 -4 d s 174 1611 m -1 3 d -5 1 d -3 X -4 -1 d -3 -5 d -2 -7 d -8 Y 2 + -6 d 3 -3 d 4 -1 d 2 X 4 1 d 3 3 d 2 5 d 1 Y -2 5 d -3 3 d -4 1 d -2 X -4 -1 d + -3 -3 d -2 -5 d s 176 1613 m -1 3 d -5 1 d -3 X -4 -1 d -3 -5 d -2 -7 d -8 Y 2 + -6 d 3 -3 d 4 -1 d 2 X 4 1 d 3 3 d 2 5 d 1 Y -2 5 d -3 3 d -4 1 d -2 X -4 -1 d + -3 -3 d -2 -5 d s 174 1611 m -1 3 d -5 1 d -3 X -4 -1 d -4 -5 d -1 -7 d -8 Y 1 + -6 d 4 -3 d 4 -2 d 2 X 4 2 d 3 3 d 2 4 d 2 Y -2 5 d -3 3 d -4 1 d -2 X -4 -1 d + -4 -3 d -1 -5 d s 177 1613 m -2 3 d -4 2 d -3 X -5 -2 d -3 -4 d -1 -8 d -7 Y 1 + -7 d 3 -3 d 5 -1 d 1 X 5 1 d 3 3 d 1 5 d 2 Y -1 4 d -3 3 d -5 2 d -1 X -5 -2 d + -3 -3 d -1 -4 d s 115 1818 m 3 1 d 4 5 d -32 Y s 115 1817 m 3 2 d 4 4 d -31 Y s + 115 1818 m 3 2 d 5 4 d -32 Y s 114 1817 m 3 2 d 5 4 d -32 Y s 116 1818 m 3 2 d + 4 4 d -31 Y s 114 1817 m 3 1 d 5 5 d -32 Y s 116 1819 m 3 1 d 4 5 d -32 Y s 114 + 1816 m 3 2 d 4 5 d -32 Y s 116 1819 m 3 2 d 5 4 d -32 Y s 144 1795 m -2 -1 d 2 + -2 d 1 2 d -1 1 d cl s 143 1795 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 144 1795 m + -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 143 1794 m -2 -1 d 2 -2 d 2 2 d -2 1 d cl s + 144 1796 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 143 1794 m -2 -1 d 2 -2 d 1 2 d -1 + 1 d cl s 145 1796 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 142 1794 m -1 -2 d 1 -1 d + 2 1 d -2 2 d cl s 145 1796 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 163 1824 m -4 -2 + d -2 -3 d -3 Y 2 -3 d 3 -1 d 6 -2 d 4 -1 d 3 -3 d 2 -3 d -5 Y -2 -3 d -1 -1 d + -5 -2 d -6 X -4 2 d -2 1 d -1 3 d 5 Y 1 3 d 3 3 d 5 1 d 6 2 d 3 1 d 1 3 d 3 Y + -1 3 d -5 2 d -6 X cl s 163 1823 m -5 -1 d -1 -3 d -3 Y 1 -3 d 3 -2 d 7 -1 d 4 + -2 d 3 -3 d 2 -3 d -4 Y -2 -3 d -1 -2 d -5 -1 d -6 X -5 1 d -1 2 d -2 3 d 4 Y 2 + 3 d 3 3 d 4 2 d 7 1 d 3 2 d 1 3 d 3 Y -1 3 d -5 1 d -6 X cl s 164 1824 m -5 -1 + d -1 -3 d -3 Y 1 -3 d 3 -2 d 6 -1 d 5 -2 d 3 -3 d 1 -3 d -5 Y -1 -3 d -2 -1 d + -4 -2 d -6 X -5 2 d -1 1 d -2 3 d 5 Y 2 3 d 3 3 d 4 2 d 6 1 d 3 2 d 2 3 d 3 Y + -2 3 d -4 1 d -6 X cl s 163 1823 m -5 -1 d -1 -3 d -3 Y 1 -3 d 3 -2 d 6 -1 d 5 + -2 d 3 -3 d 1 -3 d -5 Y -1 -3 d -2 -1 d -4 -2 d -6 X -5 2 d -1 1 d -2 3 d 5 Y 2 + 3 d 3 3 d 4 2 d 6 1 d 3 2 d 2 3 d 3 Y -2 3 d -4 1 d -6 X cl s 164 1824 m -5 -1 + d -1 -3 d -3 Y 1 -3 d 3 -2 d 6 -1 d 5 -2 d 3 -3 d 2 -3 d -4 Y -2 -3 d -1 -2 d + -5 -1 d -6 X -5 1 d -1 2 d -2 3 d 4 Y 2 3 d 3 3 d 4 2 d 6 1 d 4 2 d 1 3 d 3 Y + -1 3 d -5 1 d -6 X cl s 162 1823 m -4 -2 d -2 -3 d -3 Y 2 -3 d 3 -1 d 6 -2 d 4 + -1 d 3 -3 d 2 -3 d -5 Y -2 -3 d -1 -1 d -5 -2 d -6 X -4 2 d -2 1 d -1 3 d 5 Y 1 + 3 d 3 3 d 5 1 d 6 2 d 3 1 d 1 3 d 3 Y -1 3 d -5 2 d -6 X cl s 164 1825 m -4 -2 + d -2 -3 d -3 Y 2 -3 d 3 -1 d 6 -2 d 4 -1 d 3 -3 d 2 -3 d -5 Y -2 -3 d -1 -1 d + -5 -2 d -6 X -4 2 d -2 1 d -1 3 d 5 Y 1 3 d 3 3 d 5 1 d 6 2 d 3 1 d 1 3 d 3 Y + -1 3 d -5 2 d -6 X cl s 162 1823 m -5 -2 d -1 -3 d -3 Y 1 -3 d 4 -2 d 6 -1 d 4 + -2 d 3 -3 d 2 -3 d -4 Y -2 -3 d -1 -2 d -5 -1 d -6 X -5 1 d -1 2 d -2 3 d 4 Y 2 + 3 d 3 3 d 5 2 d 6 1 d 3 2 d 1 3 d 3 Y -1 3 d -5 2 d -6 X cl s 165 1825 m -5 -1 + d -1 -3 d -3 Y 1 -4 d 3 -1 d 6 -2 d 5 -1 d 3 -3 d 1 -3 d -5 Y -1 -3 d -2 -1 d + -4 -2 d -6 X -5 2 d -1 1 d -2 3 d 5 Y 2 3 d 3 3 d 4 1 d 6 2 d 3 1 d 2 4 d 3 Y + -2 3 d -4 1 d -6 X cl s 157 2024 m 1 Y 2 3 d 1 2 d 3 1 d 6 X 3 -1 d 2 -2 d 1 -3 + d -3 Y -1 -3 d -3 -4 d -15 -16 d 21 X s 157 2023 m 2 Y 1 3 d 2 1 d 3 2 d 6 X 3 + -2 d 2 -1 d 1 -3 d -3 Y -1 -3 d -3 -5 d -16 -15 d 22 X s 158 2024 m 1 Y 1 3 d 2 + 2 d 3 1 d 6 X 3 -1 d 1 -2 d 2 -3 d -3 Y -2 -3 d -3 -4 d -15 -15 d 21 X s 157 + 2023 m 1 Y 1 3 d 2 2 d 3 2 d 6 X 3 -2 d 1 -2 d 2 -3 d -3 Y -2 -3 d -3 -4 d -15 + -15 d 21 X s 158 2024 m 2 Y 1 3 d 2 1 d 3 2 d 6 X 3 -2 d 2 -1 d 1 -3 d -3 Y -1 + -3 d -4 -5 d -15 -15 d 22 X s 156 2023 m 1 Y 2 3 d 1 2 d 3 1 d 6 X 3 -1 d 2 -2 + d 1 -3 d -3 Y -1 -3 d -3 -4 d -15 -16 d 21 X s 158 2025 m 1 Y 2 3 d 1 2 d 3 1 d + 6 X 3 -1 d 2 -2 d 1 -3 d -3 Y -1 -3 d -3 -5 d -15 -15 d 21 X s 156 2022 m 2 Y 1 + 3 d 2 1 d 3 2 d 6 X 3 -2 d 2 -1 d 1 -3 d -3 Y -1 -3 d -3 -5 d -16 -15 d 22 X s + 159 2025 m 1 Y 1 3 d 2 2 d 3 1 d 6 X 3 -1 d 1 -2 d 2 -3 d -3 Y -2 -3 d -3 -4 d + -15 -15 d 21 X s 227 227 m 1814 X s 371 261 m -34 Y s 412 244 m -17 Y s 454 244 + m -17 Y s 495 244 m -17 Y s 536 244 m -17 Y s 577 261 m -34 Y s 619 244 m -17 Y + s 660 244 m -17 Y s 701 244 m -17 Y s 742 244 m -17 Y s 783 261 m -34 Y s 825 + 244 m -17 Y s 866 244 m -17 Y s 907 244 m -17 Y s 948 244 m -17 Y s 990 261 m + -34 Y s 1031 244 m -17 Y s 1072 244 m -17 Y s 1113 244 m -17 Y s 1155 244 m -17 + Y s 1196 261 m -34 Y s 1237 244 m -17 Y s 1278 244 m -17 Y s 1320 244 m -17 Y s + 1361 244 m -17 Y s 1402 261 m -34 Y s 1443 244 m -17 Y s 1485 244 m -17 Y s + 1526 244 m -17 Y s 1567 244 m -17 Y s 1608 261 m -34 Y s 1649 244 m -17 Y s + 1691 244 m -17 Y s 1732 244 m -17 Y s 1773 244 m -17 Y s 1814 261 m -34 Y s + 1856 244 m -17 Y s 1897 244 m -17 Y s 1938 244 m -17 Y s 1979 244 m -17 Y s + 2021 261 m -34 Y s 371 261 m -34 Y s 330 244 m -17 Y s 289 244 m -17 Y s 247 + 244 m -17 Y s 2021 261 m -34 Y s 362 197 m 1 Y 2 3 d 1 2 d 3 1 d 6 X 3 -1 d 2 + -2 d 1 -3 d -3 Y -1 -3 d -3 -5 d -15 -15 d 21 X s 362 196 m 2 Y 1 3 d 2 1 d 3 2 + d 6 X 3 -2 d 1 -1 d 2 -3 d -3 Y -2 -3 d -3 -5 d -15 -15 d 21 X s 362 197 m 1 Y + 2 3 d 1 2 d 3 1 d 6 X 3 -1 d 2 -2 d 2 -3 d -3 Y -2 -3 d -3 -4 d -15 -15 d 21 X + s 361 196 m 1 Y 2 3 d 1 2 d 3 1 d 7 X 3 -1 d 1 -2 d 2 -3 d -3 Y -2 -3 d -3 -4 d + -15 -15 d 21 X s 363 197 m 2 Y 1 3 d 2 1 d 3 2 d 6 X 3 -2 d 1 -1 d 2 -3 d -3 Y + -2 -3 d -3 -5 d -15 -15 d 21 X s 361 196 m 1 Y 2 3 d 1 2 d 3 1 d 6 X 3 -1 d 2 + -2 d 1 -3 d -3 Y -1 -3 d -3 -4 d -15 -16 d 21 X s 363 198 m 1 Y 2 3 d 1 2 d 3 1 + d 6 X 3 -1 d 2 -2 d 1 -3 d -3 Y -1 -3 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3 d s 960 205 + m 17 X -9 -12 d 4 X 3 -2 d 2 -1 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 + d -1 1 d -2 3 d s 958 203 m 17 X -9 -12 d 5 X 3 -1 d 1 -2 d 2 -4 d -4 Y -2 -4 d + -3 -3 d -4 -2 d -5 X -5 2 d -1 1 d -2 3 d s 960 205 m 17 X -9 -12 d 4 X 4 -2 d + 1 -1 d 2 -5 d -3 Y -2 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 958 203 + m 17 X -9 -12 d 4 X 3 -2 d 2 -1 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 + d -1 1 d -2 3 d s 961 205 m 16 X -9 -12 d 5 X 3 -1 d 1 -2 d 2 -4 d -3 Y -2 -5 d + -3 -3 d -4 -1 d -5 X -4 1 d -2 2 d -1 3 d s 990 175 m -2 -1 d 2 -2 d 1 2 d -1 1 + d cl s 989 175 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 990 176 m -2 -2 d 2 -1 d 2 1 + d -2 2 d cl s 989 175 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 990 176 m -1 -1 d 1 -2 + d 2 2 d -2 1 d cl s 989 174 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 991 176 m -2 -1 + d 2 -2 d 1 2 d -1 1 d cl s 988 174 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 991 177 m + -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 1020 204 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 + d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1020 + 204 m -16 X -1 -14 d 1 2 d 5 1 d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d + -4 -2 d -5 X -5 2 d -1 1 d -2 3 d s 1020 204 m -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 + -2 d 3 -3 d 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 d -4 X -5 1 d -1 2 d -2 3 d s + 1019 203 m -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 1 -4 d -3 Y -1 -5 d -3 + -3 d -5 -1 d -4 X -5 1 d -1 2 d -2 3 d s 1021 205 m -16 X -1 -14 d 1 2 d 5 1 d + 4 X 5 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d + s 1019 203 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -4 Y -2 -4 d + -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1021 205 m -15 X -2 -14 d 2 2 d 4 1 + d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 + d s 1019 203 m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d + -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -2 3 d s 1021 205 m -15 X -1 -13 d 1 1 d 5 2 + d 4 X 5 -2 d 3 -3 d 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 d -4 X -5 1 d -1 2 d -2 3 + d s 1200 204 m -15 -21 d 23 X s 1200 204 m -15 -21 d 23 X s 1201 204 m -15 -21 + d 22 X s 1200 203 m -15 -21 d 22 X s 1201 205 m -15 -21 d 23 X s 1199 203 m -15 + -21 d 23 X s 1201 205 m -15 -21 d 23 X s 1199 203 m -15 -21 d 23 X s 1202 205 m + -15 -21 d 22 X s 1200 204 m -32 Y s 1200 204 m -32 Y s 1201 204 m -31 Y s 1200 + 203 m -31 Y s 1201 205 m -32 Y s 1199 203 m -32 Y s 1201 205 m -32 Y s 1199 203 + m -32 Y s 1202 205 m -31 Y s 1384 204 m -15 -21 d 22 X s 1384 204 m -16 -21 d + 23 X s 1384 204 m -15 -21 d 23 X s 1383 203 m -15 -21 d 23 X s 1385 205 m -16 + -21 d 23 X s 1383 203 m -15 -21 d 23 X s 1385 205 m -15 -21 d 22 X s 1383 203 m + -15 -21 d 22 X s 1385 205 m -15 -21 d 23 X s 1384 204 m -32 Y s 1384 204 m -32 + Y s 1384 204 m -31 Y s 1383 203 m -31 Y s 1385 205 m -32 Y s 1383 203 m -32 Y s + 1385 205 m -32 Y s 1383 203 m -32 Y s 1385 205 m -31 Y s 1402 175 m -1 -1 d 1 + -2 d 2 2 d -2 1 d cl s 1402 175 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 1402 176 m + -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 1401 175 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s + 1403 176 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 1401 174 m -1 -1 d 1 -2 d 2 2 d -2 + 1 d cl s 1403 176 m -2 -1 d 2 -2 d 2 2 d -2 1 d cl s 1401 174 m -2 -1 d 2 -2 d + 1 2 d -1 1 d cl s 1403 177 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 1432 204 m -15 X + -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 X + -5 2 d -1 1 d -2 3 d s 1432 204 m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 d 3 -3 d + 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1433 204 m -16 + X -1 -13 d 1 1 d 5 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d -4 -1 d -5 + X -5 1 d -1 2 d -2 3 d s 1432 203 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 3 -3 + d 2 -4 d -3 Y -2 -5 d -3 -3 d -4 -1 d -5 X -4 1 d -2 2 d -2 3 d s 1433 205 m + -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 + d -5 X -4 2 d -2 1 d -1 3 d s 1431 203 m -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d + 3 -3 d 1 -4 d -4 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1433 205 + m -15 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 + -2 d -4 X -5 2 d -1 1 d -2 3 d s 1431 203 m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 + d 4 -3 d 1 -5 d -3 Y -1 -4 d -4 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1434 + 205 m -16 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d + -5 -1 d -4 X -5 1 d -1 2 d -2 3 d s 1616 204 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 + -2 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s + 1615 204 m -15 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 + -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1616 204 m -15 X -2 -13 d 2 1 d 5 2 d + 4 X 5 -2 d 3 -3 d 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 d -4 X -5 1 d -2 2 d -1 3 d + s 1615 203 m -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 1 -4 d -3 Y -1 -5 d + -3 -3 d -5 -1 d -4 X -5 1 d -1 2 d -2 3 d s 1616 205 m -15 X -1 -14 d 1 2 d 5 1 + d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 + d s 1615 203 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -4 Y -2 -4 d + -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1617 205 m -15 X -2 -14 d 2 2 d 4 1 + d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 + d s 1615 203 m -16 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d + -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1617 205 m -15 X -2 -13 d 2 1 d 4 2 + d 5 X 5 -2 d 3 -3 d 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 d -5 X -4 1 d -2 2 d -1 3 + d s 1799 204 m -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 1 -5 d -3 Y -1 -4 d + -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1799 204 m -15 X -2 -14 d 2 2 d 4 1 + d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 + d s 1800 204 m -16 X -1 -13 d 1 1 d 5 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d + -3 -3 d -4 -1 d -5 X -5 1 d -1 2 d -2 3 d s 1799 203 m -15 X -2 -13 d 2 1 d 4 2 + d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d -4 -1 d -5 X -4 1 d -2 2 d -1 3 + d s 1800 205 m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d + -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1798 203 m -15 X -1 -13 d 1 1 d 5 2 + d 4 X 5 -2 d 3 -3 d 1 -4 d -4 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 + d s 1800 205 m -15 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d + -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1798 203 m -15 X -2 -14 d 2 2 d 4 1 + d 5 X 4 -1 d 4 -3 d 1 -5 d -3 Y -1 -4 d -4 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 + d s 1801 205 m -16 X -1 -13 d 1 1 d 5 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d + -3 -3 d -4 -1 d -5 X -5 1 d -1 2 d -2 3 d s 1814 175 m -1 -1 d 1 -2 d 2 2 d -2 + 1 d cl s 1814 175 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 1815 176 m -2 -2 d 2 -1 d + 1 1 d -1 2 d cl s 1814 175 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 1815 176 m -1 -1 + d 1 -2 d 2 2 d -2 1 d cl s 1813 174 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 1815 176 + m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 1813 174 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s + 1816 177 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 1845 204 m -15 X -2 -13 d 2 1 d 4 2 + d 5 X 4 -2 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -2 3 + d s 1844 204 m -15 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d + -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1845 204 m -15 X -2 -13 d 2 1 d 4 2 + d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d -4 -1 d -5 X -4 1 d -2 2 d -1 3 + d s 1844 203 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 4 -3 d 1 -4 d -3 Y -1 -5 d + -4 -3 d -4 -1 d -5 X -4 1 d -2 2 d -1 3 d s 1845 205 m -15 X -1 -14 d 1 2 d 5 1 + d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 + d s 1844 203 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -4 Y -2 -4 d + -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1846 205 m -16 X -1 -14 d 1 2 d 5 1 + d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -5 2 d -1 1 d -2 3 + d s 1843 203 m -15 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d + -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1846 205 m -15 X -2 -13 d 2 1 d 4 2 + d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d -4 -1 d -5 X -4 1 d -2 2 d -1 3 + d s 2030 200 m -2 3 d -4 1 d -3 X -5 -1 d -3 -5 d -1 -7 d -8 Y 1 -6 d 3 -3 d 5 + -2 d 1 X 5 2 d 3 3 d 1 4 d 2 Y -1 4 d -3 4 d -5 1 d -1 X -5 -1 d -3 -4 d -1 -4 + d s 2029 199 m -1 3 d -5 2 d -3 X -4 -2 d -3 -4 d -2 -8 d -7 Y 2 -6 d 3 -3 d 4 + -2 d 2 X 4 2 d 3 3 d 2 4 d 2 Y -2 4 d -3 3 d -4 2 d -2 X -4 -2 d -3 -3 d -2 -4 + d s 2030 200 m -2 3 d -4 1 d -3 X -5 -1 d -3 -5 d -1 -7 d -8 Y 1 -6 d 3 -3 d 5 + -1 d 1 X 5 1 d 3 3 d 1 5 d 1 Y -1 5 d -3 3 d -5 1 d -1 X -5 -1 d -3 -3 d -1 -5 + d s 2029 199 m -1 3 d -5 1 d -3 X -5 -1 d -3 -5 d -1 -7 d -8 Y 1 -6 d 3 -3 d 5 + -1 d 1 X 5 1 d 3 3 d 2 5 d 1 Y -2 5 d -3 3 d -5 1 d -1 X -5 -1 d -3 -3 d -1 -5 + d s 2030 200 m -1 3 d -5 2 d -3 X -4 -2 d -3 -4 d -2 -8 d -7 Y 2 -6 d 3 -3 d 4 + -2 d 2 X 4 2 d 3 3 d 2 4 d 2 Y -2 4 d -3 3 d -4 2 d -2 X -4 -2 d -3 -3 d -2 -4 + d s 2029 199 m -2 3 d -4 1 d -3 X 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0 0 P01 + setcolor 1959 1989 m 41 X 52 Y -41 X FA black 41 52 1959 1989 bl cs 0 0 0 P01 + setcolor 2000 1989 m 41 X 52 Y -41 X FA black 41 52 2000 1989 bl + gr gr +showpage +end +%%EOF diff --git a/Magnet_Stations/11_10_2018_OPG/Makefile b/Magnet_Stations/11_10_2018_OPG/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Magnet_Stations/11_10_2018_OPG/OpenOT_zoom.eps b/Magnet_Stations/11_10_2018_OPG/OpenOT_zoom.eps new file mode 100644 index 0000000..69855ec --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/OpenOT_zoom.eps @@ -0,0 +1,1907 @@ +%!PS-Adobe-2.0 EPSF-2.0 +%%BoundingBox: 0 0 567 567 +%%Title: OpenOT_zoom.eps +%%Creator: HIGZ Version 1.29/04 +%%CreationDate: 2018/10/08 17.15 +%%EndComments +%%BeginProlog +80 dict begin +/s {stroke} def /l {lineto} def /m {moveto} def /t {translate} def +/sw {stringwidth} def /r {rotate} def /rl {roll} def /R {repeat} def +/d {rlineto} def /rm {rmoveto} def /gr {grestore} def /f {eofill} def +/c {setrgbcolor} def /lw {setlinewidth} def /sd {setdash} def +/cl {closepath} def /sf {scalefont setfont} def /black {0 setgray} def +/box {m dup 0 exch d exch 0 d 0 exch neg d cl} def +/NC{systemdict begin initclip end}def/C{NC box clip newpath}def +/bl {box s} def /bf {box f} def /Y { 0 exch d} def /X { 0 d} def +/mp {newpath /y exch def /x exch def} def +/side {[w .77 mul w .23 mul] .385 w mul sd w 0 l currentpoint t -144 r} def +/mr {mp x y w2 0 360 arc} def /m24 {mr s} def /m20 {mr f} def +/mb {mp x y w2 add m w2 neg 0 d 0 w neg d w 0 d 0 w d cl} def +/mt {mp x y w2 add m w2 neg w neg d w 0 d cl} def +/m21 {mb f} def /m25 {mb s} def /m22 {mt f} def /m26 {mt s} def +/m23 {mp x y w2 sub m w2 w d w neg 0 d cl f} def +/m27 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl s} def +/m28 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d + 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d + 0 w3 neg d w3 neg 0 d cl s } def +/m29 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t + 4 {side} repeat cl fill gr} def +/m30 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t + 5 {side} repeat s gr} def +/m31 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d + x w2 sub y w2 add m w w neg d x w2 sub y w2 + sub m w w d s} def +/m2 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d s} def +/m5 {mp x w2 sub y w2 sub m w w d x w2 sub y w2 add m w w neg d s} def +/reencdict 24 dict def /ReEncode {reencdict begin /nco&na exch def +/nfnam exch def /basefontname exch def /basefontdict basefontname findfont def +/newfont basefontdict maxlength dict def basefontdict {exch dup /FID ne +{dup /Encoding eq {exch dup length array copy newfont 3 1 roll put} {exch +newfont 3 1 roll put} ifelse} {pop pop} ifelse } forall newfont +/FontName nfnam put nco&na aload pop nco&na length 2 idiv {newfont +/Encoding get 3 1 roll put} repeat nfnam newfont definefont pop end } def +/accvec [ 176 /agrave 181 /Agrave 190 /acircumflex 192 /Acircumflex +201 /adieresis 204 /Adieresis 209 /ccedilla 210 /Ccedilla 211 /eacute +212 /Eacute 213 /egrave 214 /Egrave 215 /ecircumflex 216 /Ecircumflex +217 /edieresis 218 /Edieresis 219 /icircumflex 220 /Icircumflex +221 /idieresis 222 /Idieresis 223 /ntilde 224 /Ntilde 226 /ocircumflex +228 /Ocircumflex 229 /odieresis 230 /Odieresis 231 /ucircumflex 236 /Ucircumflex +237 /udieresis 238 /Udieresis 239 /aring 242 /Aring 243 /ydieresis +244 /Ydieresis 246 /aacute 247 /Aacute 252 /ugrave 253 /Ugrave] def +/Times-Roman /Times-Roman accvec ReEncode +/Times-Italic /Times-Italic accvec ReEncode +/Times-Bold /Times-Bold accvec ReEncode +/Times-BoldItalic /Times-BoldItalic accvec ReEncode +/Helvetica /Helvetica accvec ReEncode +/Helvetica-Oblique /Helvetica-Oblique accvec ReEncode +/Helvetica-Bold /Helvetica-Bold accvec ReEncode +/Helvetica-BoldOblique /Helvetica-BoldOblique accvec ReEncode +/Courier /Courier accvec ReEncode +/Courier-Oblique /Courier-Oblique accvec ReEncode +/Courier-Bold /Courier-Bold accvec ReEncode +/Courier-BoldOblique /Courier-BoldOblique accvec ReEncode +/oshow {gsave [] 0 sd true charpath stroke gr} def +/stwn { /fs exch def /fn exch def /text exch def fn findfont fs sf + text sw pop xs add /xs exch def} def +/stwb { /fs exch def /fn exch def /nbas exch def /textf exch def +textf length /tlen exch def nbas tlen gt {/nbas tlen def} if +fn findfont fs sf textf dup length nbas sub nbas getinterval sw +pop neg xs add /xs exch def} def +/accspe [ 65 /plusminus 66 /bar 67 /existential 68 /universal +69 /exclam 70 /numbersign 71 /greater 72 /question 73 /integral +74 /colon 75 /semicolon 76 /less 77 /bracketleft 78 /bracketright +79 /greaterequal 80 /braceleft 81 /braceright 82 /radical +83 /spade 84 /heart 85 /diamond 86 /club 87 /lessequal +88 /multiply 89 /percent 90 /infinity 48 /circlemultiply 49 /circleplus +50 /emptyset 51 /lozenge 52 /bullet 53 /arrowright 54 /arrowup +55 /arrowleft 56 /arrowdown 57 /arrowboth 48 /degree 44 /comma 43 /plus + 45 /angle 42 /angleleft 47 /divide 61 /notequal 40 /equivalence 41 /second + 97 /approxequal 98 /congruent 99 /perpendicular 100 /partialdiff 101 /florin + 102 /intersection 103 /union 104 /propersuperset 105 /reflexsuperset + 106 /notsubset 107 /propersubset 108 /reflexsubset 109 /element 110 /notelement + 111 /gradient 112 /logicaland 113 /logicalor 114 /arrowdblboth + 115 /arrowdblleft 116 /arrowdblup 117 /arrowdblright 118 /arrowdbldown + 119 /ampersand 120 /omega1 121 /similar 122 /aleph ] def +/Symbol /Special accspe ReEncode +%%EndProlog +%%BeginSetup +%%EndSetup +newpath gsave .25 .25 scale gsave 0 0 t black [] 0 sd 1 lw 1814 1814 227 227 + bl 1814 1814 227 227 C 3 lw 8 11 326 351 bl 8 10 285 403 bl 14 18 323 399 bl 16 + 21 363 398 bl 15 18 405 399 bl 9 10 449 403 bl 9 10 243 455 bl 11 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-6 X cl s 163 1305 m -5 -1 d -1 -3 d -3 Y 1 -4 d 3 -1 d 7 -2 d 4 -1 d 3 -3 d 2 + -3 d -5 Y -2 -3 d -1 -1 d -5 -2 d -6 X -5 2 d -1 1 d -2 3 d 5 Y 2 3 d 3 3 d 4 1 + d 7 2 d 3 1 d 1 4 d 3 Y -1 3 d -5 1 d -6 X cl s 164 1306 m -5 -2 d -1 -3 d -3 Y + 1 -3 d 3 -1 d 6 -2 d 5 -1 d 3 -3 d 1 -3 d -5 Y -1 -3 d -2 -2 d -4 -1 d -6 X -5 + 1 d -1 2 d -2 3 d 5 Y 2 3 d 3 3 d 4 1 d 6 2 d 3 1 d 2 3 d 3 Y -2 3 d -4 2 d -6 + X cl s 163 1305 m -5 -2 d -1 -3 d -3 Y 1 -3 d 3 -1 d 6 -2 d 5 -1 d 3 -3 d 1 -3 + d -5 Y -1 -3 d -2 -1 d -4 -2 d -6 X -5 2 d -1 1 d -2 3 d 5 Y 2 3 d 3 3 d 4 1 d + 6 2 d 3 1 d 2 3 d 3 Y -2 3 d -4 2 d -6 X cl s 164 1306 m -5 -1 d -1 -4 d -3 Y 1 + -3 d 3 -1 d 6 -2 d 5 -1 d 3 -3 d 2 -3 d -5 Y -2 -3 d -1 -1 d -5 -2 d -6 X -5 2 + d -1 1 d -2 3 d 5 Y 2 3 d 3 3 d 4 1 d 6 2 d 4 1 d 1 3 d 3 Y -1 4 d -5 1 d -6 X + cl s 162 1304 m -4 -1 d -2 -3 d -3 Y 2 -3 d 3 -2 d 6 -1 d 4 -2 d 3 -3 d 2 -3 d + -4 Y -2 -3 d -1 -2 d -5 -1 d -6 X -4 1 d -2 2 d -1 3 d 4 Y 1 3 d 3 3 d 5 2 d 6 + 1 d 3 2 d 1 3 d 3 Y -1 3 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d -5 X -4 2 d -2 1 d -1 3 d s 1020 204 m -16 X + -1 -14 d 1 2 d 5 1 d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X + -5 2 d -1 1 d -2 3 d s 1020 204 m -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d + 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 d -4 X -5 1 d -1 2 d -2 3 d s 1019 203 m -15 + X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 d -4 + X -5 1 d -1 2 d -2 3 d s 1021 205 m -16 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 + d 2 -5 d -3 Y -2 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1019 203 m + -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -4 Y -2 -4 d -3 -3 d -4 -2 + d -5 X -4 2 d -2 1 d -1 3 d s 1021 205 m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 d + 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1019 203 + m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 + -2 d -5 X -4 2 d -2 1 d -2 3 d s 1021 205 m -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 + d 3 -3 d 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 d -4 X -5 1 d -1 2 d -2 3 d s 1200 + 204 m -15 -21 d 23 X s 1200 204 m -15 -21 d 23 X s 1201 204 m -15 -21 d 22 X s + 1200 203 m -15 -21 d 22 X s 1201 205 m -15 -21 d 23 X s 1199 203 m -15 -21 d 23 + X s 1201 205 m -15 -21 d 23 X s 1199 203 m -15 -21 d 23 X s 1202 205 m -15 -21 + d 22 X s 1200 204 m -32 Y s 1200 204 m -32 Y s 1201 204 m -31 Y s 1200 203 m + -31 Y s 1201 205 m -32 Y s 1199 203 m -32 Y s 1201 205 m -32 Y s 1199 203 m -32 + Y s 1202 205 m -31 Y s 1384 204 m -15 -21 d 22 X s 1384 204 m -16 -21 d 23 X s + 1384 204 m -15 -21 d 23 X s 1383 203 m -15 -21 d 23 X s 1385 205 m -16 -21 d 23 + X s 1383 203 m -15 -21 d 22 X s 1385 205 m -15 -21 d 22 X s 1383 203 m -15 -21 + d 22 X s 1385 205 m -15 -21 d 23 X s 1384 204 m -32 Y s 1384 204 m -32 Y s 1384 + 204 m -31 Y s 1383 203 m -31 Y s 1385 205 m -32 Y s 1383 203 m -32 Y s 1385 205 + m -32 Y s 1383 203 m -32 Y s 1385 205 m -31 Y s 1402 175 m -1 -1 d 1 -2 d 2 2 d + -2 1 d cl s 1402 175 m -2 -1 d 2 -2 d 1 2 d -1 1 d cl s 1402 176 m -1 -2 d 1 -1 + d 2 1 d -2 2 d cl s 1401 175 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 1403 176 m -2 + -1 d 2 -2 d 1 2 d -1 1 d cl s 1401 174 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 1403 + 176 m -2 -1 d 2 -2 d 2 2 d -2 1 d cl s 1401 174 m -2 -1 d 2 -2 d 1 2 d -1 1 d + cl s 1403 177 m -1 -2 d 1 -1 d 2 1 d -2 2 d cl s 1432 204 m -15 X -1 -13 d 1 1 + d 5 2 d 4 X 5 -2 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 + d -2 3 d s 1432 204 m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y + -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1433 204 m -16 X -1 -13 d 1 + 1 d 5 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d -4 -1 d -5 X -5 1 d -1 + 2 d -2 3 d s 1432 203 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -3 + Y -2 -5 d -3 -3 d -4 -1 d -5 X -4 1 d -2 2 d -2 3 d s 1433 205 m -15 X -2 -14 d + 2 2 d 4 1 d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d + -2 1 d -1 3 d s 1431 203 m -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 1 -4 d + -4 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1433 205 m -15 X -1 + -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 + 2 d -1 1 d -2 3 d s 1431 203 m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 d 4 -3 d 1 + -5 d -3 Y -1 -4 d -4 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1434 205 m -16 X + -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d -5 -1 d -4 X + -5 1 d -1 2 d -2 3 d s 1616 204 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 3 -3 d + 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1615 204 m -15 + X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 + X -5 2 d -1 1 d -2 3 d s 1616 204 m -15 X -2 -13 d 2 1 d 5 2 d 4 X 5 -2 d 3 -3 + d 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 d -4 X -5 1 d -2 2 d -1 3 d s 1615 203 m + -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 + d -4 X -5 1 d -1 2 d -2 3 d s 1616 205 m -15 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d + 3 -3 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1615 203 + m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -4 Y -2 -4 d -3 -3 d -4 + -2 d -5 X -4 2 d -2 1 d -1 3 d s 1617 205 m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 + d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1615 + 203 m -16 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d + -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1617 205 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 5 + -2 d 3 -3 d 1 -4 d -3 Y -1 -5 d -3 -3 d -5 -1 d -5 X -4 1 d -2 2 d -1 3 d s + 1799 204 m -15 X -1 -13 d 1 1 d 5 2 d 4 X 5 -2 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 + -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1799 204 m -15 X -2 -14 d 2 2 d 4 1 d + 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d + s 1800 204 m -16 X -1 -13 d 1 1 d 5 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d + -3 -3 d -4 -1 d -5 X -5 1 d -1 2 d -2 3 d s 1799 203 m -15 X -2 -13 d 2 1 d 4 2 + d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d -4 -1 d -5 X -4 1 d -2 2 d -1 3 + d s 1800 205 m -15 X -2 -14 d 2 2 d 4 1 d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d + -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1798 203 m -15 X -1 -13 d 1 1 d 5 2 + d 4 X 5 -2 d 3 -3 d 1 -4 d -4 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 + d s 1800 205 m -15 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d + -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1798 203 m -15 X -2 -14 d 2 2 d 4 1 + d 5 X 4 -1 d 4 -3 d 1 -5 d -3 Y -1 -4 d -4 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 + d s 1801 205 m -16 X -1 -13 d 1 1 d 5 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d + -3 -3 d -4 -1 d -5 X -5 1 d -1 2 d -2 3 d s 1814 175 m -1 -1 d 1 -2 d 2 2 d -2 + 1 d cl s 1814 175 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 1815 176 m -2 -2 d 2 -1 d + 1 1 d -1 2 d cl s 1814 175 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 1815 176 m -1 -1 + d 1 -2 d 2 2 d -2 1 d cl s 1813 174 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 1815 176 + m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s 1813 174 m -1 -1 d 1 -2 d 2 2 d -2 1 d cl s + 1816 177 m -2 -2 d 2 -1 d 1 1 d -1 2 d cl s 1845 204 m -15 X -2 -13 d 2 1 d 4 2 + d 5 X 4 -2 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -2 3 + d s 1844 204 m -15 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d + -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1845 204 m -15 X -2 -13 d 2 1 d 4 2 + d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d -4 -1 d -5 X -4 1 d -2 2 d -1 3 + d s 1844 203 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 4 -3 d 1 -4 d -3 Y -1 -5 d + -4 -3 d -4 -1 d -5 X -4 1 d -2 2 d -1 3 d s 1845 205 m -15 X -1 -14 d 1 2 d 5 1 + d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 + d s 1844 203 m -15 X -2 -13 d 2 1 d 4 2 d 5 X 4 -2 d 3 -3 d 2 -4 d -4 Y -2 -4 d + -3 -3 d -4 -2 d -5 X -4 2 d -2 1 d -1 3 d s 1846 205 m -16 X -1 -14 d 1 2 d 5 1 + d 5 X 4 -1 d 3 -3 d 2 -5 d -3 Y -2 -4 d -3 -3 d -4 -2 d -5 X -5 2 d -1 1 d -2 3 + d s 1843 203 m -15 X -1 -14 d 1 2 d 5 1 d 4 X 5 -1 d 3 -3 d 1 -5 d -3 Y -1 -4 d + -3 -3 d -5 -2 d -4 X -5 2 d -1 1 d -2 3 d s 1846 205 m -15 X -2 -13 d 2 1 d 4 2 + d 5 X 4 -2 d 3 -3 d 2 -4 d -3 Y -2 -5 d -3 -3 d -4 -1 d -5 X -4 1 d -2 2 d -1 3 + d s 2030 200 m -2 3 d -4 1 d -3 X -5 -1 d -3 -5 d -1 -7 d -8 Y 1 -6 d 3 -3 d 5 + -2 d 1 X 5 2 d 3 3 d 1 4 d 2 Y -1 4 d -3 4 d -5 1 d -1 X -5 -1 d -3 -4 d -1 -4 + d s 2029 199 m -1 3 d -5 2 d -3 X -4 -2 d -3 -4 d -2 -8 d -7 Y 2 -6 d 3 -3 d 4 + -2 d 2 X 4 2 d 3 3 d 2 4 d 2 Y -2 4 d -3 3 d -4 2 d -2 X -4 -2 d -3 -3 d -2 -4 + d s 2030 200 m -2 3 d -4 1 d -3 X -5 -1 d -3 -5 d -1 -7 d -8 Y 1 -6 d 3 -3 d 5 + -1 d 1 X 5 1 d 3 3 d 1 5 d 1 Y -1 5 d -3 3 d -5 1 d -1 X -5 -1 d -3 -3 d -1 -5 + d s 2029 199 m -1 3 d -5 1 d -3 X -5 -1 d -3 -5 d -1 -7 d -8 Y 1 -6 d 3 -3 d 5 + -1 d 1 X 5 1 d 3 3 d 2 5 d 1 Y -2 5 d -3 3 d -5 1 d -1 X -5 -1 d -3 -3 d -1 -5 + d s 2030 200 m -1 3 d -5 2 d -3 X -4 -2 d -3 -4 d -2 -8 d -7 Y 2 -6 d 3 -3 d 4 + -2 d 2 X 4 2 d 3 3 d 2 4 d 2 Y -2 4 d -3 3 d -4 2 d -2 X -4 -2 d -3 -3 d -2 -4 + d s 2029 199 m -2 3 d -4 1 d -3 X -5 -1 d -3 -5 d -1 -7 d -8 Y 1 -6 d 3 -3 d 5 + -2 d 1 X 5 2 d 3 3 d 1 4 d 2 Y -1 5 d -3 3 d -5 1 d -1 X -5 -1 d -3 -3 d -1 -5 + d s 2031 201 m -2 3 d -4 1 d -3 X -5 -1 d -3 -5 d -2 -8 d -7 Y 2 -6 d 3 -3 d 5 + -2 d 1 X 5 2 d 3 3 d 1 4 d 2 Y -1 4 d -3 3 d -5 2 d -1 X -5 -2 d -3 -3 d -2 -4 + d s 2028 198 m -1 3 d -5 2 d -3 X -4 -2 d -3 -4 d -2 -8 d -7 Y 2 -6 d 3 -3 d 4 + -2 d 2 X 4 2 d 3 3 d 2 4 d 2 Y -2 4 d -3 3 d -4 2 d -2 X -4 -2 d -3 -3 d -2 -4 + d s 2031 201 m -2 3 d -4 1 d -3 X -5 -1 d -3 -5 d -1 -7 d -8 Y 1 -6 d 3 -3 d 5 + -1 d 1 X 5 1 d 3 3 d 1 5 d 1 Y -1 5 d -3 3 d -5 1 d -1 X -5 -1 d -3 -3 d -1 -5 + d s 1814 1814 227 227 C 2268 2268 0 0 C 2000 112 m 2 5 d 5 4 d 4 X 2 -2 d -5 Y + -2 -8 d -4 -15 d s 2000 112 m 2 4 d 4 5 d 5 X 2 -3 d -4 Y -2 -9 d -5 -15 d s + 2001 113 m 2 4 d 4 4 d 4 X 3 -2 d -4 Y -3 -9 d -4 -15 d s 1999 111 m 2 5 d 5 4 + d 4 X 2 -2 d -4 Y -2 -9 d -4 -15 d s 2001 113 m 2 5 d 5 4 d 4 X 2 -2 d -5 Y -2 + -8 d -4 -15 d s 1999 111 m 2 4 d 4 5 d 5 X 2 -3 d -4 Y -2 -9 d -5 -15 d s 2002 + 114 m 2 4 d 4 4 d 4 X 2 -2 d -4 Y -2 -9 d -4 -15 d s 1998 111 m 3 4 d 4 4 d 4 X + 2 -2 d -4 Y -2 -9 d -4 -15 d s 2002 114 m 2 4 d 4 5 d 5 X 2 -2 d -5 Y -2 -8 d + -5 -15 d s 2011 106 m 4 8 d 5 5 d 4 2 d 4 X 5 -4 d -7 Y -3 -11 d -6 -23 d s + 2011 105 m 4 9 d 4 4 d 4 3 d 5 X 4 -5 d -6 Y -2 -11 d -7 -24 d s 2011 106 m 5 9 + d 4 4 d 4 2 d 5 X 4 -4 d -6 Y -2 -11 d -7 -24 d s 2010 105 m 4 9 d 5 4 d 4 2 d + 4 X 5 -4 d -7 Y -3 -11 d -6 -23 d s 2012 107 m 4 8 d 5 5 d 4 2 d 4 X 4 -4 d -7 + Y -2 -11 d -6 -23 d s 2010 104 m 4 9 d 4 4 d 5 3 d 4 X 4 -5 d -6 Y -2 -11 d -6 + -24 d s 2012 107 m 5 9 d 4 4 d 4 2 d 5 X 4 -4 d -6 Y -2 -11 d -7 -24 d s 2009 + 104 m 4 9 d 5 4 d 4 2 d 4 X 5 -4 d -7 Y -2 -10 d -7 -24 d s 2013 108 m 4 8 d 4 + 5 d 5 2 d 4 X 4 -5 d -6 Y -2 -11 d -6 -24 d s 60 1717 m 46 X s 60 1717 m 45 X s + 61 1718 m 45 X s 60 1716 m 45 X s 61 1718 m 46 X s 59 1716 m 45 X s 62 1719 m + 45 X s 59 1715 m 45 X s 62 1719 m 46 X s 67 1717 m -4 5 d -3 4 d 6 Y 3 5 d 4 4 + d 6 2 d 5 X 6 -2 d 5 -4 d 2 -5 d -6 Y -2 -4 d -5 -5 d s 67 1717 m -5 4 d -2 4 d + 7 Y 2 4 d 5 5 d 6 2 d 4 X 7 -2 d 4 -5 d 2 -4 d -7 Y -2 -4 d -4 -4 d s 67 1718 m + -4 4 d -2 4 d 7 Y 2 4 d 4 4 d 7 3 d 4 X 7 -3 d 4 -4 d 2 -4 d -7 Y -2 -4 d -4 -4 + d s 66 1716 m -4 5 d -2 4 d 6 Y 2 5 d 4 4 d 7 2 d 4 X 6 -2 d 5 -4 d 2 -5 d -6 Y + -2 -4 d -5 -5 d s 68 1718 m -4 4 d -3 5 d 6 Y 3 5 d 4 4 d 6 2 d 5 X 6 -2 d 4 -4 + d 3 -5 d -6 Y -3 -5 d -4 -4 d s 66 1716 m -5 4 d -2 4 d 7 Y 2 4 d 5 5 d 6 2 d 4 + X 7 -2 d 4 -5 d 2 -4 d -7 Y -2 -4 d -4 -4 d s 68 1719 m -4 4 d -2 4 d 7 Y 2 4 d + 4 4 d 7 2 d 4 X 7 -2 d 4 -4 d 2 -4 d -7 Y -2 -4 d -4 -4 d s 65 1715 m -4 5 d -2 + 4 d 7 Y 2 4 d 4 4 d 7 2 d 4 X 6 -2 d 5 -4 d 2 -4 d -7 Y -2 -4 d -5 -5 d s 69 + 1719 m -5 4 d -2 5 d 6 Y 2 4 d 5 5 d 6 2 d 5 X 6 -2 d 4 -5 d 3 -4 d -6 Y -3 -5 + d -4 -4 d s 37 1795 m 4 -4 d 7 -5 d 8 -4 d 11 -2 d 9 X 10 2 d 9 4 d 7 5 d 4 4 d + s 36 1795 m 5 -5 d 6 -4 d 9 -4 d 11 -3 d 8 X 11 3 d 9 4 d 6 4 d 4 5 d s 37 1795 + m 4 -4 d 7 -4 d 9 -5 d 10 -2 d 9 X 11 2 d 8 5 d 7 4 d 4 4 d s 36 1794 m 4 -4 d + 7 -5 d 8 -4 d 11 -2 d 9 X 10 2 d 9 4 d 7 5 d 4 4 d s 38 1796 m 4 -4 d 6 -5 d 9 + -4 d 11 -2 d 9 X 10 2 d 9 4 d 6 5 d 5 4 d s 35 1794 m 5 -5 d 6 -4 d 9 -4 d 11 + -3 d 8 X 11 3 d 9 4 d 6 4 d 4 5 d s 38 1796 m 4 -4 d 7 -4 d 9 -5 d 10 -2 d 9 X + 11 2 d 8 5 d 7 4 d 4 4 d s 35 1793 m 4 -4 d 7 -4 d 8 -5 d 11 -2 d 9 X 11 2 d 8 + 5 d 7 4 d 4 4 d s 39 1797 m 4 -5 d 6 -4 d 9 -4 d 11 -2 d 8 X 11 2 d 9 4 d 6 4 d + 5 5 d s 56 1840 m -4 -2 d -4 -4 d -3 -4 d -9 Y 3 -4 d 4 -5 d 4 -2 d 7 -2 d 10 X + 7 2 d 4 2 d 5 5 d 2 4 d 9 Y -2 4 d -5 4 d -4 2 d -7 X s 56 1840 m -5 -2 d -4 -5 + d -2 -4 d -9 Y 2 -4 d 4 -4 d 5 -2 d 6 -3 d 11 X 6 3 d 5 2 d 4 4 d 2 4 d 9 Y -2 + 4 d -4 5 d -5 2 d -6 X s 57 1841 m -5 -2 d -4 -5 d -2 -4 d -9 Y 2 -4 d 4 -4 d 5 + -2 d 6 -3 d 11 X 6 3 d 5 2 d 4 4 d 2 4 d 9 Y -2 4 d -4 5 d -5 2 d -6 X s 55 + 1839 m -4 -2 d -4 -4 d -3 -4 d -9 Y 3 -4 d 4 -5 d 4 -2 d 7 -2 d 11 X 6 2 d 4 2 + d 5 5 d 2 4 d 9 Y -2 4 d -5 4 d -4 2 d -6 X s 57 1841 m -4 -2 d -5 -4 d -2 -5 d + -8 Y 2 -5 d 5 -4 d 4 -2 d 7 -2 d 10 X 7 2 d 4 2 d 4 4 d 3 5 d 8 Y -3 5 d -4 4 d + -4 2 d -7 X s 55 1839 m -5 -2 d -4 -5 d -2 -4 d -8 Y 2 -5 d 4 -4 d 5 -2 d 6 -2 + d 11 X 7 2 d 4 2 d 4 4 d 2 5 d 8 Y -2 4 d -4 5 d -4 2 d -7 X s 58 1842 m -5 -2 + d -4 -5 d -2 -4 d -9 Y 2 -4 d 4 -4 d 5 -3 d 6 -2 d 11 X 6 2 d 5 3 d 4 4 d 2 4 d + 9 Y -2 4 d -4 5 d -5 2 d -6 X s 54 1839 m -4 -3 d -4 -4 d -2 -4 d -9 Y 2 -4 d 4 + -5 d 4 -2 d 7 -2 d 11 X 6 2 d 4 2 d 5 5 d 2 4 d 9 Y -2 4 d -5 4 d -4 3 d -6 X s + 58 1842 m -4 -2 d -5 -4 d -2 -5 d -8 Y 2 -5 d 5 -4 d 4 -2 d 6 -2 d 11 X 7 2 d 4 + 2 d 4 4 d 3 5 d 8 Y -3 5 d -4 4 d -4 2 d -7 X s 73 1830 m 10 Y s 73 1829 m 11 Y + s 74 1830 m 11 Y s 73 1829 m 10 Y s 74 1830 m 11 Y s 72 1828 m 11 Y s 75 1831 m + 11 Y s 72 1828 m 11 Y s 75 1831 m 11 Y s 73 1853 m 26 Y -4 X -4 -2 d -2 -2 d -3 + -4 d -7 Y 3 -4 d 4 -5 d 6 -2 d 5 X 6 2 d 5 5 d 2 4 d 7 Y -2 4 d -5 4 d s 73 + 1853 m 26 Y -4 X -5 -2 d -2 -3 d -2 -4 d -6 Y 2 -5 d 5 -4 d 6 -2 d 4 X 7 2 d 4 + 4 d 2 5 d 6 Y -2 4 d -4 5 d s 74 1854 m 26 Y -4 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black 42 51 1010 1938 bl cs 0 0 0 P01 + setcolor 1052 1938 m 41 X 51 Y -41 X FA black 41 51 1052 1938 bl cs 0 0 0 P01 + setcolor 1093 1938 m 41 X 51 Y -41 X FA black 41 51 1093 1938 bl cs 0 0 0 P01 + setcolor 1134 1938 m 41 X 51 Y -41 X FA black 41 51 1134 1938 bl cs 0 0 0 P01 + setcolor 1175 1938 m 41 X 51 Y -41 X FA black 41 51 1175 1938 bl cs 0 0 0 P01 + setcolor 1216 1938 m 42 X 51 Y -42 X FA black 42 51 1216 1938 bl cs 0 0 0 P01 + setcolor 1258 1938 m 41 X 51 Y -41 X FA black 41 51 1258 1938 bl cs 0 0 0 P01 + setcolor 1299 1938 m 41 X 51 Y -41 X FA black 41 51 1299 1938 bl cs 0 0 0 P01 + setcolor 1340 1938 m 41 X 51 Y -41 X FA black 41 51 1340 1938 bl cs 0 0 0 P01 + setcolor 1381 1938 m 42 X 51 Y -42 X FA black 42 51 1381 1938 bl cs 0 0 0 P01 + setcolor 1423 1938 m 41 X 51 Y -41 X FA black 41 51 1423 1938 bl cs 0 0 0 P01 + setcolor 1464 1938 m 41 X 51 Y -41 X FA black 41 51 1464 1938 bl cs 0 0 0 P01 + setcolor 1505 1938 m 41 X 51 Y -41 X FA black 41 51 1505 1938 bl cs 0 0 0 P01 + 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black 9 10 243 2010 bl cs 0 0 0 P01 + setcolor 283 2008 m 11 X 15 Y -11 X FA black 11 15 283 2008 bl cs 0 0 0 P01 + setcolor 321 2004 m 18 X 23 Y -18 X FA black 18 23 321 2004 bl cs 0 0 0 P01 + setcolor 359 2001 m 24 X 29 Y -24 X FA black 24 29 359 2001 bl cs 0 0 0 P01 + setcolor 398 1998 m 28 X 35 Y -28 X FA black 28 35 398 1998 bl cs 0 0 0 P01 + setcolor 437 1994 m 33 X 42 Y -33 X FA black 33 42 437 1994 bl cs 0 0 0 P01 + setcolor 478 1994 m 34 X 43 Y -34 X FA black 34 43 478 1994 bl cs 0 0 0 P01 + setcolor 519 1993 m 35 X 44 Y -35 X FA black 35 44 519 1993 bl cs 0 0 0 P01 + setcolor 559 1993 m 36 X 45 Y -36 X FA black 36 45 559 1993 bl cs 0 0 0 P01 + setcolor 600 1992 m 37 X 46 Y -37 X FA black 37 46 600 1992 bl cs 0 0 0 P01 + setcolor 640 1991 m 39 X 49 Y -39 X FA black 39 49 640 1991 bl cs 0 0 0 P01 + setcolor 680 1989 m 42 X 52 Y -42 X FA black 42 52 680 1989 bl cs 0 0 0 P01 + setcolor 722 1989 m 41 X 52 Y -41 X FA black 41 52 722 1989 bl cs 0 0 0 P01 + setcolor 763 1989 m 41 X 52 Y -41 X FA black 41 52 763 1989 bl cs 0 0 0 P01 + setcolor 804 1989 m 41 X 52 Y -41 X FA black 41 52 804 1989 bl cs 0 0 0 P01 + setcolor 845 1989 m 42 X 52 Y -42 X FA black 42 52 845 1989 bl cs 0 0 0 P01 + setcolor 887 1989 m 41 X 52 Y -41 X FA black 41 52 887 1989 bl cs 0 0 0 P01 + setcolor 928 1989 m 41 X 52 Y -41 X FA black 41 52 928 1989 bl cs 0 0 0 P01 + setcolor 969 1989 m 41 X 52 Y -41 X FA black 41 52 969 1989 bl cs 0 0 0 P01 + setcolor 1010 1989 m 42 X 52 Y -42 X FA black 42 52 1010 1989 bl cs 0 0 0 P01 + setcolor 1052 1989 m 41 X 52 Y -41 X FA black 41 52 1052 1989 bl cs 0 0 0 P01 + setcolor 1093 1989 m 41 X 52 Y -41 X FA black 41 52 1093 1989 bl cs 0 0 0 P01 + setcolor 1134 1989 m 41 X 52 Y -41 X FA black 41 52 1134 1989 bl cs 0 0 0 P01 + setcolor 1175 1989 m 41 X 52 Y -41 X FA black 41 52 1175 1989 bl cs 0 0 0 P01 + setcolor 1216 1989 m 42 X 52 Y -42 X FA black 42 52 1216 1989 bl cs 0 0 0 P01 + setcolor 1258 1989 m 41 X 52 Y -41 X FA black 41 52 1258 1989 bl cs 0 0 0 P01 + setcolor 1299 1989 m 41 X 52 Y -41 X FA black 41 52 1299 1989 bl cs 0 0 0 P01 + setcolor 1340 1989 m 41 X 52 Y -41 X FA black 41 52 1340 1989 bl cs 0 0 0 P01 + setcolor 1381 1989 m 42 X 52 Y -42 X FA black 42 52 1381 1989 bl cs 0 0 0 P01 + setcolor 1423 1989 m 41 X 52 Y -41 X FA black 41 52 1423 1989 bl cs 0 0 0 P01 + setcolor 1464 1989 m 41 X 52 Y -41 X FA black 41 52 1464 1989 bl cs 0 0 0 P01 + setcolor 1505 1989 m 41 X 52 Y -41 X FA black 41 52 1505 1989 bl cs 0 0 0 P01 + setcolor 1546 1989 m 42 X 52 Y -42 X FA black 42 52 1546 1989 bl cs 0 0 0 P01 + setcolor 1588 1989 m 41 X 52 Y -41 X FA black 41 52 1588 1989 bl cs 0 0 0 P01 + setcolor 1629 1989 m 41 X 52 Y -41 X FA black 41 52 1629 1989 bl cs 0 0 0 P01 + setcolor 1670 1989 m 41 X 52 Y -41 X FA black 41 52 1670 1989 bl cs 0 0 0 P01 + setcolor 1711 1989 m 42 X 52 Y -42 X FA black 42 52 1711 1989 bl cs 0 0 0 P01 + setcolor 1753 1989 m 41 X 52 Y -41 X FA black 41 52 1753 1989 bl cs 0 0 0 P01 + setcolor 1794 1989 m 41 X 52 Y -41 X FA black 41 52 1794 1989 bl cs 0 0 0 P01 + setcolor 1835 1989 m 41 X 52 Y -41 X FA black 41 52 1835 1989 bl cs 0 0 0 P01 + setcolor 1876 1989 m 41 X 52 Y -41 X FA black 41 52 1876 1989 bl cs 0 0 0 P01 + setcolor 1917 1989 m 42 X 52 Y -42 X FA black 42 52 1917 1989 bl cs 0 0 0 P01 + setcolor 1959 1989 m 41 X 52 Y -41 X FA black 41 52 1959 1989 bl cs 0 0 0 P01 + setcolor 2000 1989 m 41 X 52 Y -41 X FA black 41 52 2000 1989 bl + gr gr +showpage +end +%%EOF diff --git a/Magnet_Stations/11_10_2018_OPG/beamercolorthemeFlip.sty b/Magnet_Stations/11_10_2018_OPG/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Magnet_Stations/11_10_2018_OPG/beamerinnerthemeFlip.sty b/Magnet_Stations/11_10_2018_OPG/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Magnet_Stations/11_10_2018_OPG/beamerouterthemeFlip.sty b/Magnet_Stations/11_10_2018_OPG/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Magnet_Stations/11_10_2018_OPG/beamerouterthemedecolines.sty b/Magnet_Stations/11_10_2018_OPG/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Magnet_Stations/11_10_2018_OPG/beamerthemeFlip.sty b/Magnet_Stations/11_10_2018_OPG/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Magnet_Stations/11_10_2018_OPG/images/.DS_Store b/Magnet_Stations/11_10_2018_OPG/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/images/.DS_Store Binary files differ diff --git a/Magnet_Stations/11_10_2018_OPG/images/ATLAS.png b/Magnet_Stations/11_10_2018_OPG/images/ATLAS.png new file mode 100644 index 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-dUseCIEColor -dPDFSETTINGS=/printer -dSAFER -dNOPAUSE -dQUIET -dBATCH -sOutputFile="temp.pdf" "$f" + mv temp.pdf "$f" +# pdf2ps "$f" temp.ps +# ps2pdf temp.ps "$f" +# rm temp.ps +done +#rm temp.pdf diff --git a/Magnet_Stations/11_10_2018_OPG/images/directions.pdf b/Magnet_Stations/11_10_2018_OPG/images/directions.pdf new file mode 100644 index 0000000..3cf6bd8 --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/images/directions.pdf Binary files differ diff --git a/Magnet_Stations/11_10_2018_OPG/images/getFromAFS.sh b/Magnet_Stations/11_10_2018_OPG/images/getFromAFS.sh new file mode 100644 index 0000000..7d73a4a --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/images/getFromAFS.sh @@ -0,0 +1,4 @@ +kinit egraveri@CERN.CH +aklog +cp -r /afs/cern.ch/user/e/egraveri/cmtuser/STMonitoring/NewTTAlignment/Out/Plots/AlignVSSimCond-D0Align ./img/ +cp -r /afs/cern.ch/user/e/egraveri/cmtuser/STMonitoring/NewTTAlignment/Out/Plots/AlignVSSimCond-D0AlignNoTT ./img/ diff --git 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font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\TeV}{\mathrm{TeV}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mil +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} +\def\fixme{FIXME} + + + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + +\author{ {Marcin Chrzaszcz} (CERN)} +\institute{UZH} +\title[Special LHC run for Magnet Stations]{Special LHC run for Magnet Stations} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright \bfseries \Huge {Special LHC run for \\Magnet Stations} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.99\textwidth} +\center \vspace{-1.8em} {M. Bettler$^1$, J. Bhom$^2$ , P. Billoir$^3$, M. Chrzaszcz$^4$, C. Da Silva$^5$, M.Durham$^5$, R.Greim$^6$, W.Karpinskig$^6$, T.Kiring$^6$, M. Martinelli$^4$, M. Pikies$^2$\\~\\ +$^1$ Cambridge, $^2$ IFJ PAN, $^3$ LPNHE, $^4$ CERN, $^5$ LANL, $^6$ Aachen} + +\end{column} +%\begin{column}{0.53\textwidth} +%\includegraphics[height=1.3cm]{uzh-transp} +%\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{OPG, CERN, September 13, 2018} +\end{center} +\end{frame} +} + + + + +\begin{frame}\frametitle{Where our tracks are?} +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\ARROW The upstream tracks have rather poor momentum resolution: $\frac{\Delta p}{p} \sim 15\%$. \\ +\ARROW The particles die after short and sad (for physics) life in the magnet yoke. \\ +\ARROW If one put chambers in the magnet stations, one could record the particles before they death.\\ +\ARROW This will not increase the material budget of the rest of the detector.\\ +\begin{center} +\includegraphics[width=0.7\textwidth]{images/joke.png} +\end{center} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/sketch.png}\\ +\includegraphics[width=0.95\textwidth]{images/magnet.png} + + + +\end{columns} +\end{frame} + + + + +\begin{frame}\frametitle{Studies done so far} + +\ARROW We have performed studies: +\begin{itemize} +\item Radiation: Dosimeters have been put in the magnet region to measure the radiation dose. +\item For sensitivity studies the MC was used. +\end{itemize} + +\ARROW These of course are important studies but having a data driven method is the best. + +\begin{columns} + +\column{0.5\textwidth} + +\ARROW Often our MC prediction are wrong ;) + +\column{0.5\textwidth} +\includegraphics[width=0.9\textwidth]{images/ATLAS.png} + +\end{columns} + + +\end{frame} + +\begin{frame}\frametitle{The proposal} + + +\ARROW We would like to propose of obtaining a sample of lower $p_T$ tracks from data.\\ +\ARROW There are essentially two possibilities: (many thanks to Niels for discussion and guidance): +\begin{itemize} +\item Make a run with a $50~\%$ of magnetic field. +\begin{itemize} +\item {\color{green}{Direct access to particles that would be swapped by magnet.}} +\item {\color{green}{Not much work on our side}} +\item {\color{red}{Needs additional 10-12h for machine to understand our magnetic field.}} +\end{itemize} +\item Run with nominal magnet and open the OT. +\begin{itemize} +\item {\color{green}{No work for the LHC people.}} +\item {\color{red}{Needs some extrapolation on our side.}} +\item {\color{red}{Needs 1-2h access to open the OT.}} + +\end{itemize} + +\end{itemize} + + + +\end{frame} + + + +\begin{frame}\frametitle{The golden question} + + +\begin{alertblock}{} +How much to open the OT, how much coverage/gain you get? +\end{alertblock} + +\ARROW This is a hard one ;) and took a bit of time to answer.\\ +\ARROW We made two types of simulation: +\begin{enumerate} +\item Open the OT fully. +\item Make a half magnetic field +\end{enumerate} + + +\end{frame} + +\begin{frame}\frametitle{Opened OT} + +\begin{columns} + +\column{0.5\textwidth} +\ARROW Efficiency gain:\\ +\includegraphics[width=0.99\textwidth]{OpenOT_zoom.eps} + +\column{0.5\textwidth} +\ARROW Slow pions from $\PDstar$:\\ +\includegraphics[angle=-90,width=0.99\textwidth]{out.pdf} + + +\end{columns} + + +\end{frame} + +\begin{frame}\frametitle{Half magnetic field, closed OT} + +\begin{columns} + +\column{0.5\textwidth} +\ARROW Efficiency gain:\\ +\includegraphics[width=0.99\textwidth]{ClosedOT_halffield.eps} + +\column{0.5\textwidth} +\ARROW Slow pions from $\PDstar$:\\ +\includegraphics[angle=-90,width=0.99\textwidth]{out.pdf} + + +\end{columns} + + +\end{frame} + + + + + + +\begin{frame}\frametitle{Conclusions} + +\ARROW The half magnetic field is more expensive but buys us more phase space. \\ +\ARROW The open OT is ''cheaper'' but doesn't dig in the most sensitive region. + + +\end{frame} + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Magnet_Stations/11_10_2018_OPG/mchrzasz.toc b/Magnet_Stations/11_10_2018_OPG/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Magnet_Stations/11_10_2018_OPG/out.pdf b/Magnet_Stations/11_10_2018_OPG/out.pdf new file mode 100644 index 0000000..d304d49 --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/out.pdf Binary files differ diff --git a/Magnet_Stations/11_10_2018_OPG/tikzfeynman.sty b/Magnet_Stations/11_10_2018_OPG/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Magnet_Stations/11_10_2018_OPG/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Magnet_Stations/13_09_2018_OPG/Makefile b/Magnet_Stations/13_09_2018_OPG/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Magnet_Stations/13_09_2018_OPG/beamercolorthemeFlip.sty b/Magnet_Stations/13_09_2018_OPG/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Magnet_Stations/13_09_2018_OPG/beamerinnerthemeFlip.sty b/Magnet_Stations/13_09_2018_OPG/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Magnet_Stations/13_09_2018_OPG/beamerouterthemeFlip.sty b/Magnet_Stations/13_09_2018_OPG/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Magnet_Stations/13_09_2018_OPG/beamerouterthemedecolines.sty b/Magnet_Stations/13_09_2018_OPG/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Magnet_Stations/13_09_2018_OPG/beamerthemeFlip.sty b/Magnet_Stations/13_09_2018_OPG/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Magnet_Stations/13_09_2018_OPG/images/.DS_Store b/Magnet_Stations/13_09_2018_OPG/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/images/.DS_Store Binary files differ diff --git a/Magnet_Stations/13_09_2018_OPG/images/ATLAS.png b/Magnet_Stations/13_09_2018_OPG/images/ATLAS.png new file mode 100644 index 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biblatex.cfg + english.lbx + + + + bibtex + + bibtex + + mchrzasz + + + mchrzasz.aux + + + mchrzasz.bbl + + + mchrzasz.bbl + + + mchrzasz.aux + mchrzasz-blx.bib + + + bib.bib + + + biblatex.bst + + + diff --git a/Magnet_Stations/13_09_2018_OPG/mchrzasz.snm b/Magnet_Stations/13_09_2018_OPG/mchrzasz.snm new file mode 100644 index 0000000..e69de29 --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/mchrzasz.snm diff --git a/Magnet_Stations/13_09_2018_OPG/mchrzasz.synctex.gz b/Magnet_Stations/13_09_2018_OPG/mchrzasz.synctex.gz new file mode 100644 index 0000000..30768b1 --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/mchrzasz.synctex.gz Binary files differ diff --git a/Magnet_Stations/13_09_2018_OPG/mchrzasz.tex b/Magnet_Stations/13_09_2018_OPG/mchrzasz.tex new file mode 100644 index 0000000..ba7ed6c --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/mchrzasz.tex @@ -0,0 +1,380 @@ +\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} + +\usepackage[english]{babel} +\usepackage{polski} + + +\usetheme[ + bullet=circle, % Other option: square + bigpagenumber, % circled page number on lower right + topline=true, % colored bar at the top of the frame + shadow=false, % Shading for beamer blocks + watermark=BG_lower, % png file for the watermark + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\TeV}{\mathrm{TeV}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mil +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} +\def\fixme{FIXME} + + + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + +\author{ {Marcin Chrzaszcz} (CERN)} +\institute{UZH} +\title[Special LHC run for Magnet Stations]{Special LHC run for Magnet Stations} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright \bfseries \Huge {Special LHC run for \\Magnet Stations} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.99\textwidth} +\center \vspace{-1.8em} {M. Bettler$^1$, J. Bhom$^2$ , P. Billoir$^3$, M. Chrzaszcz$^4$, C. Da Silva$^5$, M.Durham$^5$, R.Greim$^6$, W.Karpinskig$^6$, T.Kiring$^6$, M. Martinelli$^4$, M. Pikies$^2$\\~\\ +$^1$ Cambridge, $^2$ IFJ PAN, $^3$ LPNHE, $^4$ CERN, $^5$ LANL, $^6$ Aachen} + +\end{column} +%\begin{column}{0.53\textwidth} +%\includegraphics[height=1.3cm]{uzh-transp} +%\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{OPG, CERN, September 13, 2018} +\end{center} +\end{frame} +} + + + + +\begin{frame}\frametitle{Where our tracks are?} +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\ARROW The upstream tracks have rather poor momentum resolution: $\frac{\Delta p}{p} \sim 15\%$. \\ +\ARROW The particles die after short and sad (for physics) life in the magnet yoke. \\ +\ARROW If one put chambers in the magnet stations, one could record the particles before they death.\\ +\ARROW This will not increase the material budget of the rest of the detector.\\ +\begin{center} +\includegraphics[width=0.7\textwidth]{images/joke.png} +\end{center} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/sketch.png}\\ +\includegraphics[width=0.95\textwidth]{images/magnet.png} + + + +\end{columns} +\end{frame} + + + + +\begin{frame}\frametitle{Studies done so far} + +\ARROW We have performed studies: +\begin{itemize} +\item Radiation: Dosimeters have been put in the magnet region to measure the radiation dose. +\item For sensitivity studies the MC was used. +\end{itemize} + +\ARROW These of course are important studies but having a data driven method is the best. + +\begin{columns} + +\column{0.5\textwidth} + +\ARROW Often our MC prediction are wrong ;) + +\column{0.5\textwidth} +\includegraphics[width=0.9\textwidth]{images/ATLAS.png} + +\end{columns} + + +\end{frame} + +\begin{frame}\frametitle{The proposal} + + +\ARROW We would like to propose of obtaining a sample of lower $p_T$ tracks from data.\\ +\ARROW There are essentially two possibilities: (many thanks to Niels for discussion and guidance): +\begin{itemize} +\item Make a run with a $50~\%$ of magnetic field. +\begin{itemize} +\item {\color{green}{Direct access to particles that would be swapped by magnet.}} +\item {\color{green}{Not much work on our side}} +\item {\color{red}{Needs additional 10-12h for machine to understand our magnetic field.}} +\end{itemize} +\item Run with nominal magnet and open the OT. +\begin{itemize} +\item {\color{green}{No work for the LHC people.}} +\item {\color{red}{Needs some extrapolation on our side.}} +\item {\color{red}{Needs 1-2h access to open the OT.}} + +\end{itemize} + +\end{itemize} + +\begin{alertblock}{Our suggestion} +We would propose to go with the second option not to disturb the LHC. \\ +For LHCb we would sacrifice one full fill. +\end{alertblock} + + + +\end{frame} + + + +\begin{frame}\frametitle{The proposal -time table} +\begin{center} +\includegraphics[width=0.99\textwidth]{images/OPEN.png} +\end{center} + + +\ARROW We proposed to have the last Fill of pp collisions with OT opened.\\ +\ARROW There is a stop after it so we can close OT without any beam lost.\\ +\ARROW We would need only around 2h to open the OT. + +\begin{alertblock}{} +Please let us know what you think about this proposal. +\end{alertblock} + + +\end{frame} + + + + + + + + + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Magnet_Stations/13_09_2018_OPG/mchrzasz.toc b/Magnet_Stations/13_09_2018_OPG/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Magnet_Stations/13_09_2018_OPG/tikzfeynman.sty b/Magnet_Stations/13_09_2018_OPG/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Magnet_Stations/13_09_2018_OPG/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Magnet_Stations/14_02_2019_review/Makefile b/Magnet_Stations/14_02_2019_review/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Magnet_Stations/14_02_2019_review/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Magnet_Stations/14_02_2019_review/beamercolorthemeFlip.sty b/Magnet_Stations/14_02_2019_review/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Magnet_Stations/14_02_2019_review/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Magnet_Stations/14_02_2019_review/beamerinnerthemeFlip.sty b/Magnet_Stations/14_02_2019_review/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Magnet_Stations/14_02_2019_review/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Magnet_Stations/14_02_2019_review/beamerouterthemeFlip.sty b/Magnet_Stations/14_02_2019_review/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Magnet_Stations/14_02_2019_review/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Magnet_Stations/14_02_2019_review/beamerouterthemedecolines.sty b/Magnet_Stations/14_02_2019_review/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Magnet_Stations/14_02_2019_review/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Magnet_Stations/14_02_2019_review/beamerthemeFlip.sty b/Magnet_Stations/14_02_2019_review/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Magnet_Stations/14_02_2019_review/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Magnet_Stations/14_02_2019_review/images/.DS_Store b/Magnet_Stations/14_02_2019_review/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/Magnet_Stations/14_02_2019_review/images/.DS_Store Binary files differ diff --git a/Magnet_Stations/14_02_2019_review/images/BG_both.png b/Magnet_Stations/14_02_2019_review/images/BG_both.png new file 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Bettler$^1$, J. Bhom$^2$, P. Billoir$^3$, M. Chrzaszcz$^4$, C. Da Silva$^5$, M.Durham$^5$, R.Greim$^6$, W.Karpinskig$^6$, T.Kiring$^6$, M. Martinelli$^6$,\\~\\ +$^1$ Cambridge, $^2$ IFJ PAN, $^3$ LPNHE, $^4$ CERN, $^5$ LANL, $^6$ Aachen, $^7$ EPFL, $^8$ IFJ PAN} + +\end{column} +%\begin{column}{0.53\textwidth} +%\includegraphics[height=1.3cm]{uzh-transp} +%\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{Magnet Side Stations - U2PG Review, February 14, 2019} +\end{center} +\end{frame} +} + + + +\begin{frame}\frametitle{Outline} + +\ARROW Introduction\\ +\ARROW We will review the effect of an improved tracking for specific channels: +\begin{itemize} +\item Prompt Charm decays +%\item $\PD \to 5 \pi$ +\item $R(\Lambda_c^{\ast})$ +\item $R(\PDstar)$ +\item Multibody $\PB$ decays +\item $\Sigma_b$. +\item $\PB^{\ast}$. +\item Gluon PDF. +\item Spectroscopy. +\end{itemize} +\ARROW Tracking implementations.\\ +\ARROW Outlook + + +\end{frame} + + +\begin{frame}\frametitle{The idea} +\begin{center} +\includegraphics[width=0.65\textwidth]{images/mag.png} +\end{center} +\ARROW Tracks with hits in the vertex locator and the TT/UT and not in the Tstations: UPSTREAM tracks.\\ +\ARROW Those are bend outside of the T-stations acceptance by the magnetic field because of their low-momentum.\\ +\ARROW The reduced amount of field between the VELO and the TT, means that their momentum is computed with a large uncertainty. +$\Delta p/p = 20-25\%$ current, $\Delta p/p = 15-20\%$ upgrade +\end{frame} + +\begin{frame}\frametitle{Proposal} +\only<1>{ +\ARROW Original idea comes from Sheldon Stone, Paolo Gandini, Liming Zhang: \href{https://indico.cern.ch/event/327376/contributions/1713479/}{{\color{blue}[Tuesday meeting Sept 2nd 2014]}}\\ +\begin{center} +\includegraphics[width=0.65\textwidth]{images/stations.png} +\end{center} +\ARROW It is outside the LHCb acceptancen!! No $X_0$ added.\\ +\ARROW No need to have a high resolution. $\mathcal{O}(1\rm mm)$ should be enough.\\ +} + +\end{frame} + +\iffalse + +\begin{frame}\frametitle{Where our tracks are?} +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\ARROW The upstream tracks have rather poor momentum resolution: $\frac{\Delta p}{p} \sim 15\%$. \\ +\ARROW The particles die after short and sad (for physics) life in the magnet yoke. \\ +\ARROW If one put chambers in the magnet stations, one could record the particles before they death.\\ +\ARROW This will not increase the material budget of the rest of the detector.\\ +\begin{center} +\includegraphics[width=0.7\textwidth]{images/joke.png} +\end{center} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/sketch.png}\\ +\includegraphics[width=0.95\textwidth]{images/magnet.png} + + + +\end{columns} +\end{frame} + + +\begin{frame}\frametitle{Physics interest} +\begin{small} +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\ARROW We have enormous amount of channels where we have slow particles: +\begin{itemize} +\item $\PDstar \to \PD \pi$. +\item $\Lambda_c(2595, 2625) \to \Lambda_c \pi \pi$. +\item All the $\PB^{\ast \ast}$ decays! $\leftarrowtail$ huge community interests!!! +\item As well other states: $\Sigma_b \to \Lambda_b \pi$. +\item Little is known about the excited $\PBs$ states as well. + +\end{itemize} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/charmS.png}\\ + + + +\end{columns} +\end{small} +\end{frame} + + +\fi + +\begin{frame}\frametitle{The sensitivity study} + +\begin{columns} +\column{0.4\textwidth} +\ARROW Take the Gauss \texttt{v50r0} for upgrade.\\ +\ARROW Simulate the particle gun.\\ +\ARROW Decays particles with \texttt{EvtGen}.\\ +\ARROW Put for now a plates in the Magnet (and beyond) and see where the particles hit them.\\ +\ARROW $\nu=7.6$. + +\column{0.6\textwidth} +\includegraphics[width=0.95\textwidth]{images/mag3.png} +\end{columns} + + +\end{frame} + +\begin{frame}\frametitle{Current Physics cases} + +\begin{columns} +\column{0.6\textwidth} + +\begin{itemize} +\item Gains:\\ +\ARROW $\PDstar \to \PD (\pi \PK) \pi_{\rm slow}$: {\color{JungleGreen}gain $21~\%$.}\\ +\ARROW $\PB \to \tau \tau$: {\color{JungleGreen}gain: $24~\%$.}\\ +\ARROW $R(\Lambda_c^{\ast})= \frac{\mathcal{B}(\Lambda_b \to \Lambda_c^{\ast} \tau \nu) }{\mathcal{B}(\Lambda_b \to \Lambda_c^{\ast} \mu \nu)}$, $\Lambda_c^{\ast} \to p \pi_{\rm slow} \pi_{\rm slow}$ : {\color{JungleGreen}gain $60~\%$.}\\ +\ARROW $R(D^{\ast})= \frac{\mathcal{B}( \PB \to \PD^{\ast} \tau \nu) }{\mathcal{B}( \PB \to \PD^{\ast} \tau \nu) }$: {\color{JungleGreen}gain $26~\%$.}\\ +\ARROW $\PB \to n\PK$: {\color{JungleGreen}gain $10-50~\%$.}\\ +\ARROW $\Sigma_b \to \Lambda_b \pi$: {\color{JungleGreen}gain $29~\%$.}\\ +\ARROW Gluon PDF: {\color{JungleGreen} Enabled measurement.}\\ + +\end{itemize} +\includegraphics[width=0.9\textwidth]{images/pdf.png} + +\column{0.5\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{images/nk.pdf}\\ +\includegraphics[width=0.9\textwidth]{images/gluon22.png} + + + +\end{columns} + +\end{frame} + + + +\begin{frame}\frametitle{Additional Physics cases} +\only<1> +{ +\begin{columns} +\column{0.6\textwidth} + +\begin{itemize} +\item Additional:\\ +\ARROW $\Sigma_c \to \Lambda_c \pi_{\rm slow}$: {\color{JungleGreen}gain $19~\%$.}\\ +\ARROW Low-mass Drell-Yan: {\color{JungleGreen}gain $15~\%$.}\\ +\ARROW $\PBc(2S) \to \PBc \pi_{\rm slow} \pi_{\rm slow}$: {\color{JungleGreen}gain $50~\%$.}\\ +\ARROW Radiative decays? + +\end{itemize} + +\column{0.5\textwidth} +\href{https://journals.aps.org/prd/pdf/10.1103/PhysRevD.70.054017}{{\color{blue}{S.Godfrey, PHYSICAL REVIEW D 70 054017}}} +\includegraphics[width=0.95\textwidth]{images/spec2.png} + + + +\end{columns} +} +\only<2>{ +\ARROW This is just the tip of the ice berg!\\ +\begin{center} +\includegraphics[width=0.95\textwidth]{images/spec3.png} + +\end{center} + +} + + + +\end{frame} + + + + + + +\begin{frame} + + +\begin{center} + +\begin{Huge} +Tracking studies +\end{Huge} +\end{center} + +\end{frame} + + +\begin{frame}\frametitle{2-fold Runge-Kutta for MS,~~~~P.Billoir} +\begin{center} +\includegraphics[width=0.9\textwidth]{images/RK2.png} + +\end{center} +\ARROW We start from ,,standard'' Runge-Kutta method.\\ +\ARROW If $\vert t_x \vert>1$ we switch steps to $x$.\\ +\ARROW With VELO + UT we know precisely: $x$, $y$, $t_x$, $t_y$. We poorly know: $\dfrac{q}{p} \rightarrow $ MS can help.\\ +\ARROW Runge-Kutta method has to be inverted with the Newton-Raphson method. + +\end{frame} + +\begin{frame}\frametitle{2-fold Runge-Kutta for MS,~~~~P.Billoir} +\begin{center} +\includegraphics[width=0.8\textwidth]{images/MS2.png}\\ +\includegraphics[width=0.8\textwidth]{images/MS1.png} + +\end{center} + + +\end{frame} + + +\begin{frame} + + +\begin{center} + +\begin{Huge} +Detector Implementation +\end{Huge} +\end{center} + +\end{frame} + + +\begin{frame}\frametitle{Gauss implementation} +\begin{center} +\includegraphics[width=0.7\textwidth]{images/imp.png}\\ + +\end{center} +\ARROW Cloned structures of the SciFi.\\ +\ARROW Digitalization missing.\\\ +\ARROW Run full MC simulations. + +\end{frame} + + + + + +\iffalse +\begin{frame}\frametitle{Prompt charm decays} + +\ARROW Study the prompt production: $\PDstar \to \PD (\pi \PK) \pi_{\rm slow}$. +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $K$, $\pi$ in UT + FT +\item Slow $\pi$ hits UT + MS and $K$, $\pi$ in UT + FT +\end{itemize} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 20.7\% +\end{align*} + +\end{small} + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_Dstar}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_Dstar}.pdf} + +\end{columns} + + + + +\end{frame} + + + +\begin{frame}\frametitle{$\Lambda_b \to \Lambda_c^{\ast} \tau \nu$} + +\ARROW Study the LUV in: $\Lambda_b \to \Lambda_c^{\ast} \tau \nu$ +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Two slow $\pi$ hits UT + FT and p, $K$, $\pi$ in UT + FT +\item One slow $\pi$ hits UT + MS(FT) and p, $K$, $\pi$ in UT + FT +\item Two slow $\pi$ hits UT + MS and p, $K$, $\pi$ in UT + FT +\end{itemize} +\end{small} + +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 60.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_Lcstar}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_Lcstar}.pdf} + +\end{columns} + + + +\end{frame} + + + +\begin{frame}\frametitle{$\PB \to \PDstar \tau \nu$} + +\ARROW Study the LUV in: $\PB \to \PDstar \tau \nu$ +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $K$, $\pi$ in UT + FT +\item Slow $\pi$ hits UT + MS and $K$, $\pi$ in UT + FT +\end{itemize} +\end{small} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 26.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_DstarB}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_DstarB}.pdf} + +\end{columns} + + + +\end{frame} + + + +\begin{frame}\frametitle{$\PB \to n \PK$} + +\ARROW Study the multi body decays: $\PB \to n \PK$: +\begin{center} +\includegraphics[angle=-90,width=0.75\textwidth]{images/nk.pdf} +\end{center} +\ARROW Clearly a threshold effect, the less PHSP you have the more you gain. + + +\end{frame} + + + +\iffalse +\begin{frame}\frametitle{$\PD \to 5 \PK$} + +\begin{columns} +\column{0.6\textwidth} +\ARROW Similar is expected to $\PD \PD$ searches. +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $K$, $\pi$ in UT + FT +\item Slow $\pi$ hits UT + MS and $K$, $\pi$ in UT + FT +\end{itemize} +\end{small} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 26.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_DstarB}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_DstarB}.pdf} + +\end{columns} + + + +\end{frame} +\fi + +\begin{frame}\frametitle{$\Sigma_b \to \Lambda_b \pi$} + +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $\Lambda_c$, $D_s$ in UT + FT +\item Slow $\pi$ hits UT + MS and $\Lambda_c$, $D_s$ in UT + FT +\end{itemize} +\end{small} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 29.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_DstarB}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_DstarB}.pdf} + +\end{columns} + + + +\end{frame} + + + + + + +\begin{frame}\frametitle{Gluon PDF} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/gluon.png} +\end{center} +\ARROW The Gluon PDF saturates the low momentum transfer and fractional momentum. + +\end{frame} + +\begin{frame}\frametitle{Gluon PDF} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/gluon22.png} +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{Gluon PDF efficiency} + +\ARROW If one looks at the efficiency for the low tracks, one finds where is the improvement: + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/pdf.png} +\end{center} + +\ARROW For more details see \href{https://indico.cern.ch/event/557554/contributions/2247267/attachments/1423140/2181806/gluon_saturation_seminar.pdf}{{\color{blue}Cesar Luiz da Silva; Tuesday Presentation}} + + +\end{frame} + + +\begin{frame}\frametitle{Spectroscopy} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/spec.png} +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{Idea from this workshop: $\PB \to \tau \tau$} + +\ARROW LHCb has recently measured: $\PB_{s/d} \to \tau \tau$~\href{https://arxiv.org/abs/1703.02508}{\color{blue}arXiv::1703.02508}\\ + +\begin{columns} + +\column{0.6\textwidth} +\includegraphics[width=0.95\textwidth]{images/bstautau.pdf} + + +\column{0.4\textwidth} + +\includegraphics[width=0.95\textwidth]{images/Bstautau2.png} + +\end{columns} + +\ARROW As a multibody decay it will probably have non-negligable gain from MS.\\ +\ARROW From preliminary studies $\mathcal{O}(24)\%$ gain. + + +\end{frame} + + +\begin{frame}\frametitle{Soft bomb events} + +\ARROW All credits to Zoltan Ligeti.\\ +\ARROW Based on paper:\href{https://arxiv.org/pdf/1612.00850.pdf?fname=cm&font=TypeI}{\color{blue}arXiv::1612.00850} + +\includegraphics[width=0.99\textwidth]{images/bomb.png} + +\ARROW The paper gives a lot of information how to select such events $\color{blue}\rightarrow$ Need new MC study. + +\end{frame} + + +\fi + + + +\begin{frame}\frametitle{Outlook} + +\ARROW The physics program of magnet stations is growing.\\ +\ARROW For many channels, the MS are improving the efficiencies from ~$20-30\% (R(D^{\ast}))$ to $60\%$.\\ +\ARROW For other, such as the study of Gluon saturation, the MS are enabling the measurement.\\ +\ARROW MS help when little PHSP is available.\\ +\ARROW Spectroscopy measurements enhanced.\\ +\ARROW Tagging of charm meson and baryon decays $\rightarrow$ reduce background.\\{~}\\ +\ARROW Tracking algorithms are being developed.\\ +\ARROW Implementing the MS in Gauss. + + + +\end{frame} + + + + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Magnet_Stations/14_02_2019_review/mchrzasz.toc b/Magnet_Stations/14_02_2019_review/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Magnet_Stations/14_02_2019_review/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Magnet_Stations/14_02_2019_review/tikzfeynman.sty b/Magnet_Stations/14_02_2019_review/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Magnet_Stations/14_02_2019_review/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Magnet_Stations/21_03_2018_annecy/Makefile b/Magnet_Stations/21_03_2018_annecy/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Magnet_Stations/21_03_2018_annecy/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Magnet_Stations/21_03_2018_annecy/beamercolorthemeFlip.sty b/Magnet_Stations/21_03_2018_annecy/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Magnet_Stations/21_03_2018_annecy/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Magnet_Stations/21_03_2018_annecy/beamerinnerthemeFlip.sty b/Magnet_Stations/21_03_2018_annecy/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Magnet_Stations/21_03_2018_annecy/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Magnet_Stations/21_03_2018_annecy/beamerouterthemeFlip.sty b/Magnet_Stations/21_03_2018_annecy/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Magnet_Stations/21_03_2018_annecy/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Magnet_Stations/21_03_2018_annecy/beamerouterthemedecolines.sty b/Magnet_Stations/21_03_2018_annecy/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Magnet_Stations/21_03_2018_annecy/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Magnet_Stations/21_03_2018_annecy/beamerthemeFlip.sty b/Magnet_Stations/21_03_2018_annecy/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Magnet_Stations/21_03_2018_annecy/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Magnet_Stations/21_03_2018_annecy/images/.DS_Store b/Magnet_Stations/21_03_2018_annecy/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/Magnet_Stations/21_03_2018_annecy/images/.DS_Store Binary files differ diff --git a/Magnet_Stations/21_03_2018_annecy/images/BG_both.png b/Magnet_Stations/21_03_2018_annecy/images/BG_both.png new file 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Bettler$^1$, P. Billoir$^2$, M. Chrzaszcz$^3$, C. Da Silva$^4$, M.Durham$^4$, R.Greim$^5$, W.Karpinskig$^5$, T.Kiring$^5$, M. Martinelli$^6$, M. Pikies$^7$\\~\\ +$^1$ Cambridge, $^2$ LPNHE, $^3$ CERN, $^4$ LANL, $^5$ Aachen, $^6$ EPFL, $^7$ IFJ PAN} + +\end{column} +%\begin{column}{0.53\textwidth} +%\includegraphics[height=1.3cm]{uzh-transp} +%\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{Upgrade II meeting, Annecy, March 21, 2018} +\end{center} +\end{frame} +} + + + +\begin{frame}\frametitle{Outline} + +\ARROW Introduction\\ +\ARROW We will review the effect of an improved tracking for specific channels: +\begin{itemize} +\item Prompt Charm decays +%\item $\PD \to 5 \pi$ +\item $R(\Lambda_c^{\ast})$ +\item $R(\PDstar)$ +\item Multibody $\PB$ decays +\item $\Sigma_b$. +\item $\PB^{\ast}$. +\item Gluon PDF. +\item Spectroscopy. +\end{itemize} +\ARROW Tracking implementations.\\ +\ARROW Outlook + + +\end{frame} + + + +\begin{frame}\frametitle{Previous reports} + +\begin{itemize} +\item Elba, Phase-II workshop:\\ +\href{https://agenda.infn.it/getFile.py/access?contribId=19&sessionId=3&resId=0&materialId=slides&confId=12253}{ {\color{blue}M. Martineli talk}} +\item Elba, Phase-II workshop:\\ +\href{https://agenda.infn.it/getFile.py/access?contribId=20&sessionId=3&resId=0&materialId=slides&confId=12253}{ {\color{blue}M. Chrzaszcz talk}} +\item Manchester, Phase-II workshop:\\ +\href{https://indico.cern.ch/event/481359/contributions/1157520/attachments/1253747/1849859/Bettler_MAN.pdf}{ {\color{blue}M. Better talk}} +\item Manchester, Phase-II workshop:\\ +\href{https://indico.cern.ch/event/481359/contributions/1157519/attachments/1253525/1849467/MagnetStationsSimulation.pdf}{ {\color{blue}I. Babushkin talk}} +\item Manchester, Phase-II workshop:\\ +\href{https://indico.cern.ch/event/481359/contributions/1157526/attachments/1253827/1850013/UpstreamTracksPotential.pdf +}{ {\color{blue}M. Martinelli talk}} +\item Tuesday Presentation\\ + \href{https://indico.cern.ch/event/557554/contributions/2247267/attachments/1423140/2181806/gluon_saturation_seminar.pdf}{{\color{blue}Cesar Luiz da Silva talk}} + +\end{itemize} + +\end{frame} + + + +\begin{frame}\frametitle{The idea} +\begin{center} +\includegraphics[width=0.65\textwidth]{images/mag.png} +\end{center} +\ARROW Tracks with hits in the vertex locator and the TT/UT and not in the Tstations: UPSTREAM tracks.\\ +\ARROW Those are bend outside of the T-stations acceptance by the magnetic field because of their low-momentum.\\ +\ARROW The reduced amount of field between the VELO and the TT, means that their momentum is computed with a large uncertainty. +$\Delta p/p = 20-25\%$ current, $\Delta p/p = 15-20\%$ upgrade +\end{frame} + +\begin{frame}\frametitle{Proposal} +\only<1>{ +\ARROW Original idea comes from Sheldon Stone, Paolo Gandini, Liming Zhang: \href{https://indico.cern.ch/event/327376/contributions/1713479/}{{\color{blue}[Tuesday meeting Sept 2nd 2014]}}\\ +\begin{center} +\includegraphics[width=0.65\textwidth]{images/stations.png} +\end{center} +\ARROW It is outside the LHCb acceptancen!! No $X_0$ added.\\ +\ARROW No need to have a high resolution. $\mathcal{O}(1\rm mm)$ should be enough.\\ +} +\only<2>{ + +\begin{center} +\includegraphics[width=0.75\textwidth]{images/sheldon.png} +\end{center} + +} + +\end{frame} + +\iffalse + +\begin{frame}\frametitle{Where our tracks are?} +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\ARROW The upstream tracks have rather poor momentum resolution: $\frac{\Delta p}{p} \sim 15\%$. \\ +\ARROW The particles die after short and sad (for physics) life in the magnet yoke. \\ +\ARROW If one put chambers in the magnet stations, one could record the particles before they death.\\ +\ARROW This will not increase the material budget of the rest of the detector.\\ +\begin{center} +\includegraphics[width=0.7\textwidth]{images/joke.png} +\end{center} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/sketch.png}\\ +\includegraphics[width=0.95\textwidth]{images/magnet.png} + + + +\end{columns} +\end{frame} + + +\begin{frame}\frametitle{Physics interest} +\begin{small} +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\ARROW We have enormous amount of channels where we have slow particles: +\begin{itemize} +\item $\PDstar \to \PD \pi$. +\item $\Lambda_c(2595, 2625) \to \Lambda_c \pi \pi$. +\item All the $\PB^{\ast \ast}$ decays! $\leftarrowtail$ huge community interests!!! +\item As well other states: $\Sigma_b \to \Lambda_b \pi$. +\item Little is known about the excited $\PBs$ states as well. + +\end{itemize} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/charmS.png}\\ + + + +\end{columns} +\end{small} +\end{frame} + + +\fi + +\begin{frame}\frametitle{The sensitivity study} + +\begin{columns} +\column{0.4\textwidth} +\ARROW Take the Gauss \texttt{v50r0} for upgrade.\\ +\ARROW Simulate the particle gun.\\ +\ARROW Decays particles with \texttt{EvtGen}.\\ +\ARROW Put for now a plates in the Magnet (and beyond) and see where the particles hit them.\\ +\ARROW $\nu=7.6$. + +\column{0.6\textwidth} +\includegraphics[width=0.95\textwidth]{images/mag3.png} +\end{columns} + + +\end{frame} + +\begin{frame}\frametitle{Current Physics cases} + +\begin{columns} +\column{0.6\textwidth} + +\begin{itemize} +\item Previously reported:\\ +\ARROW $\PDstar \to \PD (\pi \PK) \pi_{\rm slow}$: {\color{JungleGreen}gain $21~\%$.}\\ +\ARROW $\PB \to \tau \tau$: {\color{JungleGreen}gain: $24~\%$.}\\ +\ARROW $R(\Lambda_c^{\ast})= \frac{\mathcal{B}(\Lambda_b \to \Lambda_c^{\ast} \tau \nu) }{\mathcal{B}(\Lambda_b \to \Lambda_c^{\ast} \mu \nu)}$, $\Lambda_c^{\ast} \to p \pi_{\rm slow} \pi_{\rm slow}$ : {\color{JungleGreen}gain $60~\%$.}\\ +\ARROW $R(D^{\ast})= \frac{\mathcal{B}( \PB \to \PD^{\ast} \tau \nu) }{\mathcal{B}( \PB \to \PD^{\ast} \tau \nu) }$: {\color{JungleGreen}gain $26~\%$.}\\ +\ARROW $\PB \to n\PK$: {\color{JungleGreen}gain $10-50~\%$.}\\ +\ARROW $\Sigma_b \to \Lambda_b \pi$: {\color{JungleGreen}gain $29~\%$.}\\ +\ARROW Gluon PDF: {\color{JungleGreen} Enabled measurement.}\\ + +\end{itemize} +\includegraphics[width=0.9\textwidth]{images/pdf.png} + +\column{0.5\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{images/nk.pdf}\\ +\includegraphics[width=0.9\textwidth]{images/gluon22.png} + + + +\end{columns} + +\end{frame} + + + +\begin{frame}\frametitle{Additional Physics cases} +\only<1> +{ +\begin{columns} +\column{0.6\textwidth} + +\begin{itemize} +\item Newly reported:\\ +\ARROW $\Sigma_c \to \Lambda_c \pi_{\rm slow}$: {\color{JungleGreen}gain $19~\%$.}\\ +\ARROW Low-mass Drell-Yan: {\color{JungleGreen}gain $15~\%$.}\\ +\ARROW $\PBc(2S) \to \PBc \pi_{\rm slow} \pi_{\rm slow}$: {\color{JungleGreen}gain $50~\%$.}\\ + +\end{itemize} + +\column{0.5\textwidth} +\href{https://journals.aps.org/prd/pdf/10.1103/PhysRevD.70.054017}{{\color{blue}{S.Godfrey, PHYSICAL REVIEW D 70 054017}}} +\includegraphics[width=0.95\textwidth]{images/spec2.png} + + + +\end{columns} +} +\only<2>{ +\ARROW This is just the tip of the ice berg!\\ +\begin{center} +\includegraphics[width=0.95\textwidth]{images/spec3.png} + +\end{center} + +} + + + +\end{frame} + + + + + + +\begin{frame} + + +\begin{center} + +\begin{Huge} +Tracking studies +\end{Huge} +\end{center} + +\end{frame} + + +\begin{frame}\frametitle{2-fold Runge-Kutta for MS,~~~~P.Billoir} +\begin{center} +\includegraphics[width=0.9\textwidth]{images/RK2.png} + +\end{center} +\ARROW We start from ,,standard'' Runge-Kutta method.\\ +\ARROW If $\vert t_x \vert>1$ we switch steps to $x$.\\ +\ARROW With VELO + UT we know precisely: $x$, $y$, $t_x$, $t_y$. We poorly know: $\dfrac{q}{p} \rightarrow $ MS can help.\\ +\ARROW Runge-Kutta method has to be inverted with the Newton-Raphson method. + +\end{frame} + +\begin{frame}\frametitle{2-fold Runge-Kutta for MS,~~~~P.Billoir} +\begin{center} +\includegraphics[width=0.8\textwidth]{images/MS2.png}\\ +\includegraphics[width=0.8\textwidth]{images/MS1.png} + +\end{center} + + +\end{frame} + + +\begin{frame} + + +\begin{center} + +\begin{Huge} +Detector Implementation +\end{Huge} +\end{center} + +\end{frame} + + +\begin{frame}\frametitle{Gauss implementation,~~~~M. Pikies} +\begin{center} +\includegraphics[width=0.7\textwidth]{images/imp.png}\\ + +\end{center} +\ARROW Currently cloning structures of the SciFi.\\ +\ARROW Plans to implement Cesars proposal.\\ +\ARROW Run full MC simulations. + +\end{frame} + + + + + +\iffalse +\begin{frame}\frametitle{Prompt charm decays} + +\ARROW Study the prompt production: $\PDstar \to \PD (\pi \PK) \pi_{\rm slow}$. +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $K$, $\pi$ in UT + FT +\item Slow $\pi$ hits UT + MS and $K$, $\pi$ in UT + FT +\end{itemize} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 20.7\% +\end{align*} + +\end{small} + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_Dstar}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_Dstar}.pdf} + +\end{columns} + + + + +\end{frame} + + + +\begin{frame}\frametitle{$\Lambda_b \to \Lambda_c^{\ast} \tau \nu$} + +\ARROW Study the LUV in: $\Lambda_b \to \Lambda_c^{\ast} \tau \nu$ +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Two slow $\pi$ hits UT + FT and p, $K$, $\pi$ in UT + FT +\item One slow $\pi$ hits UT + MS(FT) and p, $K$, $\pi$ in UT + FT +\item Two slow $\pi$ hits UT + MS and p, $K$, $\pi$ in UT + FT +\end{itemize} +\end{small} + +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 60.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_Lcstar}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_Lcstar}.pdf} + +\end{columns} + + + +\end{frame} + + + +\begin{frame}\frametitle{$\PB \to \PDstar \tau \nu$} + +\ARROW Study the LUV in: $\PB \to \PDstar \tau \nu$ +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $K$, $\pi$ in UT + FT +\item Slow $\pi$ hits UT + MS and $K$, $\pi$ in UT + FT +\end{itemize} +\end{small} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 26.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_DstarB}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_DstarB}.pdf} + +\end{columns} + + + +\end{frame} + + + +\begin{frame}\frametitle{$\PB \to n \PK$} + +\ARROW Study the multi body decays: $\PB \to n \PK$: +\begin{center} +\includegraphics[angle=-90,width=0.75\textwidth]{images/nk.pdf} +\end{center} +\ARROW Clearly a threshold effect, the less PHSP you have the more you gain. + + +\end{frame} + + + +\iffalse +\begin{frame}\frametitle{$\PD \to 5 \PK$} + +\begin{columns} +\column{0.6\textwidth} +\ARROW Similar is expected to $\PD \PD$ searches. +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $K$, $\pi$ in UT + FT +\item Slow $\pi$ hits UT + MS and $K$, $\pi$ in UT + FT +\end{itemize} +\end{small} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 26.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_DstarB}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_DstarB}.pdf} + +\end{columns} + + + +\end{frame} +\fi + +\begin{frame}\frametitle{$\Sigma_b \to \Lambda_b \pi$} + +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $\Lambda_c$, $D_s$ in UT + FT +\item Slow $\pi$ hits UT + MS and $\Lambda_c$, $D_s$ in UT + FT +\end{itemize} +\end{small} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 29.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_DstarB}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_DstarB}.pdf} + +\end{columns} + + + +\end{frame} + + + + + + +\begin{frame}\frametitle{Gluon PDF} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/gluon.png} +\end{center} +\ARROW The Gluon PDF saturates the low momentum transfer and fractional momentum. + +\end{frame} + +\begin{frame}\frametitle{Gluon PDF} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/gluon22.png} +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{Gluon PDF efficiency} + +\ARROW If one looks at the efficiency for the low tracks, one finds where is the improvement: + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/pdf.png} +\end{center} + +\ARROW For more details see \href{https://indico.cern.ch/event/557554/contributions/2247267/attachments/1423140/2181806/gluon_saturation_seminar.pdf}{{\color{blue}Cesar Luiz da Silva; Tuesday Presentation}} + + +\end{frame} + + +\begin{frame}\frametitle{Spectroscopy} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/spec.png} +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{Idea from this workshop: $\PB \to \tau \tau$} + +\ARROW LHCb has recently measured: $\PB_{s/d} \to \tau \tau$~\href{https://arxiv.org/abs/1703.02508}{\color{blue}arXiv::1703.02508}\\ + +\begin{columns} + +\column{0.6\textwidth} +\includegraphics[width=0.95\textwidth]{images/bstautau.pdf} + + +\column{0.4\textwidth} + +\includegraphics[width=0.95\textwidth]{images/Bstautau2.png} + +\end{columns} + +\ARROW As a multibody decay it will probably have non-negligable gain from MS.\\ +\ARROW From preliminary studies $\mathcal{O}(24)\%$ gain. + + +\end{frame} + + +\begin{frame}\frametitle{Soft bomb events} + +\ARROW All credits to Zoltan Ligeti.\\ +\ARROW Based on paper:\href{https://arxiv.org/pdf/1612.00850.pdf?fname=cm&font=TypeI}{\color{blue}arXiv::1612.00850} + +\includegraphics[width=0.99\textwidth]{images/bomb.png} + +\ARROW The paper gives a lot of information how to select such events $\color{blue}\rightarrow$ Need new MC study. + +\end{frame} + + +\fi + + + +\begin{frame}\frametitle{Outlook} + +\ARROW The physics program of magnet stations is growing.\\ +\ARROW For many channels, the MS are improving the efficiencies from ~$20-30\% (R(D^{\ast}))$ to $60\%$.\\ +\ARROW For other, such as the study of Gluon saturation, the MS are enabling the measurement.\\ +\ARROW MS help when little PHSP is available.\\ +\ARROW Spectroscopy measurements enhanced.\\ +\ARROW Tagging of charm meson and baryon decays $\rightarrow$ reduce background.\\{~}\\ +\ARROW Tracking algorithms are being developed.\\ +\ARROW Implementing the MS in Gauss. + + + +\end{frame} + + + + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Magnet_Stations/21_03_2018_annecy/mchrzasz.toc b/Magnet_Stations/21_03_2018_annecy/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Magnet_Stations/21_03_2018_annecy/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Magnet_Stations/21_03_2018_annecy/tikzfeynman.sty b/Magnet_Stations/21_03_2018_annecy/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Magnet_Stations/21_03_2018_annecy/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Magnet_Stations/31_05_2017_Elba/Makefile b/Magnet_Stations/31_05_2017_Elba/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Magnet_Stations/31_05_2017_Elba/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Magnet_Stations/31_05_2017_Elba/beamercolorthemeFlip.sty b/Magnet_Stations/31_05_2017_Elba/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Magnet_Stations/31_05_2017_Elba/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Magnet_Stations/31_05_2017_Elba/beamerinnerthemeFlip.sty b/Magnet_Stations/31_05_2017_Elba/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Magnet_Stations/31_05_2017_Elba/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Magnet_Stations/31_05_2017_Elba/beamerouterthemeFlip.sty b/Magnet_Stations/31_05_2017_Elba/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Magnet_Stations/31_05_2017_Elba/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Magnet_Stations/31_05_2017_Elba/beamerouterthemedecolines.sty b/Magnet_Stations/31_05_2017_Elba/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Magnet_Stations/31_05_2017_Elba/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Magnet_Stations/31_05_2017_Elba/beamerthemeFlip.sty b/Magnet_Stations/31_05_2017_Elba/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Magnet_Stations/31_05_2017_Elba/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Magnet_Stations/31_05_2017_Elba/images/.DS_Store b/Magnet_Stations/31_05_2017_Elba/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/Magnet_Stations/31_05_2017_Elba/images/.DS_Store Binary files differ diff --git a/Magnet_Stations/31_05_2017_Elba/images/BG_both.png b/Magnet_Stations/31_05_2017_Elba/images/BG_both.png new file mode 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Bettler$^1$, P. Billoir$^2$, M. Chrzaszcz$^3$,\\ C. Da Silva$^4$, M. Martinelli$^5$\\~\\ +$^1$ CERN, $^2$ CNRS, $^3$ UZH, $^4$ LANL,$^5$ EPFL} + +\end{column} +%\begin{column}{0.53\textwidth} +%\includegraphics[height=1.3cm]{uzh-transp} +%\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{TTFU meeting, Elba, May 30, 2017} +\end{center} +\end{frame} +} + +\begin{frame}\frametitle{Outline} + +\ARROW Introduction\\ +\ARROW We will review the effect of an improved tracking for specific channels: +\begin{itemize} +\item Prompt Charm decays +%\item $\PD \to 5 \pi$ +\item $R(\Lambda_c^{\ast})$ +\item $R(\PDstar)$ +\item Multibody $\PB$ decays +\item $\Sigma_b$. +\item $\PB^{\ast}$. +\item Gluon PDF. +\item Spectroscopy. +\item More stuff added during this workshop. +\end{itemize} +\ARROW Outlook + + +\end{frame} + + +\begin{frame}\frametitle{The idea} +\begin{center} +\includegraphics[width=0.65\textwidth]{images/mag.png} +\end{center} +\ARROW Tracks with hits in the vertex locator and the TT/UT and not in the Tstations: UPSTREAM tracks.\\ +\ARROW Those are bend outside of the T-stations acceptance by the magnetic field because of their low-momentum.\\ +\ARROW The reduced amount of field between the VELO and the TT, means that their momentum is computed with a large uncertainty. +$\Delta p/p = 20-25\%$ current, $\Delta p/p = 15-20\%$ upgrade +\end{frame} + +\begin{frame}\frametitle{Proposal} +\only<1>{ +\ARROW Original idea comes from Sheldon Stone, Paolo Gandini, Liming Zhang: \href{https://indico.cern.ch/event/327376/contributions/1713479/}{{\color{blue}[Tuesday meeting Sept 2nd 2014]}}\\ +\begin{center} +\includegraphics[width=0.65\textwidth]{images/stations.png} +\end{center} +\ARROW It is outside the LHCb acceptancen!! No $X_0$ added.\\ +\ARROW No need to have a high resolution. $\mathcal{O}(1\rm mm)$ should be enough.\\ +\ARROW See Maurizio slides for details. +} +\only<2>{ + +\begin{center} +\includegraphics[width=0.75\textwidth]{images/sheldon.png} +\end{center} + +} + +\end{frame} + +\iffalse + +\begin{frame}\frametitle{Where our tracks are?} +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\ARROW The upstream tracks have rather poor momentum resolution: $\frac{\Delta p}{p} \sim 15\%$. \\ +\ARROW The particles die after short and sad (for physics) life in the magnet yoke. \\ +\ARROW If one put chambers in the magnet stations, one could record the particles before they death.\\ +\ARROW This will not increase the material budget of the rest of the detector.\\ +\begin{center} +\includegraphics[width=0.7\textwidth]{images/joke.png} +\end{center} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/sketch.png}\\ +\includegraphics[width=0.95\textwidth]{images/magnet.png} + + + +\end{columns} +\end{frame} + + +\begin{frame}\frametitle{Physics interest} +\begin{small} +\begin{columns} +\column{0.1in} +{~}\\ +\column{3in} +\ARROW We have enormous amount of channels where we have slow particles: +\begin{itemize} +\item $\PDstar \to \PD \pi$. +\item $\Lambda_c(2595, 2625) \to \Lambda_c \pi \pi$. +\item All the $\PB^{\ast \ast}$ decays! $\leftarrowtail$ huge community interests!!! +\item As well other states: $\Sigma_b \to \Lambda_b \pi$. +\item Little is known about the excited $\PBs$ states as well. + +\end{itemize} + + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/charmS.png}\\ + + + +\end{columns} +\end{small} +\end{frame} + + +\fi + +\begin{frame}\frametitle{The study} + +\begin{columns} +\column{0.4\textwidth} +\ARROW Take the Gauss \texttt{v50r0} for upgrade.\\ +\ARROW Simulate the particle gun.\\ +\ARROW Decays particles with \texttt{EvtGen}.\\ +\ARROW Put for now a plates in the Magnet (and beyond) and see where the particles hit them.\\ +\ARROW $\nu=7.6$. + +\column{0.6\textwidth} +\includegraphics[width=0.95\textwidth]{images/mag3.png} +\end{columns} + + +\end{frame} + + + + +\begin{frame}\frametitle{Prompt charm decays} + +\ARROW Study the prompt production: $\PDstar \to \PD (\pi \PK) \pi_{\rm slow}$. +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $K$, $\pi$ in UT + FT +\item Slow $\pi$ hits UT + MS and $K$, $\pi$ in UT + FT +\end{itemize} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 20.7\% +\end{align*} + +\end{small} + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_Dstar}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_Dstar}.pdf} + +\end{columns} + + + + +\end{frame} + + + +\begin{frame}\frametitle{$\Lambda_b \to \Lambda_c^{\ast} \tau \nu$} + +\ARROW Study the LUV in: $\Lambda_b \to \Lambda_c^{\ast} \tau \nu$ +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Two slow $\pi$ hits UT + FT and p, $K$, $\pi$ in UT + FT +\item One slow $\pi$ hits UT + MS(FT) and p, $K$, $\pi$ in UT + FT +\item Two slow $\pi$ hits UT + MS and p, $K$, $\pi$ in UT + FT +\end{itemize} +\end{small} + +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 60.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_Lcstar}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_Lcstar}.pdf} + +\end{columns} + + + +\end{frame} + + + +\begin{frame}\frametitle{$\PB \to \PDstar \tau \nu$} + +\ARROW Study the LUV in: $\PB \to \PDstar \tau \nu$ +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $K$, $\pi$ in UT + FT +\item Slow $\pi$ hits UT + MS and $K$, $\pi$ in UT + FT +\end{itemize} +\end{small} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 26.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_DstarB}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_DstarB}.pdf} + +\end{columns} + + + +\end{frame} + + + +\begin{frame}\frametitle{$\PB \to n \PK$} + +\ARROW Study the multi body decays: $\PB \to n \PK$: +\begin{center} +\includegraphics[angle=-90,width=0.75\textwidth]{images/nk.pdf} +\end{center} +\ARROW Clearly a threshold effect, the less PHSP you have the more you gain. + + +\end{frame} + + + +\iffalse +\begin{frame}\frametitle{$\PD \to 5 \PK$} + +\begin{columns} +\column{0.6\textwidth} +\ARROW Similar is expected to $\PD \PD$ searches. +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $K$, $\pi$ in UT + FT +\item Slow $\pi$ hits UT + MS and $K$, $\pi$ in UT + FT +\end{itemize} +\end{small} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 26.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_DstarB}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_DstarB}.pdf} + +\end{columns} + + + +\end{frame} +\fi + +\begin{frame}\frametitle{$\Sigma_b \to \Lambda_b \pi$} + +\begin{columns} +\column{0.6\textwidth} +\ARROW The study is based on two type of cases: +\begin{small} +\begin{itemize} +\item Slow $\pi$ hits UT + FT and $\Lambda_c$, $D_s$ in UT + FT +\item Slow $\pi$ hits UT + MS and $\Lambda_c$, $D_s$ in UT + FT +\end{itemize} +\end{small} +\ARROW The gain in terms of statistics:\\ +\begin{align*} +{ \rm gain} = 29.0\% +\end{align*} + + +\column{0.4\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/z_DstarB}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/yz_DstarB}.pdf} + +\end{columns} + + + +\end{frame} + + + + + + +\begin{frame}\frametitle{Gluon PDF} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/gluon.png} +\end{center} +\ARROW The Gluon PDF saturates the low momentum transfer and fractional momentum. + +\end{frame} + +\begin{frame}\frametitle{Gluon PDF} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/gluon22.png} +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{Gluon PDF efficiency} + +\ARROW If one looks at the efficiency for the low tracks, one finds where is the improvement: + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/pdf.png} +\end{center} + +\ARROW For more details see \href{https://indico.cern.ch/event/557554/contributions/2247267/attachments/1423140/2181806/gluon_saturation_seminar.pdf}{{\color{blue}Cesar Luiz da Silva; Tuesday Presentation}} + + +\end{frame} + + +\begin{frame}\frametitle{Spectroscopy} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/spec.png} +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{Idea from this workshop: $\PB \to \tau \tau$} + +\ARROW LHCb has recently measured: $\PB_{s/d} \to \tau \tau$~\href{https://arxiv.org/abs/1703.02508}{\color{blue}arXiv::1703.02508}\\ + +\begin{columns} + +\column{0.6\textwidth} +\includegraphics[width=0.95\textwidth]{images/bstautau.pdf} + + +\column{0.4\textwidth} + +\includegraphics[width=0.95\textwidth]{images/Bstautau2.png} + +\end{columns} + +\ARROW As a multibody decay it will probably have non-negligable gain from MS.\\ +\ARROW From preliminary studies $\mathcal{O}(24)\%$ gain. + + +\end{frame} + + +\begin{frame}\frametitle{Soft bomb events} + +\ARROW All credits to Zoltan Ligeti.\\ +\ARROW Based on paper:\href{https://arxiv.org/pdf/1612.00850.pdf?fname=cm&font=TypeI}{\color{blue}arXiv::1612.00850} + +\includegraphics[width=0.99\textwidth]{images/bomb.png} + +\ARROW The paper gives a lot of information how to select such events $\color{blue}\rightarrow$ Need new MC study. + +\end{frame} + + + + + + +\begin{frame}\frametitle{Outlook} + +\ARROW The physics program of magnet stations is enormous.\\ +\ARROW For many channels, the MS are improving the efficiencies from ~$20-30\% (R(D^{\ast}))$ to $60\%$.\\ +\ARROW For other, such as the study of Gluon saturation, the MS are enabling the measurement.\\ +\ARROW MS help when little PHSP is available.\\ +\ARROW We are extending the studies for more and more decays in the future. + + + +\end{frame} + + + +\begin{frame}\frametitle{Since Guy started...} +\begin{columns} + +\column{0.5\textwidth} +''The extent of your consciousness is limited only by your ability to love''\\ +\includegraphics[width=0.9\textwidth]{images/nap.png} + + + +\column{0.5\textwidth} +\pause +''The extent of your ACCEPTANCE is limited only by your MAGNET STATIONS''\\ +\includegraphics[width=0.9\textwidth]{images/nap2.png} + + + +\end{columns} + +\end{frame} + + + + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Magnet_Stations/31_05_2017_Elba/mchrzasz.toc b/Magnet_Stations/31_05_2017_Elba/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Magnet_Stations/31_05_2017_Elba/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Magnet_Stations/31_05_2017_Elba/tikzfeynman.sty b/Magnet_Stations/31_05_2017_Elba/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Magnet_Stations/31_05_2017_Elba/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/ReInterpretation/2019/Makefile b/ReInterpretation/2019/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/ReInterpretation/2019/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/ReInterpretation/2019/beamercolorthemeFlip.sty b/ReInterpretation/2019/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/ReInterpretation/2019/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/ReInterpretation/2019/beamerinnerthemeFlip.sty b/ReInterpretation/2019/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/ReInterpretation/2019/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/ReInterpretation/2019/beamerouterthemeFlip.sty b/ReInterpretation/2019/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/ReInterpretation/2019/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/ReInterpretation/2019/beamerouterthemedecolines.sty b/ReInterpretation/2019/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/ReInterpretation/2019/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/ReInterpretation/2019/beamerthemeFlip.sty b/ReInterpretation/2019/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/ReInterpretation/2019/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/ReInterpretation/2019/images/.DS_Store b/ReInterpretation/2019/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/ReInterpretation/2019/images/.DS_Store Binary files differ diff --git a/ReInterpretation/2019/images/180.png b/ReInterpretation/2019/images/180.png new file mode 100644 index 0000000..a67d39f --- /dev/null +++ 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--git a/ReInterpretation/2019/mchrzasz-blx.bib b/ReInterpretation/2019/mchrzasz-blx.bib new file mode 100644 index 0000000..fa04f16 --- /dev/null +++ b/ReInterpretation/2019/mchrzasz-blx.bib @@ -0,0 +1,11 @@ +@Comment{$ biblatex control file $} +@Comment{$ biblatex version 2.6 $} +Do not modify this file! + +This is an auxiliary file used by the 'biblatex' package. +This file may safely be deleted. It will be recreated as +required. + +@Control{biblatex-control, + options = {2.6:0:0:1:0:0:1:1:0:0:0:0:1:1:3:1:79:+}, +} diff --git a/ReInterpretation/2019/mchrzasz.aux b/ReInterpretation/2019/mchrzasz.aux new file mode 100644 index 0000000..b590523 --- /dev/null +++ b/ReInterpretation/2019/mchrzasz.aux @@ -0,0 +1,181 @@ +\relax +\providecommand\hyper@newdestlabel[2]{} +\providecommand\zref@newlabel[2]{} +\providecommand\HyperFirstAtBeginDocument{\AtBeginDocument} +\HyperFirstAtBeginDocument{\ifx\hyper@anchor\@undefined +\global\let\oldcontentsline\contentsline +\gdef\contentsline#1#2#3#4{\oldcontentsline{#1}{#2}{#3}} +\global\let\oldnewlabel\newlabel +\gdef\newlabel#1#2{\newlabelxx{#1}#2} +\gdef\newlabelxx#1#2#3#4#5#6{\oldnewlabel{#1}{{#2}{#3}}} +\AtEndDocument{\ifx\hyper@anchor\@undefined +\let\contentsline\oldcontentsline +\let\newlabel\oldnewlabel +\fi} +\fi} +\global\let\hyper@last\relax +\gdef\HyperFirstAtBeginDocument#1{#1} +\providecommand*\HyPL@Entry[1]{} +\bibstyle{biblatex} 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+\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\TeV}{\mathrm{TeV}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mil +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} +\def\fixme{FIXME} + + + +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + +\author{Jihyun Bhom (IFJ PAN), Marcin Chrzaszcz (CERN)} +\institute{UZH} +\title[HEPLike]{HEPLike} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.15\textwidth} +{~} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.73\textwidth} + \flushright \bfseries \Large {HEPLike - tool for experimental likelihood evaluation} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-2.8em} {Jihyun Bhom\\ \small \href{mailto:jihyun.bohm@cern.ch}{jihyun.bohm@cern.ch} \vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}\\ Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +%\flushright \vspace{-2.8em} { Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + + +\end{column} +\begin{column}{0.53\textwidth} +\hspace{2.0cm} +\includegraphics[height=1.6cm]{cern}{~} +\includegraphics[height=1.6cm]{ifj.png} +\end{column} +\end{columns} + +\vspace{1em} + \vspace{1.4cm} + + + \textcolor{normal text.fg!50!Comment}{(Re)interpreting the results of new physics searches at the LHC, London, April 2-4, 2019} +\end{center} +\end{frame} +} + + +\begin{frame}\frametitle{HEP results} +\ARROW How do we publish results? +\begin{columns} +\column{0.35\textwidth} +\includegraphics[width=0.95\textwidth]{images/arxiv.png}\\ +\pause +\begin{align*} +R_K=0.846^{+0.060 +0.016}_{-0.054 - 0.014} +\end{align*} + +\pause +\column{0.65\textwidth} +\begin{center} +\includegraphics[angle=-90,width=0.5\textwidth]{images/FigS8.pdf}\\ +\pause +\includegraphics[width=0.75\textwidth]{images/hepdata.png} +\end{center} + + +\end{columns} + + +\end{frame} + + + + + +\begin{frame}\frametitle{HEP results} +\ARROW How are the results used? +\begin{columns} +\column{0.5\textwidth} + +\ARROWR Correlations are neglected +\includegraphics[width=0.75\textwidth]{{images/Table_12}.pdf} + + +\ARROWR Non Linear effects are forgotten +\includegraphics[angle=-90,width=0.75\textwidth]{{images/example}.pdf} + + + +\column{0.5\textwidth} + +\ARROWR Errors are being symmetrized +\includegraphics[angle=-90,width=0.75\textwidth]{{images/Fig62aS}.pdf} + +{~}\\{~}\\ +\end{columns} + + +\end{frame} + + +\begin{frame}\frametitle{HEP results} +\ARROW How are the results used?\\{~}\\ + +\ARROWR Interpreting Upper limits [HLFAV, 90\% UL]: +\begin{align*} +\mathcal{B} (\tau \to \mu \mu e) < 9.9 \times 10^{-9} +\end{align*} +\ARROW People interpret this assuming it's a gaussian centered around $0$ and width $\frac{9.9\times 10^{-9}}{1.64} $.\\ +\ARROW Usually a full p-value scan is published: +\begin{columns} +\column{0.5\textwidth} +\includegraphics[width=0.75\textwidth]{{images/180}.png} + +\column{0.5\textwidth} +\includegraphics[width=0.75\textwidth]{{images/dupa}.png} + + +\end{columns} +\ARROW The examples go on and on... + + +\end{frame} + + + + + +\begin{frame}\frametitle{The idea} +\ARROW The theory and experimental community need to work together about proper interpretation. +\pause +\begin{center} +\includegraphics[width=0.95\textwidth]{{images/kim}.jpg} +\end{center} + + + + + +\end{frame} + + + +\begin{frame}\frametitle{HEPLike} + +\ARROW High Energy Physics Likelihood (HEPLike). +\begin{itemize} +\item Open source software. +\item With separate database of measurements. +\item Statistics library. +\item Can be interfaced with existing codes. +\end{itemize} +\ARROW It constructs the experimental likelihoods for you!\\ +\ARROW Does work with both the $\chi^2$ and (log-)likelihood fits.\\ +\ARROW Useful utilities for creating citations and database search. +\end{frame} + + +\begin{frame}\frametitle{HEPLike} + +\ARROW The are couple of measurement types: +\begin{itemize} +\item Upper limits, +\item Single measurement with symmetric uncertainty, +\item Single measurement with asymmetric uncertainty, +\item Multiple measurements with symmetric uncertainty, +\item Multiple measurements with asymmetric uncertainty, +\item One dimensional likelihood function, +\item n-dimensional likelihood function. +\end{itemize} + + +\begin{alertblock}{Bonus} +In addition we provide a way for the future that the experiments can publish the dataset. +\end{alertblock} + +\end{frame} + + +\begin{frame}\frametitle{HEPLike - code structure} + +\begin{center} +\includegraphics[width=0.99\textwidth]{images/diagram.png} + +\end{center} + + + +\end{frame} + + + + + + +\begin{frame}\frametitle{Measurement encoding, \texttt{Hl\_Data}} + +\ARROW Measurements are stored in \texttt{YAML} file: +\includegraphics[width=0.9\textwidth]{images/yaml.png} \\ +\includegraphics[width=0.9\textwidth]{images/yaml2.png} + + +\end{frame} + + + + +\begin{frame}\frametitle{Upper limits, \texttt{HL\_Limit}} + +\ARROW Example of published p-value scans:\\ +\begin{columns} + +\column{0.4\textwidth} + +\includegraphics[angle=-90,width=0.95\textwidth]{images/Bs2tautau.pdf} + +\column{0.6\textwidth} +\ARROW Information coded as: +\includegraphics[width=0.95\textwidth]{images/yaml3.png} + +\end{columns} + + + +\end{frame} + + + +\begin{frame}\frametitle{Upper limits, \texttt{HL\_Limit}} + +\begin{equation} +pdf(x) = \frac{1}{2^{1/2} \Gamma(1/2)} x^{1/2 -1} e ^{-x/2}, +\end{equation} +which had the cumulative distribution function defined as: +\begin{equation} +cdf(x)=\frac{1}{\Gamma(1/2) } \gamma(1/2,x/2). +\end{equation} +In the above equations the $\Gamma(x)$ and $\gamma(k,x)$ correspond to Gamma and incomplete gamma functions. +By revering the $cdf(x)$ one can obtain the $\chi^2$ value: +\begin{equation} +\chi^2=cdf^{-1}(1-p), +\end{equation} +and if needed the log-likelihood: +\begin{equation} +-\log(\mathcal{L})= \frac{1}{2}\chi^2, \label{eq:wilks} +\end{equation} +\end{frame} + + + + +\begin{frame}\frametitle{Single measurement, symmetric error, \texttt{HL\_Gaussian}} + +\ARROW Well this is as simple as: +\begin{center} +\includegraphics[width=0.6\textwidth]{images/yaml4.png} +\end{center} +\ARROW The $\chi^2$ is simple: +\begin{equation} +\chi^2 = \frac{(x_{obs}-x)^{2}}{ \sigma_{stat}^{2}+ \sigma_{syst}^{2} }, +\end{equation} + +\ARROW Wilks theorem can be used to translate to (log-)likelihood. + + +\end{frame} + + + +\begin{frame}\frametitle{Single measurement, symmetric error, \texttt{HL\_Gaussian}} + +\ARROW Well this is as simple as: +\begin{center} +\includegraphics[width=0.6\textwidth]{images/yaml4.png} +\end{center} +\ARROW The $\chi^2$ is simple: +\begin{equation} +\chi^2 = \frac{(x_{obs}-x)^{2}}{ \sigma_{stat}^{2}+ \sigma_{syst}^{2} }, +\end{equation} + +\ARROW Wilks theorem can be used to translate to (log-)likelihood. + + +\end{frame} + + + + +\begin{frame}\frametitle{Multiple measurement, symmetric error, \texttt{HL\_nDimGaussian}} + +\ARROW You need to pass two arguments: +\begin{center} +\includegraphics[width=0.6\textwidth]{images/yaml5.png} +\end{center} +\ARROW From this one constructs the covariance matrix, and evaluates the $\chi^2$: +\begin{align} +\chi^2 = V^{T} {\rm Cov}^{-1} V,\label{eq:chi2ndim} +\end{align} + + +\end{frame} + + +\begin{frame}\frametitle{Measurement, asymmetric error, \texttt{HL\_BifurGaussian}, \texttt{HL\_ndimBifurGaussian}} + +\ARROW You need to pass two arguments: +\begin{center} +\includegraphics[width=0.6\textwidth]{images/yaml6.png} +\end{center} + +\ARROW We choose to interpret this as Bifurcated Gaussian: + + \begin{align} +{\rm Cov}_{i,j}= +\begin{cases} +{\rm Corr}_{i,j}~\sigma^{i}_+ \sigma^{j}_+, & \text{if } x^i \geq x^i_{obs} \text{ and } x^j \geq x^j_{obs} \\ +{\rm Corr}_{i,j}~\sigma^{i}_+ \sigma^{j}_-, & \text{if } x^i \geq x^i_{obs} \text{ and } x^j < x^j_{obs} \\ +{\rm Corr}_{i,j}~\sigma^{i}_- \sigma^{j}_+, & \text{if } x^i < x^i_{obs} \text{ and } x^j \geq x^j_{obs} \\ +{\rm Corr}_{i,j}~\sigma^{i}_- \sigma^{j}_-, & \text{if } x^i < x^i_{obs} \text{ and } x^j < x^j_{obs} \\ +\end{cases} +\end{align} + + +\end{frame} + + + + +\begin{frame}\frametitle{Likelihoods, \texttt{HL\_ProfLikelihood}, \texttt{HL\_nDimLikelihood}} + +\ARROW Here we add just the location of \texttt{ROOT} object.\\ +\begin{columns} +\column{0.7\textwidth} + \begin{center} +\includegraphics[width=0.9\textwidth]{images/yaml7.png}\\ +\includegraphics[width=0.9\textwidth]{images/yaml8.png} +\end{center} + +\ARROW This is the best way to publish results!!!\\ +\ARROW The problem is in what way one should publish the higher dim likelihoods? + + +\column{0.3\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig2-S.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig21.pdf} +\end{columns} + + + + + +\end{frame} + + + +\begin{frame}\frametitle{Publishing data} + + \includegraphics[width=0.95\textwidth]{images/patrick.png} + + + + Stolen from P. Owen +\end{frame} + + + +\begin{frame}\frametitle{Publishing data \texttt{HL\_ExpData}} + +\ARROW The \texttt{YAML} entry: + + \includegraphics[width=0.5\textwidth]{images/yaml9.png}\\ + \ARROW Set the PDF you want to fit:\\ \texttt{double (*fun)(vector par , vector point)}\\ + \ARROW The program will evaluate the (log-)likelihood on the whole dataset for given parameters.\\ + \ARROW You only need a scanning tools and you are done. + + +\end{frame} + + +\begin{frame}\frametitle{Useful functions} + + + +\ARROW Search for measurement you need: +\begin{center} +\includegraphics[width=0.9\textwidth]{images/example.png} +\end{center} + + + +\ARROW Create citation file: +\begin{center} +\includegraphics[width=0.9\textwidth]{images/example2.png} +\end{center} + + +\end{frame} + + + + + + + + +\begin{frame}\frametitle{Check it out} + +\ARROW The HEPLike code:\\ +\url{https://github.com/mchrzasz/HEPLike} + +\ARROW The HEPLike database:\\ +\url{https://github.com/mchrzasz/HEPLikeData} + +\begin{alertblock}{} +Don't be shy! Give it a spin. Feedback is welcomed. +\end{alertblock} + \pause + + + \begin{exampleblock}{} + \begin{center} + Thank you for your attention + + \end{center} + + \end{exampleblock} + + +\end{frame} + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/ReInterpretation/2019/mchrzasz.toc b/ReInterpretation/2019/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/ReInterpretation/2019/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/ReInterpretation/2019/tikzfeynman.sty b/ReInterpretation/2019/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/ReInterpretation/2019/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Review_LHCb/A2mumu/Makefile b/Review_LHCb/A2mumu/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Review_LHCb/A2mumu/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Review_LHCb/A2mumu/beamercolorthemeFlip.sty b/Review_LHCb/A2mumu/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Review_LHCb/A2mumu/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Review_LHCb/A2mumu/beamerinnerthemeFlip.sty b/Review_LHCb/A2mumu/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Review_LHCb/A2mumu/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Review_LHCb/A2mumu/beamerouterthemeFlip.sty b/Review_LHCb/A2mumu/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Review_LHCb/A2mumu/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Review_LHCb/A2mumu/beamerouterthemedecolines.sty b/Review_LHCb/A2mumu/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Review_LHCb/A2mumu/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Review_LHCb/A2mumu/beamerthemeFlip.sty b/Review_LHCb/A2mumu/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Review_LHCb/A2mumu/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Review_LHCb/A2mumu/images/.DS_Store b/Review_LHCb/A2mumu/images/.DS_Store new file mode 100644 index 0000000..5008ddf --- /dev/null +++ b/Review_LHCb/A2mumu/images/.DS_Store Binary files differ diff --git a/Review_LHCb/A2mumu/images/BG_both.png b/Review_LHCb/A2mumu/images/BG_both.png new file mode 100755 index 0000000..49b62d5 --- /dev/null +++ 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"SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + 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+\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} + + + +\author{ {Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich, IFJ PAN)} +\institute{UZH} +\title[Review Committee report]{Review Committee report} +\date{13 November 2015} + + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright\bfseries \Huge {RC report} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} { \Large Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=1.3cm]{cern} + +\end{column} +\end{columns} + +\vspace{1em} + + \textcolor{normal text.fg!50!Comment}{For the RC: MCh, Hang Yin (CCNU), Mike Williams (MIT) } + +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{Analysis approval, CERN\\February 20, 2018} +\end{center} +\end{frame} +} + +\begin{frame}{Analysis details} + \begin{minipage}{\textwidth} +\begin{itemize} +\item \textbf{Analysis:} Model-independent search for a light BSM di-muon resonance in the bottomonium region. +\item \textbf{Contact authors}: Carlos Vazquez Sierra, Martino Borsato, Xabier Cid Vidal +\item \textbf{WG Aproval}: 28-Jun-2016 +\item \textbf{Data set}: $3~\rm fb^{-1}$ Run1 +\item \textbf{Twiki}: \href{https://twiki.cern.ch/twiki/bin/viewauth/LHCbPhysics/A02MuMu +}{https://twiki.cern.ch/twiki/bin/viewauth/LHCbPhysics/A02MuMu} +\end{itemize} +A bit statistics: +\begin{itemize} +\item 5 versions of ANA note. +\item 3 meetings with the RC. +\end{itemize} + + \end{minipage} + +\end{frame} + +\begin{frame}{Motivation} + \begin{minipage}{\textwidth} +\begin{center} +\includegraphics[width=0.49\textwidth]{images/motivation.png} + + + +\end{center} + + +\begin{itemize} +\item LHCb has a unique opportunity to find it in the hardest area. +\end{itemize} + + + \end{minipage} + +\end{frame} + + +\begin{frame}{No spoilers!!} + + \begin{minipage}{\textwidth} +\begin{center} + +\begin{columns} +\column{0.4\textwidth} +\begin{itemize} +\item The difficulty of analysis is controlling the mass shape close to the resonance region. +\item Now I will not show you what they do as you would not listen to the authors ;) +\end{itemize} + + +\column{0.6\textwidth} +\includegraphics[width=0.98\textwidth]{images/motivation2.png} + + + +\end{columns} + + +\end{center} + + \end{minipage} + + + +\end{frame} + + + + + +\begin{frame}{Conclusions} + \begin{minipage}{\textwidth} + + + +\begin{large} +\begin{itemize} +\item We recommend that analysis is approved to go to paper. +\item Thanks to the proponents for an interesting and productive review +\end{itemize} +\end{large} + + + + \end{minipage} + + +\end{frame} + + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Review_LHCb/A2mumu/mchrzasz.tex~ b/Review_LHCb/A2mumu/mchrzasz.tex~ new file mode 100644 index 0000000..85cc86a --- /dev/null +++ b/Review_LHCb/A2mumu/mchrzasz.tex~ @@ -0,0 +1,307 @@ +\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} + +\usepackage[english]{babel} +\usepackage{polski} + + +\usetheme[ + bullet=circle, % Other option: square + bigpagenumber, % circled page number on lower right + topline=true, % colored bar at the top of the frame + shadow=false, % Shading for beamer blocks + watermark=BG_lower, % png file for the watermark + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +\usepackage{emerald} +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% 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more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} + + + +\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich, IFJ PAN)} +\institute{UZH} +\title[$\PBzero \to \PKstar \Pmuon \APmuon$ update]{$\PBzero \to \PKstar \Pmuon \APmuon$ update} +\date{25 September 2014} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright\fontspec{Trebuchet MS}\bfseries \Huge {$\PBzero \to \PKstar \Pmuon \APmuon$ update} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} {\fontspec{Trebuchet MS} \Large Marcin Chrząszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=1.3cm]{uzh-transp}{~}{~} +\includegraphics[height=1.1cm]{ifj.png} +\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{Zurich meeting, CERN\\September 24, 2014} +\end{center} +\end{frame} +} + + +\begin{frame}[c]{A short introduction to the $\nu$MSM}%{{\footnotesize\href{http://arxiv.org/abs/hep-ph/0503065}{[T. Asaka et al. 2005]}}} +\topline + \begin{minipage}{\textwidth} +\topline + \begin{exampleblock}{} + Leptons and quarks get their mass through the Yukawa interaction: + \vspace*{-0.7em}\begin{align*} + \mathcal{L} = m\,\psi^\dagger_L\, h\, \psi_R + c.c. + \end{align*} + \end{exampleblock} + \begin{figure} + % \centering + \flushleft + %\includegraphics<1-1>[width=0.48\textwidth]{img/neutrinos-sm} + %%\hfill + %\phantom{\includegraphics<1-1>[width=0.48\textwidth]{img/neutrinos-nusm}} + %\includegraphics<2-2>[width=0.48\textwidth]{img/neutrinos-nusm} + \end{figure} + \only<1-2>{\Put(170,180){\begin{minipage}{0.45\textwidth}\vskip0pt plus 1filll + \Alert{\vskip0pt plus 1filll Neutrinos need a right-handed partner to get their masses like the other SM fermions!} + \newline{}%\vskip0pt plus 1filll + %\only<1-1>{\vskip0pt plus 1filll\phantom{An extra \ALERT{$N$} field could exist. It would be a $SU(2)$ singlet, as it is still unobserved.}} + %\only<2-2>{An extra \ALERT{$N$} field could exist. It would be a $SU(2)$ singlet, as it is still unobserved.} + \onslide<2-2>{Three extra \ALERT{$N$} field could exist (\Alert{\textit{sterile neutrinos}}). They would be $SU(2)$ singlets, as they are still unobserved.} + \end{minipage}}} +% \vskip0pt plus 1filll +% \only<1-1>{\phantom{ +% \begin{align*} +% &\mathcal{L} = \bar{N_i}i\slashed\partial N_i - f_{i\alpha}H\bar{N_i}L_\alpha - \frac{M_i}{2}\bar{N_i}^c N_i + h.c. +% \end{align*}}} +% Sterile neutrinos would \Alert{mix to $\nu_{e,\mu,\tau}$} with very small couplings \Alert{$U^2_{e,\mu,\tau}$}.}} + \only<2-2>{ +\vspace{-0.5cm} + \begin{align*} + &\mathcal{L} = \mathcal{L}_{SM} \bar{N_i}i\slashed\partial N_i - f_{i\alpha}H\bar{N_i}L_{\alpha} - \frac{M_i}{2}\bar{N_i}^c N_i + h.c. + \end{align*} +\kern-0.9em +\ALERT{\textbf{Sterile neutrinos}} would \Alert{mix to $\nu_{e,\mu,\tau}$} with very small couplings \Alert{$U^2_{e,\mu,\tau}$}. + } + \end{minipage} + \vspace*{2.cm} +\end{frame} + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/Review_LHCb/A2mumu/mchrzasz.toc b/Review_LHCb/A2mumu/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Review_LHCb/A2mumu/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Review_LHCb/A2mumu/tikzfeynman.sty b/Review_LHCb/A2mumu/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Review_LHCb/A2mumu/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Seminars/Bialasowka_2018/Makefile b/Seminars/Bialasowka_2018/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Seminars/Bialasowka_2018/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Seminars/Bialasowka_2018/beamercolorthemeFlip.sty b/Seminars/Bialasowka_2018/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Seminars/Bialasowka_2018/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Seminars/Bialasowka_2018/beamerinnerthemeFlip.sty b/Seminars/Bialasowka_2018/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Seminars/Bialasowka_2018/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Seminars/Bialasowka_2018/beamerouterthemeFlip.sty b/Seminars/Bialasowka_2018/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Seminars/Bialasowka_2018/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Seminars/Bialasowka_2018/beamerouterthemedecolines.sty b/Seminars/Bialasowka_2018/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Seminars/Bialasowka_2018/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Seminars/Bialasowka_2018/beamerthemeFlip.sty b/Seminars/Bialasowka_2018/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Seminars/Bialasowka_2018/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Seminars/Bialasowka_2018/distracted_ilissa-ocko-cartoon.jpg b/Seminars/Bialasowka_2018/distracted_ilissa-ocko-cartoon.jpg new file mode 100644 index 0000000..5f007b0 --- /dev/null +++ b/Seminars/Bialasowka_2018/distracted_ilissa-ocko-cartoon.jpg Binary files differ diff --git a/Seminars/Bialasowka_2018/images/1.png b/Seminars/Bialasowka_2018/images/1.png new file 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+\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\MeV}{\rm{MeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\re}{{\rm Re}} +\newcommand{\invfb}{\rm{fb^{-1}}} +\newcommand{\fixme}{\rm{{\color{red}{FIXME!}}}} +\newcommand{\thetal}{\theta_l} +\newcommand{\thetak}{\theta_k} +\newcommand{\nn}{\nonumber} +\newcommand{\eq}[1]{\begin{equation} #1 \end{equation}} +%\newcommand{\eqn}[1]{\begin{displaymath} #1 \end{displaymath}} +\newcommand{\eqa}[1]{\begin{eqnarray} #1 \end{eqnarray}} +\newcommand{\apeL}{{A_\perp^L}} +\newcommand{\apeR}{{A_\perp^R}} +\newcommand{\ape}{{A_\perp}} +\newcommand{\apeLR}{{A_\perp^{L,R}}} +\newcommand{\apaL}{{A_\|^L}} +\newcommand{\apaR}{{A_\|^R}} +\newcommand{\apa}{{A_\|}} +\newcommand{\apaLR}{{A_\|^{L,R}}} +\newcommand{\azeL}{{A_0^L}} +\newcommand{\azeR}{{A_0^R}} +\newcommand{\aze}{{A_0}} + +\newcommand{\azeLR}{{A_0^{L,R}}} +\newcommand{\Real}{\ensuremath{\mathcal{R}e}\xspace} +\newcommand{\Imag}{\ensuremath{\mathcal{I}m}\xspace} + +\renewcommand{\C}[1]{{\cal C}_{#1}} +\newcommand{\Ceff}[1]{{\cal C}^{\rm eff}_{#1}} +\newcommand{\Cpeff}[1]{{\cal C}^{\rm eff\prime}_{#1}} +\newcommand{\Cp}[1]{{\cal C}^{\prime}_{#1}} +\def\FL {\ensuremath{F_{\mathrm{L}}}\xspace} +\def\ATDPH {\ensuremath{A_{\mathrm{T,PR}}^{(2)}}\xspace} +\def\ATImPH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Im}}}\xspace} +\def\ATRePH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Re}}}\xspace} +\def\FLPH {\ensuremath{F_{\mathrm{L,PR}}}\xspace} +\def\ATDKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{(2)}}\xspace} +\def\ATImKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Im}}}\xspace} +\def\ATReKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Re}}}\xspace} +\def\FLKG {\ensuremath{F_{\mathrm{L,\Kstarz \gamma}}}\xspace} +\def\ATD {\ensuremath{A_{\mathrm{T}}^{(2)}}\xspace} +\def\ATIm {\ensuremath{A_{\mathrm{T}}^{\mathrm{Im}}}\xspace} +\def\ATRe {\ensuremath{A_{\mathrm{T}}^{\mathrm{Re}}}\xspace} +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} + + + +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + + + +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\mathcal{B}}} + +\newcommand{\av}[1]{\langle #1 \rangle} +% particles +\def\LstFTTT {\ensuremath{\PLambda^{*}(1520)^{0}}\xspace} +\def\dll {\ensuremath{\mathrm{DLL}}\xspace} + \def\Lb {\ensuremath{\PLambda_b}} + + +% useful decays +\def\BdToKpimm {\decay{\Bd}{\Kp\pim\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsToJPsiKst {\decay{\Bs}{\jpsi\Kstarz}} +\def\BdTopsitwosKst {\decay{\Bd}{\psitwos\Kstarz}} +\def\LstFTTTT {\decay{\LstFTTT}{p\Km}} +%\def\LbToLstmm {\decay{\Lb}{\PLambda^{*}(1520)^{0} \mumu}} +\def\LbTopKmm {\decay{\Lb}{p\Km\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsTophimm {\decay{\Bs}{\Pphi\mumu}} + +% interesting variables +\def\mkpi {\ensuremath{m_{K\pi}}\xspace} +\def\mkpimm{\ensuremath{m_{K\pi\mu\mu}}\xspace} + +%% peaking background mass hypotheses +\def\mkmm {\ensuremath{m_{K\mu\mu}}\xspace} +\def\mSwappKmm {\ensuremath{m_{(\pi\to p)K\mu\mu}}\xspace} +\def\mSwappiK {\ensuremath{m_{(\pi\to K)K}}\xspace} +\def\mSwappiKmm {\ensuremath{m_{(\pi\to K)K\mu\mu}}\xspace} +\def\mSwappK {\ensuremath{m_{(\pi\to p)K}}\xspace} +\def\mDoubleSwappKmm {\ensuremath{m_{(K\to p)(\pi\to K)\mu\mu}}\xspace} +\def\mDoubleSwappK {\ensuremath{m_{(K\to p)(\pi\to K)}}\xspace} +\def\mSwapKst {\ensuremath{m_{K\leftrightarrow\pi}}\xspace} + +%% some other decays +\def\BsToPhimm {\decay{\Bs}{\phi\mumu}} +\def\BsToPhimmFULL {\decay{\Bs}{\phi(\to\!K^{+}K^{-})\mumu}} +\def\BsToKKmm {\decay{\Bs}{\Kp\Km\mumu}} + +\newcommand{\delC}[1]{\delta {\cal C}_{#1}} +\newcommand{\dC}[1]{{\cal C}_{#1}^{\rm NP}} +\newcommand{\dCp}[1]{{\cal C}_{#1^\prime}^{\rm NP}} + + + + +\definecolor{green}{rgb}{0.2,0.6,0.2} +\definecolor{lightgreen}{rgb}{0.4,1,0.4} +\definecolor{verylightgreen}{rgb}{0.7,1,0.7} +\def\cgreen{\color{green}} +\definecolor{brown}{rgb}{0.4,0.2,0.0} +\def\cbrown{\color{brown}} +\def\cred{\color{red}} +\definecolor{darkblue}{rgb}{0.0,0.0,1.0} +\def\cdarkblue{\color{darkblue}} +\definecolor{darkgrey}{rgb}{0.4,0.4,0.4} +\definecolor{lightgrey}{rgb}{0.7,0.7,0.7} +\definecolor{verylightblue}{rgb}{0.8,0.8,1.0} +\definecolor{lightblue}{rgb}{0.6,0.6,1.0} +\definecolor{verylightyellow}{rgb}{1.0,1.0,0.5} +\definecolor{lightyellow}{rgb}{1.0,0.7,0.3} +\definecolor{darkred}{rgb}{0.6,0.0,0.0} + +\definecolor{green}{rgb}{0.3,0.6,0.2} +\definecolor{green}{rgb}{0.3,0.7,0.4} + + + +\definecolor{indigo}{RGB}{100,0,100} +\definecolor{dgray}{RGB}{80,80,80} +\definecolor{lgray}{RGB}{220,220,220} +\definecolor{dred}{RGB}{190,0,0} +\definecolor{dgreen}{RGB}{0,110,0} +\definecolor{lyellow}{RGB}{245,245,210} +\definecolor{bblue}{RGB}{93,93,255} +\definecolor{bbrown}{RGB}{150,85,52} +\definecolor{llgray}{RGB}{230,230,230} + + + +\newcommand{\F}{\mathcal{F}} +\newcommand{\A}{\mathcal{A}} +\newcommand{\N}{\mathcal{N}} +\renewcommand{\H}{\mathcal{H}} +\newcommand{\Leff}{\mathcal{L}_{\rm eff}} +\newcommand{\heff}{\mathcal{H}_{\rm eff}} +\newcommand{\Lag}{\mathcal{L}} +\newcommand{\red}{\color{red}} +\newcommand{\blue}{\color{blue}} +\newcommand{\indigo}{\color{indigo}} +\newcommand{\brown}{\color{bbrown}} +\newcommand{\bs}{\mathbf} +\newcommand{\sss}{\scriptscriptstyle} +\newcommand{\btr}{{ $\blacktriangleright\ $}} + + +\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (CERN, IFJ PAN)} +\institute{UZH} +\title[Quo Vadis Flavour Anomalies?]{Quo Vadis Flavour Anomalies?} +\date{25 September 2014} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.9\textwidth} + \flushright\fontspec{Trebuchet MS}\bfseries \Huge {Quo Vadis Flavour Anomalies?} + \end{column} + \begin{column}{0.2\textwidth} + %\includegraphics[width=\textwidth]{SHiP-2} + \end{column} + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} {\fontspec{Trebuchet MS} \Large Marcin Chrząszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=1.3cm]{cern}{~}{~} +\includegraphics[height=1.1cm]{ifj.png} +\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + \textcolor{normal text.fg!50!Comment}{Białasówka seminar \\Novembar 30, 2018} +\end{center} +\end{frame} +} + + +\begin{frame}{Outline} + + \begin{minipage}{\textwidth} +{~}\\ + +\begin{enumerate} +\item Why flavour is important. +\item The flavour anomalies: +\begin{itemize} +\item $R(\PDstar)$ +\item $R_K$ and $R_{\PKstar}$ +\item $P_5^{\prime}$ +\end{itemize} +\item Global fits results. +\item Robustness of SM prediction. +\item Conclusions. +\end{enumerate} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Why flavour physics +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +Why Flavour is important? +\end{Huge} +\end{center} + + + + +\end{frame} + + + +\begin{frame}{A lesson from history - GIM mechanism} + \begin{minipage}{\textwidth} + +\begin{center} +\includegraphics[width=0.62\textwidth]{images/GIM2.png} +\end{center} +\begin{columns} +\column{0.7\textwidth} +\begin{itemize} +\begin{footnotesize} + + +\item Cabibbo angle was successful in explaining dozens of decay rates in the 1960s. +\item There was, however, one that was not observed by experiments: $\PKzero \to \Pmuon \APmuon$. +\item Glashow, Iliopoulos, Maiani (GIM) mechanism was proposed in the 1970 to fix this problem. The mechanism required the existence of a $4^{th}$ quark. +\item At that point most of the people were skeptical about that. Fortunately in 1974 the discovery of the $\PJpsi$ meson silenced the skeptics. +\end{footnotesize} +\end{itemize} +\column{0.3\textwidth} +\begin{center} +\includegraphics[width=0.95\textwidth]{images/GIM3.png}\\ +\includegraphics[width=0.7\textwidth]{images/604.jpg}\\{~}\\{~} +\end{center} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + +\begin{frame}{A lesson from history - CKM matrix} + \begin{minipage}{\textwidth} + +\begin{center} +{~}\\{~}\\ +\includegraphics[width=0.5\textwidth]{images/CKMmatrix.png} + +\end{center} +\begin{columns} +\column{0.6\textwidth} +\begin{itemize} +\begin{small} + + + + +\item Similarly, CP violation was discovered in 1960s in the neutral kaons decays. +\item $2 \times 2$ Cabbibo matrix could not allow for any CP violation. +\item For CP violation to be possible one needs at least a $3 \times 3$ unitary matrix \\ $\looparrowright$ Cabibbo-Kobayashi-Maskawa matrix (1973). +\item It predicts existence of $\Pbottom$ (1977) and $\Ptop$ (1995) quarks. +\end{small} + +\end{itemize} +\column{0.4\textwidth} +\begin{center} +{~} +%\includegraphics[height=2cm]{images/CP.png}\\ +\includegraphics[width=0.96\textwidth]{bottom.jpg} + +\end{center} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{A lesson from history - Weak neutral current} + \begin{minipage}{\textwidth} + +\begin{center} +\includegraphics[height=3cm]{images/weakcurr.png}{~} +\includegraphics[height=3cm]{images/weakcurr2.png} +\end{center} + +\begin{columns} +\column{0.6\textwidth} +\begin{itemize} +\begin{small} + + +\item Weak neutral currents were first introduced in 1958 by Buldman. +\item Later on they were naturally incorporated into unification of weak and electromagnetic interactions. +\item 't Hooft proved that the GWS models was renormalizable. +\item Everything was there on theory side, only missing piece was the experiment, till 1973. +\end{small} + +\end{itemize} +\column{0.4\textwidth} +\begin{center} +{~} +%\includegraphics[height=2cm]{images/CP.png}\\ +\includegraphics[width=0.85\textwidth]{images/bubblecern.png} +\end{center} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + + + +\iffalse + + + +\begin{frame} +\begin{center} +\begin{Huge} +LHCb detector +\end{Huge} +\end{center} + + + + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% DETECTOR +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\only<1>{\frametitle{LHCb detector - tracking} +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/sketch.png} +\end{columns} +\begin{itemize} +\item Excellent Impact Parameter (IP) resolution ($20~\rm \mu m$).\\ +$\Rightarrow$ Identify secondary vertices from heavy flavour decays +\item Proper time resolution $\sim~40~\rm fs$.\\ +$\Rightarrow$ Good separation of primary and secondary vertices. +\item Excellent momentum ($\delta p/p \sim 0.4 - 0.6\%$) and inv. mass resolution.\\ +$\Rightarrow$ Low combinatorial background. + +\end{itemize} + + +} + +\only<2>{\frametitle{LHCb detector - particle identification} +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/cher.png} +\end{columns} +\begin{itemize} +\item Excellent Muon identification $\epsilon_{\mu \to \mu} \sim 97\%$, $\epsilon_{\pi \to \mu} \sim 1-3\%$ +\item Good $\PK-\Ppi$ separation via RICH detectors, $\epsilon_{\PK \to \PK} \sim 95\%$, $\epsilon_{\Ppi \to \PK} \sim 5\%$.\\ +$\Rightarrow$ Reject peaking backgrounds. +\item High trigger efficiencies, low momentum thresholds. +Muons: $p_T > 1.76 \GeV$ at L0, $p_T > 1.0 \GeV$ at HLT1,\\ +$B \to \PJpsi X $: Trigger $\sim 90\%$. + +\end{itemize} + + +} + + +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Modern challenges: loops come in to the game} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\item Standard Model contributions suppressed or absent: +\begin{itemize} +\item Flavour Changing Neutral Currents. +\item CP violation +\item Lepton Flavour/Number or Lepton Universality violation. +\end{itemize} +\item In general can probe physics beyond General Purpose Detectors reach. +\end{itemize} +\column{0.5\textwidth} +\includegraphics[width=0.99\textwidth]{{images/TauLFV_UL_2014001_averaged}.png} + + +\end{columns} +\begin{center} +\includegraphics[width=0.75\textwidth]{images/Bsmumu.png} +\includegraphics[width=0.20\textwidth]{{images/bsmumu_SM}.png} +\end{center} +\end{minipage} + + \vspace*{2.1cm} +\end{frame} +\fi + + + + + +\begin{frame}\frametitle{Modern Flavour Physics} +\begin{center} +\only<1>{ +\includegraphics[width=1.05\textwidth]{1.png} +} +\only<2>{ +\includegraphics[width=1.05\textwidth]{2.png} + +} +\end{center} + + + + +\end{frame} + + +\begin{frame}\frametitle{Why semi-leptonic decays?} +\begin{large} +\ARROW A decay is semi-leptonic if its products are part leptons +and part hadrons. +\end{large} + +\begin{center} +\includegraphics[width=0.99\textwidth]{3.png} +\end{center} + +\begin{large} +\ARROW These decays can be factorised into the weak and +strong parts, greatly simplifying theoretical calculations. +\end{large} + + +\end{frame} + + + +\begin{frame}\frametitle{Types of semi-leptonic decays} + +\begin{center} +\includegraphics[width=1.05\textwidth]{4.png} +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Anomalies} +\only<1>{ +\begin{center} +\includegraphics[width=1.05\textwidth]{6.png} +\end{center} +} +\only<2>{ +\ARROW Today I will talk about three anomalies in $\PB$ +decays: +\begin{itemize} +\item $R(\PDstar)$ +\item $R_{\PK/\PKstar}$ +\item $P^{\prime}_5$ +\end{itemize} + +} + +\end{frame} + + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 1\\ +\begin{align*} +R(\PDstar) = \frac{\Br (\PB \to \PDstar \tau \nu )}{\Br(\PB \to \PDstar \mu \nu)} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{$R(\PDstar) $} + +\begin{large} + +\ARROW Large rate of charged current decays allow for measurement +in semi-tauonic decays +\end{large} + +\begin{columns} +\column{0.5\textwidth} +\begin{align*} +R(\PDstar) = \frac{\Br (\PB \to \PDstar \tau \nu )}{\Br(\PB \to \PDstar \mu \nu)} +\end{align*} +\column{0.5\textwidth} +\begin{large} +\ARROW Form ratio of decays with different lepton generations.\\ +\ARROW Cancel QCD uncertainties. +\end{large} + +\end{columns} +~\\ +\begin{large} + +\ARROW $R(\PDstar)$ is sensitive to the NP with strong 3rd generation couplings. +\end{large} + +\includegraphics[width=0.8\textwidth]{images/7.png} + + +\end{frame} + +\begin{frame}\frametitle{The Rule of three} + +\begin{center} + +\includegraphics[width=1.\textwidth]{images/8.png} + +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Experimental challenges} +\begin{large} +\ARROW With the $\tau \to \mu \nu \nu$ decay we are missing 3 neutrinos!\\ +\ARROW No sharp peak in any distributions.\\ +\end{large} +{~}\\ +\begin{columns} +\column{0.5\textwidth} +\begin{large} +\ARROW At B-factories, can control this +using tagging technique.\\ +\end{large} + + +\includegraphics[width=0.9\textwidth]{9.png} + +\column{0.5\textwidth} + + +\includegraphics[width=0.9\textwidth]{10.png}\\ +\begin{large} +\ARROW More difficult at LHCb, compensate +using large boost (flight information) +and huge B production\\ +\end{large} +\end{columns} + +\end{frame} + +\begin{frame}\frametitle{Signal fits} +\ARROW Three main backgrounds: +\begin{itemize} +\item $\PB \to \PDstar \ell \nu$. +\item $\PB \to \PD^{\ast \ast} \ell \nu$. +\item $\PB \to \PD \PDstar X$ +\end{itemize} +\begin{center} +\includegraphics[width=0.9\textwidth]{12.png} +\end{center} +\ARROW Fit variables which discriminate between the signal and background modes. + +\end{frame} + +\begin{frame}\frametitle{Results} +\ARROW All experiments see an access w.r.t. to SM prediction: +\begin{center} +\includegraphics[angle=-90,width=0.6\textwidth]{rdrds_summer18.pdf} +\end{center} +\ARROW Theoretical uncertainties negligible.\\ +\ARROW The ball is on the experimental side. + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + + +\begin{frame}\frametitle{Introduction to anomaly 2 \& 3} + +\begin{columns} +\column{4in} +\begin{itemize} +\item The SM allows only the charged interactions to change flavour. +\begin{itemize} +\item Other interactions are flavour conserving. +\end{itemize} +\item One can escape this constraint and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. +\begin{itemize} +\item These kind of processes are suppressed in SM $\to$~Rare decays. +\item New Physics can enter in the loops. +\end{itemize} +\end{itemize} +\begin{center} +\includegraphics[scale=0.3]{lupa.png} +\includegraphics[scale=0.3]{example.png} +\end{center} +\column{1.5in} +\includegraphics[width=0.61\textwidth]{couplings.png} +\end{columns} + +\end{frame} + + +\begin{frame}{Analysis of Rare decays} +\begin{footnotesize} + +%{\Large Since a long time ago...} \\ \medskip +%\hspace*{1.4cm}$\Rightarrow$ $b \to s \gamma$ and $b \to s \ell\ell $ {\bf Flavour Changing Neutral Currents} have been used as {\bf \cred Our Portal} \\ to explore the fundamental theory beyond SM. \\ +%\medskip +%\medskip +%\hfill....... with not much success till 2013.\hspace*{1cm} +%\bigskip + +Analysis of FCNC in a model-independent approach, effective Hamiltonian: +\vspace*{-0.1cm} +\begin{columns} +\begin{column}{1cm} +~ +\end{column} +\begin{column}{8cm} +\begin{equation*} +b\to s\gamma(^*): {\mathcal H}^{SM}_{\Delta F=1} \propto + \sum_{i=1}^{10} V_{ts}^* V_{tb} {\cgreen \C{i}} \alert{ {\cal O}_i} + \ldots +\end{equation*} + +\vspace{-0.2cm} + +\begin{itemize} +\item $\alert{ {\cal O}_7} = \frac{e}{16 \pi^2}m_b\, + (\bar s\sigma^{\mu\nu} P_R b) F_{\mu\nu}\,$ %\quad [real or soft photon] +\item $\alert{ {\cal O}_9}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b)\ (\bar\ell\gamma_\mu\ell)$ + %\quad [$b\to s\mu\mu$ via $Z$/hard $\gamma$] +\item $\alert{ {\cal O}_{10}}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b) \ (\bar\ell\gamma_\mu\gamma_5\ell)$, ... +%\quad [$b\to s\mu\mu$ via $Z$] +\end{itemize} +\end{column} +\begin{column}{5.5cm} +\includegraphics[width=3.5cm]{images/qum1.png} +%\includegraphics[width=3cm]{bsll.pdf} +\end{column} +\end{columns} + +%\hspace*{5cm} with no clear success yet... +%\bigskip + + +%\centerline{{\bf Goal}: \underline{Decode the short distance physics to find a smoking gun of BSM}\hspace*{2cm}} + + +\bigskip +\hspace*{0.0cm} $\bullet$ {\bf SM} Wilson coefficients up to NNLO + e.m. corrections at $\mu_{ref}=4.8$ GeV [{\cgreen Misiak et al.}]: $${\cal C}_7^{\rm SM}=-0.29,\, {\cal C}_9^{\rm SM}=4.1,\, {\cal C}_{10}^{\rm SM}=-4.3$$ +%BUT, like in the film there is always the good, the bad and the ugly. +\bigskip +$\bullet$ {\bf NP} changes short distance ${\cal C}_i-{\cal C}_i^{\rm SM}={\cal C}_i^{\rm NP}$ and induce new operators, like ${\cal O}^\prime_{7,9,10}={\cal O}_{7,9,10}\,\, (P_L \leftrightarrow P_R)$ ... also scalars, pseudoescalar, tensor operators...%\bigskip + + +\end{footnotesize} + +\end{frame} + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 2\\ +\begin{align*} +R_{\PK/\PKstar} = \frac{\Br(\PB \to \PK/\PKstar \mu \mu)}{\Br(\PB \to \PK/\PKstar e e)} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + + + +\begin{frame}\frametitle{Measurement at LHCb} + +\ARROW Most precise measurements performed at LHCb.\\ +\ARROW Main challenge is due to electron Bremsstrahlung.\\ +\begin{center} +\includegraphics[width=0.99\textwidth]{13.png} +\end{center} +\ARROW To protect ourself from electron reconstruction issue we use double ratio: +\begin{align*} +R_K = \frac{ \Br(\PB \to \PK \mu \mu ) \times \Br(\PB \to \PK \PJpsi(\to e e)) }{ \Br(\PB \to \PK e e ) \times \Br(\PB \to \PK \PJpsi(\to \mu \mu)) } +\end{align*} + + +\end{frame} + + +\begin{frame}\frametitle{Result} + +\begin{center} +\begin{large} +\begin{align*} +R_K = 0.745^{+0.090}_{-0.074} ({\rm stat.}) \pm 0.036 ({\rm syst}) +\end{align*} +\end{large} + +\includegraphics[width=0.7\textwidth]{images/RK.png}\\ + +\end{center} +\ARROW $2.6~\sigma$ away from SM prediction. +\end{frame} + +\begin{frame}\frametitle{The continuation - $R_{\PKstar}$} +\ARROW The neutral continuation of the $R_K$ measurement is to measure its partner: +\begin{center} +\begin{align*} +R_{\PKstar} = \frac{\Br(\PB \to \PKstar \mu \mu)}{\Br(\PB \to \PKstar e e)} +\end{align*} +\end{center} + + +\begin{columns} +\column{0.4\textwidth} +\ARROW Measurement performed in two $q^2$ bins. \\ +\ARROW Normalized in double ratio to $\PB \to \PKstar \PJpsi$.\\ +\includegraphics[width=0.95\textwidth]{images/plot.png} + + +\column{0.6\textwidth} +\begin{center} +\includegraphics[width=0.95\textwidth]{Fig10a.pdf} +\end{center} + +\end{columns} + + + +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PB \to \PKstar^{\pm} \Pmu \Pmu$} +{~} +\includegraphics[width=0.5\textwidth]{images/ksmumu_BF.png} +\includegraphics[width=0.5\textwidth]{images/kmumu_BF.png} + +\begin{center} +\begin{columns} + +\column{0.4\textwidth} +\begin{itemize} +\item Despite large theoretical errors the results are consistently smaller than SM prediction. +\end{itemize} +\column{0.6\textwidth} +\includegraphics[width=0.87\textwidth]{images/bukst_BF.png} + + +\end{columns} + + + + + + + +\end{center} + \vspace*{2.1cm} +\end{frame} + + + + + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 3\\ +\begin{align*} +P_5^{\prime} = \sqrt{2} \frac{\Re (\apeL \apaL^{\ast} - \apeR \apaR^{\ast} )}{\sqrt{ |\aze|^2 ( |\ape|^2 + |\aze|^2 )}} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + + +%\azeLR +%\apaLR +%\apeLR + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{$\PBzero \to \PKstar \Pmuon \APmuon$ kinematics} +{~} + \begin{minipage}{\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ The kinematics of $\PBzero \to \PKstar \Pmuon \APmuon$ decay is described by three angles $\thetal$, $\thetak$, $\phi$ and invariant mass of the dimuon system ($q^2)$. + + \only<1>{ +\begin{columns} +\column{0.5\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ $\cos \thetak$: the angle between the direction of the kaon in the $\PKstar$ ($\overline{\PKstar}$) rest frame and the direction of the $\PKstar$ ($\overline{\PKstar}$) in the $\PBzero$ ($\APBzero$) rest frame.\\ +$\color{JungleGreen}{\Rrightarrow}$ $\cos \thetal$: the angle between the direction of the $\Pmuon$ ($\APmuon$) in the dimuon rest frame and the direction of the dimuon in the $\PBzero$ ($\APBzero$) rest frame.\\ +$\color{JungleGreen}{\Rrightarrow}$ $\phi$: the angle between the plane containing the $\Pmuon$ and $\APmuon$ and the plane containing the kaon and pion from the $\PKstar$. + + + +\column{0.5\textwidth} +\includegraphics[width=0.95\textwidth]{images/angles.png} + +\end{columns} + } + \only<2>{ +{\tiny{ +\eqa{\label{dist} +\frac{d^4\Gamma}{dq^2\,d\!\cos\theta_K\,d\!\cos\theta_l\,d\phi}&=&\frac9{32\pi} \bigg[ +J_{1s} \sin^2\theta_K + J_{1c} \cos^2\theta_K + (J_{2s} \sin^2\theta_K + J_{2c} \cos^2\theta_K) \cos 2\theta_l\nn\\[1.5mm] +&&\hspace{-2.7cm}+ J_3 \sin^2\theta_K \sin^2\theta_l \cos 2\phi + J_4 \sin 2\theta_K \sin 2\theta_l \cos\phi + J_5 \sin 2\theta_K \sin\theta_l \cos\phi \nn\\[1.5mm] +&&\hspace{-2.7cm}+ (J_{6s} \sin^2\theta_K + {J_{6c} \cos^2\theta_K}) \cos\theta_l ++ J_7 \sin 2\theta_K \sin\theta_l \sin\phi + J_8 \sin 2\theta_K \sin 2\theta_l \sin\phi \nn\\[1.5mm] +&&\hspace{-2.7cm}+ J_9 \sin^2\theta_K \sin^2\theta_l \sin 2\phi \bigg]\,, +\nonumber} +}} + +$\color{JungleGreen}{\Rrightarrow}$ This is the most general expression of this kind of decay.\\ +\ARROW The $12$ observables $(J_i)$ can be reduced to $8$ thanks to some symmetries. + + + +} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Transversity amplitudes } +{~} + \begin{minipage}{\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ One can link the angular observables to transversity amplitudes +{\tiny{ +\eqa{ +J_{1s} & = & \frac{(2+\beta_\ell^2)}{4} \left[|\apeL|^2 + |\apaL|^2 +|\apeR|^2 + |\apaR|^2 \right] + + \frac{4 m_\ell^2}{q^2} \re\left(\apeL\apeR^* + \apaL\apaR^*\right)\,,\nn\\[1mm] +% +J_{1c} & = & |\azeL|^2 +|\azeR|^2 + \frac{4m_\ell^2}{q^2} \left[|A_t|^2 + 2\re(\azeL^{}\azeR^*) \right] + \beta_\ell^2\, |A_S|^2 \,,\nn\\[1mm] +% +J_{2s} & = & \frac{ \beta_\ell^2}{4}\left[ |\apeL|^2+ |\apaL|^2 + |\apeR|^2+ |\apaR|^2\right], +\hspace{0.92cm} J_{2c} = - \beta_\ell^2\left[|\azeL|^2 + |\azeR|^2 \right]\,,\nn\\[1mm] +% +J_3 & = & \frac{1}{2}\beta_\ell^2\left[ |\apeL|^2 - |\apaL|^2 + |\apeR|^2 - |\apaR|^2\right], +\qquad J_4 = \frac{1}{\sqrt{2}}\beta_\ell^2\left[\re (\azeL\apaL^* + \azeR\apaR^* )\right],\nn \\[1mm] +% +J_5 & = & \sqrt{2}\beta_\ell\,\Big[\re(\azeL\apeL^* - \azeR\apeR^* ) - \frac{m_\ell}{\sqrt{q^2}}\, +\re(\apaL A_S^*+ \apaR^* A_S) \Big]\,,\nn\\[1mm] +% +J_{6s} & = & 2\beta_\ell\left[\re (\apaL\apeL^* - \apaR\apeR^*) \right]\,, +\hspace{2.25cm} J_{6c} = 4\beta_\ell\, \frac{m_\ell}{\sqrt{q^2}}\, \re (\azeL A_S^*+ \azeR^* A_S)\,,\nn\\[1mm] +% +J_7 & = & \sqrt{2} \beta_\ell\, \Big[\im (\azeL\apaL^* - \azeR\apaR^* ) + +\frac{m_\ell}{\sqrt{q^2}}\, \im (\apeL A_S^* - \apeR^* A_S)) \Big]\,,\nn\\[1mm] +% +J_8 & = & \frac{1}{\sqrt{2}}\beta_\ell^2\left[\im(\azeL\apeL^* + \azeR\apeR^*)\right]\,, +% +\hspace{1.9cm} J_9 = \beta_\ell^2\left[\im (\apaL^{*}\apeL + \apaR^{*}\apeR)\right] \,, +\label{Js}\nonumber} +}} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Link to effective operators} +{~} + \begin{minipage}{\textwidth} +$\color{JungleGreen}{\Rrightarrow}$ So here is where the magic happens. At leading order the amplitudes can be written as: +{\tiny{ +\eqa{ +\apeLR &=&\sqrt{2} N m_B(1- \hat s)\bigg[ (\Ceff9 + \Cpeff9) \mp (\C{10} + \Cp{10}) ++\frac{2\hat{m}_b}{\hat s} (\Ceff7 + \Cpeff7) \bigg]\xi_{\bot}(E_{K^*}) \nn \\[2mm] +\apaLR &=& -\sqrt{2} N m_B (1-\hat s)\bigg[(\Ceff9 - \Cpeff9) \mp (\C{10} - \Cp{10}) ++\frac{2\hat{m}_b}{\hat s}(\Ceff7 - \Cpeff7) \bigg] \xi_{\bot}(E_{K^*}) \nn \\[2mm] +\azeLR &=& -\frac{N m_B (1-\hat s)^2}{2 \hat{m}_{K^*} \sqrt{\hat s}} \bigg[ (\Ceff9 - \Cpeff9) \mp (\C{10} - \Cp{10}) + 2\hat{m}_b (\Ceff7 - \Cpeff7) \bigg]\xi_{\|}(E_{K^*}), +\label{LargeRecoilAs}\nonumber} +}} +where $\hat s = q^2 /m_B^2$, $\hat{m}_i = m_i/m_B$. The $\xi_{\|,\bot }$ are the form factors. \\ +\pause +$\color{JungleGreen}{\Rrightarrow}$ Now we can construct observables that cancel the $\xi$ form factors at leading order: +\eq{P_5^{\prime} = \dfrac{J_5+\bar{J}_5}{2\sqrt{-(J_2^c+\bar{J}_2^c)(J_2^s+\bar{J}_2^s)} }\nonumber +} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +LHCb measurement of $\PBd \to \PKstar \Pmu \Pmu$ +\end{Huge} +\end{center} + + + + +\end{frame} +\iffalse + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{LHCbs $\PBzero \to \PKstar \Pmuon \APmuon$, Selection} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\begin{columns} +\column{0.2in} +{~} +\column{2in} +\ARROW Trigger +\begin{itemize} +\item Muon trigger. +\item Topological trigger. +\end{itemize} +\ARROW Good modelling with MC. \\ +\ARROW Selection: +\begin{itemize} +\item As loose as possible. +\item Based on the $\PBzero$ vertex quality, impact parameters, loose Particle identification for the hadrons. +\item The variables were chosen in a way we are sure the are correctly modelled in MC. +\end{itemize} +\column{2.8in} + +\includegraphics[angle=-90,width=0.75\textwidth]{{images/tistos_L0Muon_pt}.pdf}\\ +\includegraphics[angle=-90,width=0.75\textwidth]{{images/tistos_L0Muon_costhetal}.pdf} +\end{columns} + + + +\end{footnotesize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Peaking backgrounds} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\ARROW A number of peaking backgrounds that can mistaken as your signal.\\ +\ARROW There where a specially designed vetoes to fight each of them. +\begin{center} +\begin{tiny} +\hspace{-1cm}\begin{tabular}{ r | c c | c c } + \hline + & \multicolumn{2}{c|}{after preselection, before vetoes} & \multicolumn{2}{c }{after vetoes and selection}\\ + Channel & Estimated events & \% signal & Estimated events & \% signal \\ + \hline + \hline + $\PLambda_b \to \PLambda^{\ast}(1520)^{0} \mu\mu$ &$ (1.0\pm0.5)\times10^3 $&$ 19\pm8 $&$ 51\pm25 $&$ 1.0\pm0.4$\\ + $\PLambda_b \to {\rm p } \PK \mu\mu$ &$ (1.0\pm0.5)\times10^2 $&$ 1.9\pm0.8 $&$ 5.7\pm2.8 $&$ 0.11\pm0.05$ \\ + $\PBd \to \PKplus \mu \mu$ &$ 28\pm7 $&$ 0.55\pm0.06 $&$ 1.6\pm0.5 $&$ 0.031\pm0.006$\\ +$\PBs \to \Pphi \mu \mu$ &$ (3.2\pm1.3)\times10^2 $&$ 6.2\pm2.1 $&$ 17\pm7 $&$ 0.33\pm0.12$\\ +signal swaps &$ (3.6\pm0.9)\times10^2 $&$ 6.9\pm0.6 $&$ 33\pm9 $&$ 0.64\pm0.06$ \\ +$\PBd \to \PKstar \PJpsi$ swaps &$ (1.3\pm0.4)\times10^2 $&$ 2.6\pm0.4 $&$ 2.7\pm2.8 $&$ 0.05\pm0.05$ \\ + + \hline + \end{tabular} +\end{tiny} +\includegraphics[angle=-90,width=0.49\textwidth]{{images/h_Bd_Kstmm_vetoes}.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{{h_Lb_L1520mm_vetoes}.pdf} + +\end{center} + + + + +\end{footnotesize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +\fi + + +\iffalse +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate selection} +{~} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\begin{footnotesize} +\item PID, kinematics and isolation variables used in a Boosted Decision Tree (BDT) to discriminate signal and background. +\item BDT with k-Folding technique. +\item Completely data driven. +\end{footnotesize} +\end{itemize} +\begin{center} +\includegraphics[width=0.70\textwidth]{images/Chopping_Distrib.pdf} +\end{center} + +\column{0.5\textwidth} + +\includegraphics[angle=-90,width=0.82\textwidth]{images/Fig1.pdf} \\ +\includegraphics[width=0.88\textwidth]{images/fold.png} + +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +\fi +\iffalse + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate selection, efficiency} +{~} + + \begin{minipage}{\textwidth} + \begin{footnotesize} + +\ARROW BDT was also checked in order not to bias our angular distribution: +\begin{center} +\includegraphics[angle=-90,width=0.8\textwidth]{images/BDT_Eff_Comp.pdf} +\end{center} +\ARROW The BDT has small impact on our angular observables. We will correct for these effects later on. + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\iffalse + +\begin{frame}{Mass modelling} +{~} +\begin{minipage}{\textwidth} +\begin{tiny} +\begin{columns} +\column{0.1in} +{~} +\column{2.5in} +\ARROW The signal is modelled by a sum of two Crystal-Ball functions with common mean.\\ +\ARROW The background is a single exponential.\\ +\ARROW The base parameters are obtained from the proxy channel: $\PBd \to \PJpsi (\mu\mu) \PKstar$.\\ +\ARROW All the parameters are fixed in the signal pdf.\\ +\ARROW Scaling factors for resolution are determined from MC.\\ +\ARROW In fitting the rare mode only the signal, background yield and the slope of the exponential is left floating.\\ +\begin{center} +\includegraphics[angle=-90,width=0.9\textwidth]{images/msignal.pdf}\\ + +\end{center} +\ARROW We found $624\pm30$ candidates in the most interesting $\left[1.1,6.0\right]~\GeV^2/c^4$ region \\ and $2398 \pm 57$ in the full range $\left[ 1.1, 19.\right]~\GeV^2/c^4$. +\column{2.5in} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/FitJpsiKstar_withBDT_withoutPartially}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/Scaling_factor}.pdf}\\ +\ARROW The S-wave fraction is extracted using a \texttt{LASS} model. +\end{columns} + +\end{tiny} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +\fi +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Monte Carlo corrections} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\ARROW No Monte Carlo simulation is perfect! One needs to correct for remaining differences.\\ +\ARROW We reweighted our $\PBd \to \PKstar \mu \mu$ Monte Carlo accordingly to differences between the $\PBd \to \PKstar \PJpsi$ in data (Splot) and Monte Carlo. +\only<1>{ +\begin{center} +\includegraphics[angle=-90,width=0.38\textwidth]{images/pt.pdf} +\includegraphics[angle=-90,width=0.38\textwidth]{images/vertex.pdf}\\ +\includegraphics[angle=-90,width=0.38\textwidth]{images/nTracks.pdf} +\end{center} +} +\only<2>{ +\begin{center} +\includegraphics[angle=-90,width=0.38\textwidth]{images/eta_logy.pdf} +\includegraphics[angle=-90,width=0.38\textwidth]{images/B0_p.pdf} \\ +\includegraphics[angle=-90,width=0.38\textwidth]{{images/bdt_data_mc_nominalMkpi}.pdf} +\end{center} +} + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +\fi + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{The columns of New Physics} +{~} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[width=0.94\textwidth]{images/columns.png} + + \end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{The columns of New Physics} +{~} + \begin{minipage}{\textwidth} +\begin{enumerate} +\item Maximum likelihood fit: +\begin{itemize} +\item The most standard way of obtaining the parameters. +\item Suffers from convergence problems, under coverages, etc. in low statistics. +\end{itemize} +\item Method of moments: +\begin{itemize} +\item Less precise then the likelihood estimator ($10-15\%$ larger uncertainties). +\item Does not suffer from the problems of likelihood fit. +\end{itemize} +\item Amplitude fit: +\begin{itemize} +\item Incorporates all the physical symmetries inside the amplitudes! The most precise estimator. +\item Has theoretical assumptions inside! +\end{itemize} +\end{enumerate} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\iffalse +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} +{~} +\begin{footnotesize} + + \begin{minipage}{\textwidth} +\ARROW In the maximum likelihood fit one could weight the events accordingly to the $\dfrac{1}{\varepsilon(\cos \thetal, \cos \thetak, \phi, q^2)}$\\ +\ARROW Better alternative is to put the efficiency into the maximum likelihood fit itself: +\begin{align*} +\mathcal{L}=\prod_{i=1}^N \epsilon_i(\Omega_i, q_i^2) \mathcal{P}(\Omega_i, q_i^2) / \int \epsilon(\Omega, q^2) \mathcal{P}(\Omega, q^2) d\Omega dq^2 +\end{align*} +\ARROW Only the relative weights matters!\\ +\ARROW The Procedure was commissioned with TOY MC study.\\ +\ARROW Use Feldmann-Cousins to determine the uncertainties. \\ +\ARROW Angular background component is modelled with $2^{\rm nd }$ order Chebyshev polynomials, which was tested on the side-bands.\\ +\ARROW S-wave component treated as nuisance parameter.\\ +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_Afb3}.pdf} +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_P11}.pdf} +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_P57}.pdf} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} +\iffalse +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} +{~} + \begin{minipage}{\textwidth} +\begin{center} +\only<1>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/FLPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S3Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/S4Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S5Pad.pdf} +} +\only<2>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/AFBPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S7Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/S8Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S9Pad.pdf} +} + + +\end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +\fi + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[angle=-90,width=0.65\textwidth]{images/P5pPadOverlay.pdf}\\ + \end{center} + +\begin{itemize} +\item Tension with $3~\invfb$ gets confirmed! +\item two bins both deviate by $2.8~\sigma$ from SM prediction. +\item Result compatible with previous result. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +\fi + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Method of moments} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} +\ARROW See {\color{blue}{\href{http://arxiv.org/abs/1503.04100}{Phys.Rev.D91(2015)114012}}}, F.Beaujean , M.Chrzaszcz, N.Serra, D. van Dyk for details.\\ +\ARROW The idea behind Method of Moments is simple: Use orthogonality of spherical harmonics, $f_j(\overrightarrow{\Omega})$ to solve for coefficients within a $q^2$ bin: +\begin{align*} +\int f_i(\overrightarrow{\Omega}) f_j(\overrightarrow{\Omega}) = \delta_{ij} +\end{align*} +\begin{align*} +M_i = \int \left( \dfrac{1}{d(\Gamma+ \bar{\Gamma})/dq^2} \right) \dfrac{d^3(\Gamma+\bar{\Gamma})}{d \overrightarrow{\Omega}} f_i(\overrightarrow{\Omega})d \Omega +\end{align*} +\ARROW Don’t have true angular distribution but we ''sample'' it with our data.\\ +\ARROW Therefore: $\int \to \sum$ and $M_i \to \widehat{M}_i$ +\begin{align*} +\hat{M}_i=\dfrac{1}{\sum_e \omega_e} \sum_e \omega_e f_i(\overrightarrow{\Omega}_e) +\end{align*} +\ARROW The weight $\omega$ accounts for the efficiency. Again the normalization of weights does not matter. + + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Method of moments - results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + +\only<3> +{ +\ARROW Method of Moments allowed us to measure for the first time a new observable: +} + +\begin{center} +\only<1>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_FLPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S3Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S4Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S5Pad.pdf} +} +\only<2>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_AFBPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S7Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S8Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S9Pad.pdf} +} +\only<3>{ +\includegraphics[angle=-90,width=0.75\textwidth]{images/S6cPad.pdf} +} + +\end{center} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + + + + + +\begin{frame}{Compatibility with SM} +{~} + + \begin{minipage}{\textwidth} + +\begin{columns} +\column{0.1in} +{~} +\column{2in} +\ARROW Use \texttt{EOS} software package to test compatibility with SM.\\ +\ARROW Perform the $\chi^2$ fit to the measured: +\begin{center} +\begin{align*} +F_L, A_{FB}, S_{3,..., 9} . +\end{align*} +\end{center} +\ARROW Float a vector coupling: $\Re(C_9)$.\\ +\ARROW Best fit is found to be $3.4~\sigma$ away from the SM. + + +\column{3in} +\begin{align*} +\Delta \Re (C_9) \equiv \Re(C_9)^{{\rm fit}} - \Re(C_9)^{{\rm SM}} = -1.03 +\end{align*} +\includegraphics[angle=-90,width=0.95\textwidth]{images/wilsonchi2.pdf} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}\frametitle{Global picture of $P_5^{\prime}$} + +\begin{columns} + +\column{0.4\textwidth} +\only<1>{{\color{gray}{\ARROW 2013 LHCb: \href{https://arxiv.org/pdf/1308.1707.pdf}{arXiv::1308.1707}}}\\} +\only<1>{\ARROW 2015 LHCb: \href{https://arxiv.org/abs/1512.04442}{arXiv::1512.0444}\\} +\only<1>{{\color{red}{\ARROW 2016 Belle: \href{https://arxiv.org/abs/1604.04042}{arXiv::1604.04042}}}\\} +\only<1>{\ARROW 2017: {\color{blue}{\href{https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2017-023/}{ATLAS-CONF-2017-023}}} $(20.5~\rm fb^{-1})$ and {\color{OliveGreen}{\href{http://cds.cern.ch/record/2256738?ln=en}{CMS-PAS-BPH-15-008}}} $(20.8~\rm fb^{-1})$} + + + +\column{0.6\textwidth} +\only<1>{ +\ARROW Theory: +~~DHMV: \href{https://arxiv.org/abs/1407.8526}{arXiv::1407.8526} +~~ASZB: \href{https://arxiv.org/abs/1411.3161}{arXiv::1411.3161} +} +%\includegraphics[width=0.95\textwidth]{images/P5p1.png} +\only<1>{ +\includegraphics[angle=-90,width=0.9\textwidth]{images/P5p.pdf} +} + + +\end{columns} +\only<1>{ + + +} + +\end{frame} + + + +\iffalse + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PLambdab \to \PLambda \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + + \begin{center} + \only<1>{ + \includegraphics[width=0.65\textwidth]{images/Lb_BR.png} +} + \only<2>{ + \includegraphics[width=0.45\textwidth]{images/Lblow.png} +\includegraphics[width=0.45\textwidth]{images/Lbhigh.png} + +} + + + \end{center} + + +\begin{itemize} +\item This years LHCb measurement [JHEP 06 (2015) 115]]. +\item In total $\sim 300$ candidates in data set. +\item Decay not present in the low $q^2$. + +\end{itemize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}{Angular analysis of $\PLambdab \to \PLambda \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item For the bins in which we have $>3~\sigma$ significance the forward backward asymmetry for the hadronic and leptonic system. +\end{itemize} +\begin{center} +\includegraphics[width=0.9\textwidth]{{images/AFB_Lb}.png} +\end{center} +\begin{itemize} +\item $A_{FB}^H$ is in good agreement with SM. +\item $A_{FB}^{\ell}$ always in above SM prediction. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Lepton universality test} +{~} + \begin{minipage}{\textwidth} +\begin{columns} +\column{3.0in} +\begin{itemize} +\item If $\PZprime$ is responsible for the $P'_5$ anomaly, does it couple equally to all flavours? +\includegraphics[width=0.9\textwidth]{images/uni2.png} +\item Challenging analysis due to bremsstrahlung. +\item Migration of events modeled by MC. +\item Correct for bremsstrahlung. +\item Take double ratio with $\PBplus \to \PJpsi \PKplus$ to cancel systematics. +\item In $3\invfb$, LHCb measures $R_K=0.745^{+0.090}_{-0.074}(stat.)^{+0.036}_{-0.036}(syst.)$ +\item Consistent with SM at $2.6\sigma$. + +\end{itemize} +\column{2.0in} +\includegraphics[width=0.99\textwidth]{images/RK.png}\\ +\begin{itemize} +\item \href{http://arxiv.org/abs/1406.6482}{Phys. Rev. Lett. 113, 151601 (2014)} +\end{itemize} +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Angular analysis of $\PBzero \to \PKstar \Pe \Pe$} +{~} +\only<1>{ + \begin{minipage}{\textwidth} + \begin{itemize} + \item With the full data set ($3\invfb$) we performed angular analysis in $0.0004 < q^2 <1~\GeV^2$. + \item Electrons channels are extremely challenging experimentally: + \begin{itemize} + \item Bremsstrahlung. + \item Trigger efficiencies. + \end{itemize} + \item Determine the angular observables: $\FL$, $\ATD$, $\ATRe$, $\ATIm$: + \end{itemize} +\begin{equation} + \label{eq:physPars} + \begin{split} + \FL &=\frac{|A_0|^2}{|A_0|^2+|A_{||}|^2 + |A_\perp|^2}\\ + \ATD &= \frac{|A_\perp|^2-|A_{||}|^2}{|A_\perp|^2+|A_{||}|^2}\\ + \ATRe &= \frac{2\Real(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}\\ + \ATIm &= \frac{2\Imag(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}, +\end{split}\nonumber +\end{equation} + +\end{minipage} +} +\only<2>{ +\begin{center} +\includegraphics[width=0.5\textwidth]{images/Kstee.png}\\ +\end{center} +\begin{itemize} +\item Results in full agreement with the SM. +\item Similar strength on $C_7$ Wilson coefficient as from $\Pbeauty \to \Pstrange \Pphoton$ decays. +\end{itemize} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/Kstee2.png} +\end{center} + +} + \vspace*{2.1cm} +\end{frame} + +\fi + +\begin{frame} +\begin{center} +\begin{Huge} +Global fit to $\Pbeauty \to \Pstrange \ell \ell$ measurements +\end{Huge} +\end{center} + + + + +\end{frame} + + + +\begin{frame}{Link the observables} +\begin{footnotesize} + +\ARROW Fits prepare by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}} + +\begin{itemize} + +\item Inclusive + +\begin{itemize} +\item $B\to X_s\gamma$ {\color{gray}($BR$) +.......................................................... } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} +\item $B\to X_s\ell^+\ell^-$ {\color{gray}($dBR/dq^2$) +............................................ } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} +\end{itemize} + +\item Exclusive leptonic + +\begin{itemize} +\item $B_s\to \ell^+\ell^-$ {\color{gray}($BR$) +........................................................ } {\color{red} $\C{10}^{(\prime)}$} +\end{itemize} + +\item Exclusive radiative/semileptonic +\begin{itemize} +\item $B\to K^*\gamma$ {\color{gray}($BR$, $S$, $A_I$) +................................................ } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $B\to K\ell^+\ell^-$ {\color{gray}($dBR/dq^2$) +.............................................. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $\bf \color{Red} B\to K^*\ell^+\ell^-$ {\color{gray}($dBR/dq^2$, {\bf Optimized Angular Obs.}) +.. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $B_s\to \phi \ell^+\ell^-$ {\color{gray}($dBR/dq^2$, Angular Observables) +.............. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $\Lambda_b\to \Lambda\ell^+\ell^-$ {\color{gray}(None so far)} +\item etc. +\end{itemize} + + + +\end{itemize} +\end{footnotesize} + +\end{frame} + +\frame{ \frametitle{Statistic details} + +\begin{footnotesize} + +\ARROW Frequentist approach: +\medskip + +$$\chi^2(C_i) = [O_\text{exp}- O_\text{th}(C_i)]_j \, [Cov^{-1}]_{jk}\, [O_\text{exp}- O_\text{th}(C_i)]_k$$ + + +\begin{itemize} +\item $\bf Cov = Cov^\text{exp} + Cov^\text{th}$. We have $Cov^\text{exp}$ for the first time +\item Calculate $Cov^\text{th}$: correlated multigaussian scan over all nuisance parameters +\item $Cov^\text{th}$ depends on $C_i$: Must check this dependence\\[5mm] +\end{itemize} +For the Fit: +\begin{itemize} +\item Minimise $\chi^2 \to \chi^2_\text{min} = \chi^2(C_i^0)\quad$ (Best Fit Point = $C_i^0$) +\item Confidence level regions: $\chi^2(C_i) - \chi^2_\text{min} < \Delta\chi_{\sigma,n}$ +%\item Compute pulls by inversion of the above formula +\end{itemize} +\medskip +\ARROW The results from 1D scans:{~}\\{~}\\ +\begin{tiny} +\begin{tabular}{crccc} +%\toprule[1.6pt] +Coefficient ${\cal C}_i^{NP}={\cal C}_i-{\cal C}_i^{SM}$ & Best fit & 1$\sigma$ & 3$\sigma$ & Pull$_{\rm SM}$ \\ \hspace{10mm} \\[5mm] +% \midrule + $\bf\cred\C9^{\rm NP}$ & $ -1.09 $ & $ [-1.29,-0.87] $ & $ [-1.67,-0.39] $ & $\,\,\,\,\,\,\bf 4.5 + \cred \Leftarrow$ \hspace{5mm} \\[3mm] + $\C9^{\rm NP}=-\C{10}^{\rm NP}$ & $ -0.68 $ & $ [-0.85,-0.50] $ & $ [-1.22,-0.18] $ & \bf \quad 4.2 + $\cred\Leftarrow$ \hspace{5mm} \\[3mm] + $\C9^{\rm NP}=-\C{9'}^{\rm NP}$ & $ -1.06 $ & $ [-1.25,-0.86] $ & $ [-1.60,-0.40] $ & \quad \quad \quad \,\,\quad 4.8 + $\cred\Leftarrow$ (no $R_K$)\hspace{5mm} \\[3mm] + + \hspace{5mm} \\[3mm] +% \bottomrule[1.6pt] +\end{tabular} +\end{tiny} +\end{footnotesize} + +} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Theory implications} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item The data can be explained by modifying the $C_9$ Wilson coefficient. +\item Overall there is around $4.5~\sigma$ discrepancy wrt. SM. +\end{itemize} +\includegraphics[width=0.9\textwidth]{images/C9.png} + + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{2D scans} +{~} +\begin{footnotesize} + + \begin{minipage}{\textwidth} +\begin{columns} +\begin{column}{0.5cm} + + +\end{column} +\begin{column}{17cm} + +\renewcommand{\arraystretch}{1.4} + \setlength{\tabcolsep}{13pt} +\begin{tabular}{cccr} +\hline +Coefficient & Best Fit Point & Pull$_{\rm SM}$ \\ \hline + + $(\C7^{\rm NP},\C9^{\rm NP})$ & $(-0.00,-1.07)$ & {\bf 4.1} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{10}^{\rm NP})$ & $(-1.08,0.33)$ & {\bf 4.3} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{7'}^{\rm NP})$ & $(-1.09,0.02)$ & {\bf 4.2} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{9'}^{\rm NP})$ & $(-1.12,0.77)$ & {\bf 4.5} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{10'}^{\rm NP})$ & $(-1.17,-0.35)$ & {\bf 4.5} \hspace{5mm} \\ + $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ & $(-1.15,0.34)$ & \!\!\!\!\!\!\!\!\!\!\! {\bf 4.7} \\ + $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=-\C{10'}^{\rm NP})$ & $(-1.06,0.06)$ & {\bf 4.4} \hspace{5mm} \\ + $(\C{9}^{\rm NP}=\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ & $(-0.64,-0.21)$ & 3.9 \hspace{5mm} \\ + $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=\C{10'}^{\rm NP})$ & $(-0.72,0.29)$ & 3.8 \hspace{5mm} \\ +% $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ & $(-0.66,0.03)$ & 2.0 & 23.0 + %$(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ & $(-0.69,0.05)$ & 1.9 & 22.0 \hspace{5mm} \\ + +\end{tabular} +\end{column} +\end{columns} + + +\medskip +\begin{itemize} +\item $C_9^{NP}$ always play a dominant role +\item All 2D scenarios above 4$\sigma$ are quite indistinguishable. + +\end{itemize} + + + +\end{minipage} + +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%% + + + +\begin{frame}{$B\to K^\ast \ell\ell\ $ Amplitudes} + +\small + +\mbox{ +\includegraphics[width=3cm,height=2cm]{bsg0.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2cm]{bsg1.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2.4cm]{bsg2.jpg} +} + +\vspace{3mm} + +\mbox{ +\hspace{-10mm} +\colorbox{llgray}{ +\hspace{1mm} +$\displaystyle +A_\lambda^{L,R} = N_\lambda\ \bigg\{ +(C_9 \mp C_{10}) {\blue \F_\lambda(q^2)} ++\frac{2m_b M_B}{q^2} \bigg[ C_7 {\blue \F_\lambda^{T}(q^2)} +- 16\pi^2 \frac{M_B}{m_b} {\red \H_\lambda(q^2)} \bigg] +\bigg\} +$ +\hspace{2mm} +} +} + +\vspace{5mm} +{\small + +\hspace{-8mm} \btr {\brown Local (Form Factors) :} \hspace{2mm} {\blue $ \F_\lambda^{(T)}(q^2) = \av{\bar M_\lambda(k)| \,\bar s\, \Gamma_\lambda^{(T)}\, b\, | \bar{ B}(k+q)}$} +\\[5mm] + +\mbox{ +\hspace{-9mm} +\btr {\brown Non-Local :} \hspace{0mm} {\red $\displaystyle \H_\lambda(q^2) = i \,{\cal P}_\mu^\lambda \int d^4 x\ e^{i q\cdot x}\, +\av{\bar{M}_\lambda(k)| +T\big\{ {\cal J}_{\rm em}^\mu(x), \C{i} \, \mathcal{O}(0) \big\} | \bar{B}(q+k)}$} +} + +\vspace{3mm} + +\hspace{-8mm} +\btr CKM structure : \hspace{2mm} $\displaystyle \H_\lambda = {\color{gray}- \frac{\lambda_u}{\lambda_t} \H_\lambda^{(u)}} - \frac{\lambda_c}{\lambda_t} \H_\lambda^{(c)}$ \hspace{5mm} $\Rightarrow\ \mathcal{O} \sim (\bar{ c} b)(\bar{ s} c)$ + +} + +\end{frame} + + + + + +\begin{frame}{Analytic structure of $\H_\lambda(q^2)$} + +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{3mm} + + +Neglecting OZI- and CKM-suppressed contributions : + +\begin{center} +\includegraphics[width=7.5cm]{Analyticq2.png} +\end{center} + + +$\displaystyle { \hat{\mathcal{H}}_\lambda(q^2)} = (q^2 - M_{J/\psi}^2)(q^2 -M_{\psi(2S)}^2) \,{ {\mathcal{H}}_\lambda(q^2)} \quad $ has no poles. + +\end{frame} + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} + +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{2mm} + +\btr Conformal mapping : \hspace{5mm} $q^2 \mapsto \ z\,(q^2) = \frac{\sqrt{t_+ - q^2} - \sqrt{t_+ - t_0}}{\sqrt{t_+ - q^2} + \sqrt{t_+ - t_0}}$ $t_0=t_+-\sqrt{t_+(t_+-M^2_{\psi(2S)} )}$ + +\mbox{ +\hspace{-10mm} +\raisebox{8mm}{\includegraphics[width=5.6cm]{Analyticq22.png}} +\hspace{1mm} +\includegraphics[width=6.5cm]{Analyticz.png} +} + +\vspace{-7mm} + +\btr ${\red \hat \H_\lambda (q^2(z))}$ is {\bf analytic in $|z|<1$}\\[3mm] + +\btr Taylor expand $\red \hat{\H}_\lambda(z)$ around $z=0$.\\[3mm] + +\btr Expansion needed for $|z| < 0.52\ $ ( $-7\,\GeV^2 \leq q^2 \leq 14 \GeV^2$ ) + + +\end{frame} + + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} + +\vspace{3mm} + + +\hspace{-5mm} {\bf \brown Some details for actual parametrisation :} + +\mbox{\hspace{-5mm} \btr Try to capture most features of the expansion (better convergence)} + +\mbox{\hspace{-5mm} \btr Parametrize the ratios $\H_\lambda(q^2)/\F_\lambda(q^2)$ instead} + +\mbox{\hspace{-5mm} \btr The poles should not modify the asymptotic behaviour at $|q^2|\to \infty$} + +\begin{eqnarray} +\H_\lambda(z) &=& +\frac{1-z\, z^*_{J/\psi}}{z-z_{J/\psi}} \frac{1-z\,z^*_{\psi(2S)}}{z-z_{\psi(2S)}} \ \hat\H_\lambda(z) +\nonumber\\[2mm] +% +\hat\H_\lambda(z) &=& \Big[ \sum_{k=0}^K \alpha_k^{(\lambda)} z^{k} \Big] \F_\lambda(z) +\nonumber +\end{eqnarray} + + +where $\alpha^{(\lambda)}_k$ are complex coefficients, and the expansion is truncated after the term $z^{K}$. +We will take $K=2$ ({\brown 16} real parameters). + + +\end{frame} + + + + +\begin{frame}{Experimental constraints on $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown Experimental constraints :} + +\mbox{\hspace{-5mm} \btr The residues of the poles are given by $B\to K^* \psi_n$ :} + +$$ +\H_\lambda(q^2 \to M_{\psi_n}^2) \sim +\frac{M_{\psi_n} f^{\,*}_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2 (q^2 - M_{\psi_n}^2)} + \cdots +$$ + +\mbox{\hspace{-5mm} \btr Angular analyses \Cite{Belle, Babar, LHCb} determine : } + +$$ +|r_\perp^{\psi_n}|,\, +|r_\|^{\psi_n}|,\, +|r_0^{\psi_n}|,\, +\arg\{r_\perp^{\psi_n} r_{0}^{\psi_n*}\},\, +\arg\{r_\|^{\psi_n} r_{0}^{\psi_n*}\}, +$$ + +where $\quad \displaystyle r_\lambda^{\psi_n} \equiv \operatorname*{Res}_{q^2\to M^2_{\psi_n}} \frac{\H_\lambda(q^2)}{\F_\lambda(q^2)} +\sim +\frac{M_{\psi_n} f^*_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2\, \F_\lambda(M_{\psi_n}^2)}$\\[3mm] + + +\mbox{\hspace{-5mm} \btr We produce correlated pseudo-observables from a fit (5+5).} + + + +\end{frame} + + + + +\begin{frame}{Prior Fit to $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown (Prior) Fit to Experimental and theoretical pseudo-observables :} + + + +\begin{table}[b] +% \resizebox{.85\textwidth}{!}{% +\centering +\renewcommand{\arraystretch}{1.5} +\renewcommand{\tabcolsep}{3.1mm} +\begin{tabular}{@{}crrr@{}} +\hline +$k$ & 0\hspace{7mm} & 1\hspace{7mm} & 2\hspace{7mm} \\ +\hline +%re perp +${\rm Re}[\alpha_{k}^{(\perp)}]$ & $-0.06 \pm 0.21$ & $-6.77 \pm 0.27$ & $18.96 \pm 0.59$ \\ +%re para +${\rm Re}[\alpha_{k}^{(\parallel)}]$ & $-0.35 \pm 0.62$ & $-3.13 \pm 0.41$ & $12.20 \pm 1.34$ \\ +%re long +${\rm Re}[\alpha_{k}^{(0)}]$ & $0.05 \pm 1.52$ & $17.26 \pm 1.64$ & -- \\ +%im perp +${\rm Im}[\alpha_{k}^{(\perp)}]$ & $-0.21 \pm 2.25$ & $1.17 \pm 3.58$ & $-0.08 \pm 2.24$ \\ +%im para +${\rm Im}[\alpha_{k}^{(\parallel)}]$ & $-0.04 \pm 3.67$ & $-2.14 \pm 2.46$ & $6.03 \pm 2.50$ \\ +%im long +${\rm Im}[\alpha_{k}^{(0)}]$ & $-0.05 \pm 4.99$ & $4.29 \pm 3.14$ & -- \\ +\hline +\end{tabular} +% } +\caption{Mean values and standard deviations (in units of $10^{-4}$) +of the prior PDF for the parameters $\alpha_k^{(\lambda)}$.} +\label{alphak} +\end{table} + +\end{frame} + +\begin{frame}{New Physics Analysis } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown SM predictions and Fit including $B\to K^* \mu^+\mu^-$ data and $\C{9}^{\rm NP}$ :}\\[4mm] + +\mbox{ +\hspace{-10mm} +\includegraphics[width=12cm]{NPFit.png} +} + +The NP hypothesis with {\red $\C{9}^{\bf NP}\sim -1$} is favored strongly in the global fit + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Quo Vadis Flavour Anomalies?} +{~} + \begin{minipage}{\textwidth} + +\begin{columns} +\column{0.5\textwidth} +\begin{exampleblock}{New Physics} +\ARROWR What kind of NP?\\ +\ARROWR Which anomalies will stand the test of time?\\ + +\end{exampleblock} + + + +\column{0.5\textwidth} +\begin{alertblock}{Standard Model} +Unlucky contingency: \\ +\ARROW QCD effects.\\ +\ARROW Fluctations. +\end{alertblock} + +\end{columns} +{~}\\ +\ARROW To know we need more data! +\pause +\begin{center} +\includegraphics[width=0.9\textwidth]{images/klucz.jpg} +\end{center} + + + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Conclusions} +{~} + \begin{minipage}{\textwidth} +\begin{itemize} +\item Clear tensions wrt. SM predictions! +\item Measurements cluster in the same direction. +\item We are not opening the champagne yet! +\item Still need improvement both on theory and experimental side. +\item Time will tell if this is QCD+fluctuations or new Physics: +\end{itemize} +\pause +''... when you have eliminated all the\\ +Standard Model explanations, whatever remains,\\ +however improbable, must be New Physics.''\\ +prof. Joaquim Matias + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +{~} + \begin{minipage}{\textwidth} +\begin{center} +\begin{LARGE} +Thank you for the attention! +\end{LARGE} +\includegraphics[width=0.8\textwidth]{images/Joke.jpg} + +\end{center} + + + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +\backupbegin + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Detector acceptance} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} + +\begin{columns} + +\column{0.6\textwidth} +\begin{itemize} +\item Detector distorts our angular distribution. +\item We need to model this effect. +\item 4D function is used: +\begin{align*} +\epsilon (\cos \thetal, \cos \thetak, \phi, q^2) = \\\sum_{ijkl} P_i(\cos \thetal) P_j(\cos \thetak ) P_k(\phi) P_l(q^2), +\end{align*} +where $P_i$ is the Legendre polynomial of order $i$. +\item We use up to $4^{th}, 5^{th}, 6^{th}, 5^{th}$ order for the $\cos \thetal, \cos \thetak, \phi, q^2$. +\item The coefficients were determined using Method of Moments, with a huge simulation sample. +\item The simulation was done assuming a flat phase space and reweighing the $q^2$ distribution to make is flat. +\item To make this work the $q^2$ distribution needs to be reweighted to be flat. +\end{itemize} +%\includegraphics[width=0.75\textwidth]{images/q2PHSP.png} + + + +\column{0.4\textwidth} +\only<1>{ + +\includegraphics[width=0.99\textwidth]{images/det.png} +} +\end{columns} + + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Control channel} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\begin{itemize} +\item We tested our unfolding procedure on $\PB \to \PJpsi \PKstar$. +\item The result is in perfect agreement with other experiments and our different analysis of this decay. +\end{itemize} +\end{footnotesize} +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{images/mlogjpsi.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{images/mkpijpsi.pdf}\\ +\includegraphics[width=0.99\textwidth]{images/angles3.png} +\end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + +\begin{frame}\frametitle{Backup} + + +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate selection} +{~} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\begin{footnotesize} +\item PID, kinematics and isolation variables used in a Boosted Decision Tree (BDT) to discriminate signal and background. +\item BDT with k-Folding technique. +\item Completely data driven. +\end{footnotesize} +\end{itemize} +\begin{center} +\includegraphics[width=0.70\textwidth]{images/Chopping_Distrib.pdf} +\end{center} + +\column{0.5\textwidth} + +\includegraphics[angle=-90,width=0.82\textwidth]{images/Fig1.pdf} \\ +\includegraphics[width=0.88\textwidth]{images/fold.png} + +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate selection, efficiency} +{~} + + \begin{minipage}{\textwidth} + \begin{footnotesize} + +\ARROW BDT was also checked in order not to bias our angular distribution: +\begin{center} +\includegraphics[angle=-90,width=0.8\textwidth]{images/BDT_Eff_Comp.pdf} +\end{center} +\ARROW The BDT has small impact on our angular observables. We will correct for these effects later on. + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +\begin{frame}{Amplitudes method} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + +\ARROW Fit for amplitudes as (continuous) functions of $q^2$ in the region: $q^2 \in \left[ 1.1. 6.0 \right]~\GeV^2/c^4$.\\ +\ARROW Needs some Ansatz: +\begin{align*} +A(q^2) = \alpha + \beta q^2+ \dfrac{\gamma}{q^2} +\end{align*} +\ARROW The assumption is tested extensively with toys.\\ +\ARROW Set of 3 complex parameters $ \alpha, \beta, \gamma $ per vector amplitude:\begin{itemize} +\item {\color{Magenta}{$L, ~R$}}, {\color{Cerulean}{$0 ,~\| ,~\bot$}}, {\color{PineGreen}{$\Re ,~\Im$}} $\rightarrowtail$~~ $3 \times {\color{PineGreen}{2}} \times {\color{Cerulean}{3}} \times {\color{Magenta}{2}} = 36$ DoF. +\item Scalar amplitudes: $+4$ DoF. +\item Symmetries of the amplitudes reduces the total budget to: $28$. +\end{itemize} +\ARROW The technique is described in \href{http://arxiv.org/pdf/1504.00574v2.pdf}{\color{blue}{JHEP06(2015)084}}.\\ +\ARROW Allows to build the observables as continuous functions of $q^2$: +\begin{itemize} +\item At current point the method is limited by statistics. +\item In the future the power of this method will increase. +\end{itemize} +\ARROW Allows to measure the zero-crossing points for free and with smaller errors than previous methods. +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Amplitudes - results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} +\begin{center} +\begin{columns} +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_AFBOverlay}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S4Overlay}.pdf} + +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S5Overlay}.pdf}\\ +{~}\\{~}\\{~}\\{~}\\ +\begin{large} +Zero crossing points: +\end{large} +\begin{align*} +q_0(S_4) & <2.65 & {\rm{~at~}} & 95\% ~CL \\ +q_0(S_5) & \in \left[ 2.49,3.95 \right] & {\rm{~at~}} & 68\% ~CL \\ +q_0(A_{FB}) & \in \left[ 3.40, 4.87 \right] & {\rm{~at~}} & 68\% ~CL +\end{align*} + + +\end{columns} +\end{center} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\backupend + +\end{document} diff --git a/Seminars/Bialasowka_2018/mchrzasz.toc b/Seminars/Bialasowka_2018/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Seminars/Bialasowka_2018/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Seminars/Bialasowka_2018/tikzfeynman.sty b/Seminars/Bialasowka_2018/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Seminars/Bialasowka_2018/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Seminars/FCAL/Makefile b/Seminars/FCAL/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Seminars/FCAL/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Seminars/FCAL/beamercolorthemeFlip.sty b/Seminars/FCAL/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Seminars/FCAL/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Seminars/FCAL/beamerinnerthemeFlip.sty b/Seminars/FCAL/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Seminars/FCAL/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Seminars/FCAL/beamerouterthemeFlip.sty b/Seminars/FCAL/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Seminars/FCAL/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Seminars/FCAL/beamerouterthemedecolines.sty b/Seminars/FCAL/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Seminars/FCAL/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Seminars/FCAL/beamerthemeFlip.sty b/Seminars/FCAL/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Seminars/FCAL/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Seminars/FCAL/distracted_ilissa-ocko-cartoon.jpg b/Seminars/FCAL/distracted_ilissa-ocko-cartoon.jpg new file mode 100644 index 0000000..5f007b0 --- /dev/null +++ b/Seminars/FCAL/distracted_ilissa-ocko-cartoon.jpg Binary files differ diff --git a/Seminars/FCAL/images/1.png b/Seminars/FCAL/images/1.png new file mode 100644 index 0000000..b1b3955 --- /dev/null +++ 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Font Trebuchet MS does not contain any OpenType `Script' information. +................................................. +LaTeX Info: Redefining \HepProcess on input line 2345. + +[63 + +] +Underfull \hbox (badness 2173) in paragraph at lines 2376--2376 +[]$\U/msa/m/n/9 V$[] \EU1/GilliusADF(0)/m/n/9 Fit for amplitudes as (continuous +) functions of $\OML/plm/m/it/9 q[]$ \EU1/GilliusADF(0)/m/n/9 in the region: $\ +OML/plm/m/it/9 q[] \OMS/plsy/m/n/9 2 + [] + + +Overfull \vbox (46.58122pt too high) detected at line 2376 + [] + +File: images/BG_lower.png Graphic file (type QTm) + +Overfull \vbox (19.18185pt too high) has occurred while \output is active [] + +................................................. +. fontspec info: "no-scripts" +. +. 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b/Seminars/FCAL/mchrzasz.tex new file mode 100644 index 0000000..1259a3f --- /dev/null +++ b/Seminars/FCAL/mchrzasz.tex @@ -0,0 +1,2415 @@ +\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} + +\usepackage[english]{babel} +\usepackage{polski} + + +\usetheme[ + bullet=circle, % Other option: square + bigpagenumber, % circled page number on lower right + topline=true, % colored bar at the top of the frame + shadow=false, % Shading for beamer blocks + watermark=BG_lower, % png file for the watermark + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +%\usepackage{emerald} +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\MeV}{\rm{MeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\re}{{\rm Re}} +\newcommand{\invfb}{\rm{fb^{-1}}} +\newcommand{\fixme}{\rm{{\color{red}{FIXME!}}}} +\newcommand{\thetal}{\theta_l} +\newcommand{\thetak}{\theta_k} +\newcommand{\nn}{\nonumber} +\newcommand{\eq}[1]{\begin{equation} #1 \end{equation}} +%\newcommand{\eqn}[1]{\begin{displaymath} #1 \end{displaymath}} +\newcommand{\eqa}[1]{\begin{eqnarray} #1 \end{eqnarray}} +\newcommand{\apeL}{{A_\perp^L}} +\newcommand{\apeR}{{A_\perp^R}} +\newcommand{\ape}{{A_\perp}} +\newcommand{\apeLR}{{A_\perp^{L,R}}} +\newcommand{\apaL}{{A_\|^L}} +\newcommand{\apaR}{{A_\|^R}} +\newcommand{\apa}{{A_\|}} +\newcommand{\apaLR}{{A_\|^{L,R}}} +\newcommand{\azeL}{{A_0^L}} +\newcommand{\azeR}{{A_0^R}} +\newcommand{\aze}{{A_0}} + +\newcommand{\azeLR}{{A_0^{L,R}}} +\newcommand{\Real}{\ensuremath{\mathcal{R}e}\xspace} +\newcommand{\Imag}{\ensuremath{\mathcal{I}m}\xspace} + +\renewcommand{\C}[1]{{\cal C}_{#1}} +\newcommand{\Ceff}[1]{{\cal C}^{\rm eff}_{#1}} +\newcommand{\Cpeff}[1]{{\cal C}^{\rm eff\prime}_{#1}} +\newcommand{\Cp}[1]{{\cal C}^{\prime}_{#1}} +\def\FL {\ensuremath{F_{\mathrm{L}}}\xspace} +\def\ATDPH {\ensuremath{A_{\mathrm{T,PR}}^{(2)}}\xspace} +\def\ATImPH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Im}}}\xspace} +\def\ATRePH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Re}}}\xspace} +\def\FLPH {\ensuremath{F_{\mathrm{L,PR}}}\xspace} +\def\ATDKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{(2)}}\xspace} +\def\ATImKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Im}}}\xspace} +\def\ATReKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Re}}}\xspace} +\def\FLKG {\ensuremath{F_{\mathrm{L,\Kstarz \gamma}}}\xspace} +\def\ATD {\ensuremath{A_{\mathrm{T}}^{(2)}}\xspace} +\def\ATIm {\ensuremath{A_{\mathrm{T}}^{\mathrm{Im}}}\xspace} +\def\ATRe {\ensuremath{A_{\mathrm{T}}^{\mathrm{Re}}}\xspace} +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} + + + +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + + + +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\mathcal{B}}} + +\newcommand{\av}[1]{\langle #1 \rangle} +% particles +\def\LstFTTT {\ensuremath{\PLambda^{*}(1520)^{0}}\xspace} +\def\dll {\ensuremath{\mathrm{DLL}}\xspace} + \def\Lb {\ensuremath{\PLambda_b}} + + +% useful decays +\def\BdToKpimm {\decay{\Bd}{\Kp\pim\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsToJPsiKst {\decay{\Bs}{\jpsi\Kstarz}} +\def\BdTopsitwosKst {\decay{\Bd}{\psitwos\Kstarz}} +\def\LstFTTTT {\decay{\LstFTTT}{p\Km}} +%\def\LbToLstmm {\decay{\Lb}{\PLambda^{*}(1520)^{0} \mumu}} +\def\LbTopKmm {\decay{\Lb}{p\Km\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsTophimm {\decay{\Bs}{\Pphi\mumu}} + +% interesting variables +\def\mkpi {\ensuremath{m_{K\pi}}\xspace} +\def\mkpimm{\ensuremath{m_{K\pi\mu\mu}}\xspace} + +%% peaking background mass hypotheses +\def\mkmm {\ensuremath{m_{K\mu\mu}}\xspace} +\def\mSwappKmm {\ensuremath{m_{(\pi\to p)K\mu\mu}}\xspace} +\def\mSwappiK {\ensuremath{m_{(\pi\to K)K}}\xspace} +\def\mSwappiKmm {\ensuremath{m_{(\pi\to K)K\mu\mu}}\xspace} +\def\mSwappK {\ensuremath{m_{(\pi\to p)K}}\xspace} +\def\mDoubleSwappKmm {\ensuremath{m_{(K\to p)(\pi\to K)\mu\mu}}\xspace} +\def\mDoubleSwappK {\ensuremath{m_{(K\to p)(\pi\to K)}}\xspace} +\def\mSwapKst {\ensuremath{m_{K\leftrightarrow\pi}}\xspace} + +%% some other decays +\def\BsToPhimm {\decay{\Bs}{\phi\mumu}} +\def\BsToPhimmFULL {\decay{\Bs}{\phi(\to\!K^{+}K^{-})\mumu}} +\def\BsToKKmm {\decay{\Bs}{\Kp\Km\mumu}} + +\newcommand{\delC}[1]{\delta {\cal C}_{#1}} +\newcommand{\dC}[1]{{\cal C}_{#1}^{\rm NP}} +\newcommand{\dCp}[1]{{\cal C}_{#1^\prime}^{\rm NP}} + + + + +\definecolor{green}{rgb}{0.2,0.6,0.2} +\definecolor{lightgreen}{rgb}{0.4,1,0.4} +\definecolor{verylightgreen}{rgb}{0.7,1,0.7} +\def\cgreen{\color{green}} +\definecolor{brown}{rgb}{0.4,0.2,0.0} +\def\cbrown{\color{brown}} +\def\cred{\color{red}} +\definecolor{darkblue}{rgb}{0.0,0.0,1.0} +\def\cdarkblue{\color{darkblue}} +\definecolor{darkgrey}{rgb}{0.4,0.4,0.4} +\definecolor{lightgrey}{rgb}{0.7,0.7,0.7} +\definecolor{verylightblue}{rgb}{0.8,0.8,1.0} +\definecolor{lightblue}{rgb}{0.6,0.6,1.0} +\definecolor{verylightyellow}{rgb}{1.0,1.0,0.5} +\definecolor{lightyellow}{rgb}{1.0,0.7,0.3} +\definecolor{darkred}{rgb}{0.6,0.0,0.0} + +\definecolor{green}{rgb}{0.3,0.6,0.2} +\definecolor{green}{rgb}{0.3,0.7,0.4} + + + +\definecolor{indigo}{RGB}{100,0,100} +\definecolor{dgray}{RGB}{80,80,80} +\definecolor{lgray}{RGB}{220,220,220} +\definecolor{dred}{RGB}{190,0,0} +\definecolor{dgreen}{RGB}{0,110,0} +\definecolor{lyellow}{RGB}{245,245,210} +\definecolor{bblue}{RGB}{93,93,255} +\definecolor{bbrown}{RGB}{150,85,52} +\definecolor{llgray}{RGB}{230,230,230} + + + +\newcommand{\F}{\mathcal{F}} +\newcommand{\A}{\mathcal{A}} +\newcommand{\N}{\mathcal{N}} +\renewcommand{\H}{\mathcal{H}} +\newcommand{\Leff}{\mathcal{L}_{\rm eff}} +\newcommand{\heff}{\mathcal{H}_{\rm eff}} +\newcommand{\Lag}{\mathcal{L}} +\newcommand{\red}{\color{red}} +\newcommand{\blue}{\color{blue}} +\newcommand{\indigo}{\color{indigo}} +\newcommand{\brown}{\color{bbrown}} +\newcommand{\bs}{\mathbf} +\newcommand{\sss}{\scriptscriptstyle} +\newcommand{\btr}{{ $\blacktriangleright\ $}} + + +\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (CERN, IFJ PAN)} +\institute{UZH} +\title[Anomalies in Physics]{Anomalies in Physics} +\date{25 September 2014} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.9\textwidth} + \flushright\fontspec{Trebuchet MS}\bfseries \Huge {Anomalies in Physics or Physics of anomalies?} + \end{column} + \begin{column}{0.2\textwidth} + %\includegraphics[width=\textwidth]{SHiP-2} + \end{column} + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} {\fontspec{Trebuchet MS} \Large Marcin Chrząszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=1.3cm]{cern}{~}{~} +\includegraphics[height=1.1cm]{ifj.png} +\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + \textcolor{normal text.fg!50!Comment}{IFJ FCAL workshop \\May 10, 2018} +\end{center} +\end{frame} +} + + +\begin{frame}{Outline} + + \begin{minipage}{\textwidth} +{~}\\ + +\begin{enumerate} +\item Why flavour is important. +\item The flavour anomalies: +\begin{itemize} +\item $R(\PDstar)$ +\item $R_K$ and $R_{\PKstar}$ +\item $P_5^{\prime}$ +\end{itemize} +\item Global fits results. +\item Conclusions. +\end{enumerate} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Why flavour physics +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +Why Flavour is important? +\end{Huge} +\end{center} + + + + +\end{frame} + + + +\begin{frame}{A lesson from history - GIM mechanism} + \begin{minipage}{\textwidth} + +\begin{center} +\includegraphics[width=0.62\textwidth]{images/GIM2.png} +\end{center} +\begin{columns} +\column{0.7\textwidth} +\begin{itemize} +\begin{footnotesize} + + +\item Cabibbo angle was successful in explaining dozens of decay rates in the 1960s. +\item There was, however, one that was not observed by experiments: $\PKzero \to \Pmuon \APmuon$. +\item Glashow, Iliopoulos, Maiani (GIM) mechanism was proposed in the 1970 to fix this problem. The mechanism required the existence of a $4^{th}$ quark. +\item At that point most of the people were skeptical about that. Fortunately in 1974 the discovery of the $\PJpsi$ meson silenced the skeptics. +\end{footnotesize} +\end{itemize} +\column{0.3\textwidth} +\begin{center} +\includegraphics[width=0.95\textwidth]{images/GIM3.png}\\ +\includegraphics[width=0.7\textwidth]{images/604.jpg}\\{~}\\{~} +\end{center} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + +\begin{frame}{A lesson from history - CKM matrix} + \begin{minipage}{\textwidth} + +\begin{center} +{~}\\{~}\\ +\includegraphics[width=0.5\textwidth]{images/CKMmatrix.png} + +\end{center} +\begin{columns} +\column{0.6\textwidth} +\begin{itemize} +\begin{small} + + + + +\item Similarly, CP violation was discovered in 1960s in the neutral kaons decays. +\item $2 \times 2$ Cabbibo matrix could not allow for any CP violation. +\item For CP violation to be possible one needs at least a $3 \times 3$ unitary matrix \\ $\looparrowright$ Cabibbo-Kobayashi-Maskawa matrix (1973). +\item It predicts existence of $\Pbottom$ (1977) and $\Ptop$ (1995) quarks. +\end{small} + +\end{itemize} +\column{0.4\textwidth} +\begin{center} +{~} +%\includegraphics[height=2cm]{images/CP.png}\\ +\includegraphics[width=0.96\textwidth]{bottom.jpg} + +\end{center} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{A lesson from history - Weak neutral current} + \begin{minipage}{\textwidth} + +\begin{center} +\includegraphics[height=3cm]{images/weakcurr.png}{~} +\includegraphics[height=3cm]{images/weakcurr2.png} +\end{center} + +\begin{columns} +\column{0.6\textwidth} +\begin{itemize} +\begin{small} + + +\item Weak neutral currents were first introduced in 1958 by Buldman. +\item Later on they were naturally incorporated into unification of weak and electromagnetic interactions. +\item 't Hooft proved that the GWS models was renormalizable. +\item Everything was there on theory side, only missing piece was the experiment, till 1973. +\end{small} + +\end{itemize} +\column{0.4\textwidth} +\begin{center} +{~} +%\includegraphics[height=2cm]{images/CP.png}\\ +\includegraphics[width=0.85\textwidth]{images/bubblecern.png} +\end{center} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + + + +\iffalse + + + +\begin{frame} +\begin{center} +\begin{Huge} +LHCb detector +\end{Huge} +\end{center} + + + + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% DETECTOR +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\only<1>{\frametitle{LHCb detector - tracking} +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/sketch.png} +\end{columns} +\begin{itemize} +\item Excellent Impact Parameter (IP) resolution ($20~\rm \mu m$).\\ +$\Rightarrow$ Identify secondary vertices from heavy flavour decays +\item Proper time resolution $\sim~40~\rm fs$.\\ +$\Rightarrow$ Good separation of primary and secondary vertices. +\item Excellent momentum ($\delta p/p \sim 0.4 - 0.6\%$) and inv. mass resolution.\\ +$\Rightarrow$ Low combinatorial background. + +\end{itemize} + + +} + +\only<2>{\frametitle{LHCb detector - particle identification} +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/cher.png} +\end{columns} +\begin{itemize} +\item Excellent Muon identification $\epsilon_{\mu \to \mu} \sim 97\%$, $\epsilon_{\pi \to \mu} \sim 1-3\%$ +\item Good $\PK-\Ppi$ separation via RICH detectors, $\epsilon_{\PK \to \PK} \sim 95\%$, $\epsilon_{\Ppi \to \PK} \sim 5\%$.\\ +$\Rightarrow$ Reject peaking backgrounds. +\item High trigger efficiencies, low momentum thresholds. +Muons: $p_T > 1.76 \GeV$ at L0, $p_T > 1.0 \GeV$ at HLT1,\\ +$B \to \PJpsi X $: Trigger $\sim 90\%$. + +\end{itemize} + + +} + + +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Modern challenges: loops come in to the game} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\item Standard Model contributions suppressed or absent: +\begin{itemize} +\item Flavour Changing Neutral Currents. +\item CP violation +\item Lepton Flavour/Number or Lepton Universality violation. +\end{itemize} +\item In general can probe physics beyond General Purpose Detectors reach. +\end{itemize} +\column{0.5\textwidth} +\includegraphics[width=0.99\textwidth]{{images/TauLFV_UL_2014001_averaged}.png} + + +\end{columns} +\begin{center} +\includegraphics[width=0.75\textwidth]{images/Bsmumu.png} +\includegraphics[width=0.20\textwidth]{{images/bsmumu_SM}.png} +\end{center} +\end{minipage} + + \vspace*{2.1cm} +\end{frame} +\fi + + + + + +\begin{frame}\frametitle{Modern Flavour Physics} +\begin{center} +\only<1>{ +\includegraphics[width=1.05\textwidth]{1.png} +} +\only<2>{ +\includegraphics[width=1.05\textwidth]{2.png} + +} +\end{center} + + + + +\end{frame} + + +\begin{frame}\frametitle{Why semi-leptonic decays?} +\begin{large} +\ARROW A decay is semi-leptonic if its products are part leptons +and part hadrons. +\end{large} + +\begin{center} +\includegraphics[width=0.99\textwidth]{3.png} +\end{center} + +\begin{large} +\ARROW These decays can be factorised into the weak and +strong parts, greatly simplifying theoretical calculations. +\end{large} + + +\end{frame} + + + +\begin{frame}\frametitle{Types of semi-leptonic decays} + +\begin{center} +\includegraphics[width=1.05\textwidth]{4.png} +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Anomalies} +\only<1>{ +\begin{center} +\includegraphics[width=1.05\textwidth]{6.png} +\end{center} +} +\only<2>{ +\ARROW Today I will talk about three anomalies in $\PB$ +decays: +\begin{itemize} +\item $R(\PDstar)$ +\item $R_{\PK/\PKstar}$ +\item $P^{\prime}_5$ +\end{itemize} + +} + +\end{frame} + + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 1\\ +\begin{align*} +R(\PDstar) = \frac{\Br (\PB \to \PDstar \tau \nu )}{\Br(\PB \to \PDstar \mu \nu)} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{$R(\PDstar) $} + +\begin{large} + +\ARROW Large rate of charged current decays allow for measurement +in semi-tauonic decays +\end{large} + +\begin{columns} +\column{0.5\textwidth} +\begin{align*} +R(\PDstar) = \frac{\Br (\PB \to \PDstar \tau \nu )}{\Br(\PB \to \PDstar \mu \nu)} +\end{align*} +\column{0.5\textwidth} +\begin{large} +\ARROW Form ratio of decays with different lepton generations.\\ +\ARROW Cancel QCD uncertainties. +\end{large} + +\end{columns} +~\\ +\begin{large} + +\ARROW $R(\PDstar)$ is sensitive to the NP with strong 3rd generation couplings. +\end{large} + +\includegraphics[width=0.8\textwidth]{images/7.png} + + +\end{frame} + +\begin{frame}\frametitle{The Rule of three} + +\begin{center} + +\includegraphics[width=1.\textwidth]{images/8.png} + +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Experimental challenges} +\begin{large} +\ARROW With the $\tau \to \mu \nu \nu$ decay we are missing 3 neutrinos!\\ +\ARROW No sharp peak in any distributions.\\ +\end{large} +{~}\\ +\begin{columns} +\column{0.5\textwidth} +\begin{large} +\ARROW At B-factories, can control this +using tagging technique.\\ +\end{large} + + +\includegraphics[width=0.9\textwidth]{9.png} + +\column{0.5\textwidth} + + +\includegraphics[width=0.9\textwidth]{10.png}\\ +\begin{large} +\ARROW More difficult at LHCb, compensate +using large boost (flight information) +and huge B production\\ +\end{large} +\end{columns} + +\end{frame} + +\begin{frame}\frametitle{Signal fits} +\ARROW Three main backgrounds: +\begin{itemize} +\item $\PB \to \PDstar \ell \nu$. +\item $\PB \to \PD^{\ast \ast} \ell \nu$. +\item $\PB \to \PD \PDstar X$ +\end{itemize} +\begin{center} +\includegraphics[width=0.9\textwidth]{12.png} +\end{center} +\ARROW Fit variables which discriminate between the signal and background modes. + +\end{frame} + +\begin{frame}\frametitle{Results} +\ARROW All experiments see an access w.r.t. to SM prediction: +\begin{center} +\includegraphics[angle=-90,width=0.5\textwidth]{rdrds_fpcp2017.pdf} +\end{center} +\ARROW Theoretical uncertainties negligible.\\ +\ARROW The ball is on the experimental side. + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + + +\begin{frame}\frametitle{Introduction to anomaly 2 \& 3} + +\begin{columns} +\column{4in} +\begin{itemize} +\item The SM allows only the charged interactions to change flavour. +\begin{itemize} +\item Other interactions are flavour conserving. +\end{itemize} +\item One can escape this constraint and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. +\begin{itemize} +\item These kind of processes are suppressed in SM $\to$~Rare decays. +\item New Physics can enter in the loops. +\end{itemize} +\end{itemize} +\begin{center} +\includegraphics[scale=0.3]{lupa.png} +\includegraphics[scale=0.3]{example.png} +\end{center} +\column{1.5in} +\includegraphics[width=0.61\textwidth]{couplings.png} +\end{columns} + +\end{frame} + + +\begin{frame}{Analysis of Rare decays} +\begin{footnotesize} + +%{\Large Since a long time ago...} \\ \medskip +%\hspace*{1.4cm}$\Rightarrow$ $b \to s \gamma$ and $b \to s \ell\ell $ {\bf Flavour Changing Neutral Currents} have been used as {\bf \cred Our Portal} \\ to explore the fundamental theory beyond SM. \\ +%\medskip +%\medskip +%\hfill....... with not much success till 2013.\hspace*{1cm} +%\bigskip + +Analysis of FCNC in a model-independent approach, effective Hamiltonian: +\vspace*{-0.1cm} +\begin{columns} +\begin{column}{1cm} +~ +\end{column} +\begin{column}{8cm} +\begin{equation*} +b\to s\gamma(^*): {\mathcal H}^{SM}_{\Delta F=1} \propto + \sum_{i=1}^{10} V_{ts}^* V_{tb} {\cgreen \C{i}} \alert{ {\cal O}_i} + \ldots +\end{equation*} + +\vspace{-0.2cm} + +\begin{itemize} +\item $\alert{ {\cal O}_7} = \frac{e}{16 \pi^2}m_b\, + (\bar s\sigma^{\mu\nu} P_R b) F_{\mu\nu}\,$ %\quad [real or soft photon] +\item $\alert{ {\cal O}_9}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b)\ (\bar\ell\gamma_\mu\ell)$ + %\quad [$b\to s\mu\mu$ via $Z$/hard $\gamma$] +\item $\alert{ {\cal O}_{10}}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b) \ (\bar\ell\gamma_\mu\gamma_5\ell)$, ... +%\quad [$b\to s\mu\mu$ via $Z$] +\end{itemize} +\end{column} +\begin{column}{5.5cm} +\includegraphics[width=3.5cm]{images/qum1.png} +%\includegraphics[width=3cm]{bsll.pdf} +\end{column} +\end{columns} + +%\hspace*{5cm} with no clear success yet... +%\bigskip + + +%\centerline{{\bf Goal}: \underline{Decode the short distance physics to find a smoking gun of BSM}\hspace*{2cm}} + + +\bigskip +\hspace*{0.0cm} $\bullet$ {\bf SM} Wilson coefficients up to NNLO + e.m. corrections at $\mu_{ref}=4.8$ GeV [{\cgreen Misiak et al.}]: $${\cal C}_7^{\rm SM}=-0.29,\, {\cal C}_9^{\rm SM}=4.1,\, {\cal C}_{10}^{\rm SM}=-4.3$$ +%BUT, like in the film there is always the good, the bad and the ugly. +\bigskip +$\bullet$ {\bf NP} changes short distance ${\cal C}_i-{\cal C}_i^{\rm SM}={\cal C}_i^{\rm NP}$ and induce new operators, like ${\cal O}^\prime_{7,9,10}={\cal O}_{7,9,10}\,\, (P_L \leftrightarrow P_R)$ ... also scalars, pseudoescalar, tensor operators...%\bigskip + + +\end{footnotesize} + +\end{frame} + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 2\\ +\begin{align*} +R_{\PK/\PKstar} = \frac{\Br(\PB \to \PK/\PKstar \mu \mu)}{\Br(\PB \to \PK/\PKstar e e)} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + + + +\begin{frame}\frametitle{Measurement at LHCb} + +\ARROW Most precise measurements performed at LHCb.\\ +\ARROW Main challenge is due to electron Bremsstrahlung.\\ +\begin{center} +\includegraphics[width=0.99\textwidth]{13.png} +\end{center} +\ARROW To protect ourself from electron reconstruction issue we use double ratio: +\begin{align*} +R_K = \frac{ \Br(\PB \to \PK \mu \mu ) \times \Br(\PB \to \PK \PJpsi(\to e e)) }{ \Br(\PB \to \PK e e ) \times \Br(\PB \to \PK \PJpsi(\to \mu \mu)) } +\end{align*} + + +\end{frame} + + +\begin{frame}\frametitle{Result} + +\begin{center} +\begin{large} +\begin{align*} +R_K = 0.745^{+0.090}_{-0.074} ({\rm stat.}) \pm 0.036 ({\rm syst}) +\end{align*} +\end{large} + +\includegraphics[width=0.7\textwidth]{images/RK.png}\\ + +\end{center} +\ARROW $2.6~\sigma$ away from SM prediction. +\end{frame} + +\begin{frame}\frametitle{The continuation - $R_{\PKstar}$} +\ARROW The neutral continuation of the $R_K$ measurement is to measure its partner: +\begin{center} +\begin{align*} +R_{\PKstar} = \frac{\Br(\PB \to \PKstar \mu \mu)}{\Br(\PB \to \PKstar e e)} +\end{align*} +\end{center} + + +\begin{columns} +\column{0.4\textwidth} +\ARROW Measurement performed in two $q^2$ bins. \\ +\ARROW Normalized in double ratio to $\PB \to \PKstar \PJpsi$.\\ +\includegraphics[width=0.95\textwidth]{images/plot.png} + + +\column{0.6\textwidth} +\begin{center} +\includegraphics[width=0.95\textwidth]{Fig10a.pdf} +\end{center} + +\end{columns} + + + +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PB \to \PKstar^{\pm} \Pmu \Pmu$} +{~} +\includegraphics[width=0.5\textwidth]{images/ksmumu_BF.png} +\includegraphics[width=0.5\textwidth]{images/kmumu_BF.png} + +\begin{center} +\begin{columns} + +\column{0.4\textwidth} +\begin{itemize} +\item Despite large theoretical errors the results are consistently smaller than SM prediction. +\end{itemize} +\column{0.6\textwidth} +\includegraphics[width=0.87\textwidth]{images/bukst_BF.png} + + +\end{columns} + + + + + + + +\end{center} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PBs \to \Pphi \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[width=0.65\textwidth]{images/bs2phipi.png}\\ + \end{center} + +\begin{itemize} +\item Recent LHCb measurement [JHEPP09 (2015) 179]. +\item Suppressed by $\frac{f_s}{f_d}$. +\item Cleaner because of narrow $\Pphi$ resonance. +\item $3.3~\sigma$ deviation in SM in the $1-6\GeV^2$ bin. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + + + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 3\\ +\begin{align*} +P_5^{\prime} = \sqrt{2} \frac{\Re (\apeL \apaL^{\ast} - \apeR \apaR^{\ast} )}{\sqrt{ |\aze|^2 ( |\ape|^2 + |\aze|^2 )}} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + + +%\azeLR +%\apaLR +%\apeLR + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{$\PBzero \to \PKstar \Pmuon \APmuon$ kinematics} +{~} + \begin{minipage}{\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ The kinematics of $\PBzero \to \PKstar \Pmuon \APmuon$ decay is described by three angles $\thetal$, $\thetak$, $\phi$ and invariant mass of the dimuon system ($q^2)$. + + \only<1>{ +\begin{columns} +\column{0.5\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ $\cos \thetak$: the angle between the direction of the kaon in the $\PKstar$ ($\overline{\PKstar}$) rest frame and the direction of the $\PKstar$ ($\overline{\PKstar}$) in the $\PBzero$ ($\APBzero$) rest frame.\\ +$\color{JungleGreen}{\Rrightarrow}$ $\cos \thetal$: the angle between the direction of the $\Pmuon$ ($\APmuon$) in the dimuon rest frame and the direction of the dimuon in the $\PBzero$ ($\APBzero$) rest frame.\\ +$\color{JungleGreen}{\Rrightarrow}$ $\phi$: the angle between the plane containing the $\Pmuon$ and $\APmuon$ and the plane containing the kaon and pion from the $\PKstar$. + + + +\column{0.5\textwidth} +\includegraphics[width=0.95\textwidth]{images/angles.png} + +\end{columns} + } + \only<2>{ +{\tiny{ +\eqa{\label{dist} +\frac{d^4\Gamma}{dq^2\,d\!\cos\theta_K\,d\!\cos\theta_l\,d\phi}&=&\frac9{32\pi} \bigg[ +J_{1s} \sin^2\theta_K + J_{1c} \cos^2\theta_K + (J_{2s} \sin^2\theta_K + J_{2c} \cos^2\theta_K) \cos 2\theta_l\nn\\[1.5mm] +&&\hspace{-2.7cm}+ J_3 \sin^2\theta_K \sin^2\theta_l \cos 2\phi + J_4 \sin 2\theta_K \sin 2\theta_l \cos\phi + J_5 \sin 2\theta_K \sin\theta_l \cos\phi \nn\\[1.5mm] +&&\hspace{-2.7cm}+ (J_{6s} \sin^2\theta_K + {J_{6c} \cos^2\theta_K}) \cos\theta_l ++ J_7 \sin 2\theta_K \sin\theta_l \sin\phi + J_8 \sin 2\theta_K \sin 2\theta_l \sin\phi \nn\\[1.5mm] +&&\hspace{-2.7cm}+ J_9 \sin^2\theta_K \sin^2\theta_l \sin 2\phi \bigg]\,, +\nonumber} +}} +$\color{JungleGreen}{\Rrightarrow}$ This is the most general expression of this kind of decay. + +} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Transversity amplitudes } +{~} + \begin{minipage}{\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ One can link the angular observables to transversity amplitudes +{\tiny{ +\eqa{ +J_{1s} & = & \frac{(2+\beta_\ell^2)}{4} \left[|\apeL|^2 + |\apaL|^2 +|\apeR|^2 + |\apaR|^2 \right] + + \frac{4 m_\ell^2}{q^2} \re\left(\apeL\apeR^* + \apaL\apaR^*\right)\,,\nn\\[1mm] +% +J_{1c} & = & |\azeL|^2 +|\azeR|^2 + \frac{4m_\ell^2}{q^2} \left[|A_t|^2 + 2\re(\azeL^{}\azeR^*) \right] + \beta_\ell^2\, |A_S|^2 \,,\nn\\[1mm] +% +J_{2s} & = & \frac{ \beta_\ell^2}{4}\left[ |\apeL|^2+ |\apaL|^2 + |\apeR|^2+ |\apaR|^2\right], +\hspace{0.92cm} J_{2c} = - \beta_\ell^2\left[|\azeL|^2 + |\azeR|^2 \right]\,,\nn\\[1mm] +% +J_3 & = & \frac{1}{2}\beta_\ell^2\left[ |\apeL|^2 - |\apaL|^2 + |\apeR|^2 - |\apaR|^2\right], +\qquad J_4 = \frac{1}{\sqrt{2}}\beta_\ell^2\left[\re (\azeL\apaL^* + \azeR\apaR^* )\right],\nn \\[1mm] +% +J_5 & = & \sqrt{2}\beta_\ell\,\Big[\re(\azeL\apeL^* - \azeR\apeR^* ) - \frac{m_\ell}{\sqrt{q^2}}\, +\re(\apaL A_S^*+ \apaR^* A_S) \Big]\,,\nn\\[1mm] +% +J_{6s} & = & 2\beta_\ell\left[\re (\apaL\apeL^* - \apaR\apeR^*) \right]\,, +\hspace{2.25cm} J_{6c} = 4\beta_\ell\, \frac{m_\ell}{\sqrt{q^2}}\, \re (\azeL A_S^*+ \azeR^* A_S)\,,\nn\\[1mm] +% +J_7 & = & \sqrt{2} \beta_\ell\, \Big[\im (\azeL\apaL^* - \azeR\apaR^* ) + +\frac{m_\ell}{\sqrt{q^2}}\, \im (\apeL A_S^* - \apeR^* A_S)) \Big]\,,\nn\\[1mm] +% +J_8 & = & \frac{1}{\sqrt{2}}\beta_\ell^2\left[\im(\azeL\apeL^* + \azeR\apeR^*)\right]\,, +% +\hspace{1.9cm} J_9 = \beta_\ell^2\left[\im (\apaL^{*}\apeL + \apaR^{*}\apeR)\right] \,, +\label{Js}\nonumber} +}} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Link to effective operators} +{~} + \begin{minipage}{\textwidth} +$\color{JungleGreen}{\Rrightarrow}$ So here is where the magic happens. At leading order the amplitudes can be written as: +{\tiny{ +\eqa{ +\apeLR &=&\sqrt{2} N m_B(1- \hat s)\bigg[ (\Ceff9 + \Cpeff9) \mp (\C{10} + \Cp{10}) ++\frac{2\hat{m}_b}{\hat s} (\Ceff7 + \Cpeff7) \bigg]\xi_{\bot}(E_{K^*}) \nn \\[2mm] +\apaLR &=& -\sqrt{2} N m_B (1-\hat s)\bigg[(\Ceff9 - \Cpeff9) \mp (\C{10} - \Cp{10}) ++\frac{2\hat{m}_b}{\hat s}(\Ceff7 - \Cpeff7) \bigg] \xi_{\bot}(E_{K^*}) \nn \\[2mm] +\azeLR &=& -\frac{N m_B (1-\hat s)^2}{2 \hat{m}_{K^*} \sqrt{\hat s}} \bigg[ (\Ceff9 - \Cpeff9) \mp (\C{10} - \Cp{10}) + 2\hat{m}_b (\Ceff7 - \Cpeff7) \bigg]\xi_{\|}(E_{K^*}), +\label{LargeRecoilAs}\nonumber} +}} +where $\hat s = q^2 /m_B^2$, $\hat{m}_i = m_i/m_B$. The $\xi_{\|,\bot }$ are the form factors. \\ +\pause +$\color{JungleGreen}{\Rrightarrow}$ Now we can construct observables that cancel the $\xi$ form factors at leading order: +\eq{P_5^{\prime} = \dfrac{J_5+\bar{J}_5}{2\sqrt{-(J_2^c+\bar{J}_2^c)(J_2^s+\bar{J}_2^s)} }\nonumber +} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +LHCb measurement of $\PBd \to \PKstar \Pmu \Pmu$ +\end{Huge} +\end{center} + + + + +\end{frame} +\iffalse + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{LHCbs $\PBzero \to \PKstar \Pmuon \APmuon$, Selection} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\begin{columns} +\column{0.2in} +{~} +\column{2in} +\ARROW Trigger +\begin{itemize} +\item Muon trigger. +\item Topological trigger. +\end{itemize} +\ARROW Good modelling with MC. \\ +\ARROW Selection: +\begin{itemize} +\item As loose as possible. +\item Based on the $\PBzero$ vertex quality, impact parameters, loose Particle identification for the hadrons. +\item The variables were chosen in a way we are sure the are correctly modelled in MC. +\end{itemize} +\column{2.8in} + +\includegraphics[angle=-90,width=0.75\textwidth]{{images/tistos_L0Muon_pt}.pdf}\\ +\includegraphics[angle=-90,width=0.75\textwidth]{{images/tistos_L0Muon_costhetal}.pdf} +\end{columns} + + + +\end{footnotesize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Peaking backgrounds} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\ARROW A number of peaking backgrounds that can mistaken as your signal.\\ +\ARROW There where a specially designed vetoes to fight each of them. +\begin{center} +\begin{tiny} +\hspace{-1cm}\begin{tabular}{ r | c c | c c } + \hline + & \multicolumn{2}{c|}{after preselection, before vetoes} & \multicolumn{2}{c }{after vetoes and selection}\\ + Channel & Estimated events & \% signal & Estimated events & \% signal \\ + \hline + \hline + $\PLambda_b \to \PLambda^{\ast}(1520)^{0} \mu\mu$ &$ (1.0\pm0.5)\times10^3 $&$ 19\pm8 $&$ 51\pm25 $&$ 1.0\pm0.4$\\ + $\PLambda_b \to {\rm p } \PK \mu\mu$ &$ (1.0\pm0.5)\times10^2 $&$ 1.9\pm0.8 $&$ 5.7\pm2.8 $&$ 0.11\pm0.05$ \\ + $\PBd \to \PKplus \mu \mu$ &$ 28\pm7 $&$ 0.55\pm0.06 $&$ 1.6\pm0.5 $&$ 0.031\pm0.006$\\ +$\PBs \to \Pphi \mu \mu$ &$ (3.2\pm1.3)\times10^2 $&$ 6.2\pm2.1 $&$ 17\pm7 $&$ 0.33\pm0.12$\\ +signal swaps &$ (3.6\pm0.9)\times10^2 $&$ 6.9\pm0.6 $&$ 33\pm9 $&$ 0.64\pm0.06$ \\ +$\PBd \to \PKstar \PJpsi$ swaps &$ (1.3\pm0.4)\times10^2 $&$ 2.6\pm0.4 $&$ 2.7\pm2.8 $&$ 0.05\pm0.05$ \\ + + \hline + \end{tabular} +\end{tiny} +\includegraphics[angle=-90,width=0.49\textwidth]{{images/h_Bd_Kstmm_vetoes}.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{{h_Lb_L1520mm_vetoes}.pdf} + +\end{center} + + + + +\end{footnotesize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +\fi + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate simulation} +{~} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\begin{footnotesize} +\item PID, kinematics and isolation variables used in a Boosted Decision Tree (BDT) to discriminate signal and background. +\item BDT with k-Folding technique. +\item Completely data driven. +\end{footnotesize} +\end{itemize} +\begin{center} +\includegraphics[width=0.70\textwidth]{images/Chopping_Distrib.pdf} +\end{center} + +\column{0.5\textwidth} + +\includegraphics[angle=-90,width=0.82\textwidth]{images/Fig1.pdf} \\ +\includegraphics[width=0.88\textwidth]{images/fold.png} + +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate simulation, efficiency} +{~} + + \begin{minipage}{\textwidth} + \begin{footnotesize} + +\ARROW BDT was also checked in order not to bias our angular distribution: +\begin{center} +\includegraphics[angle=-90,width=0.8\textwidth]{images/BDT_Eff_Comp.pdf} +\end{center} +\ARROW The BDT has small impact on our angular observables. We will correct for these effects later on. + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\iffalse + +\begin{frame}{Mass modelling} +{~} +\begin{minipage}{\textwidth} +\begin{tiny} +\begin{columns} +\column{0.1in} +{~} +\column{2.5in} +\ARROW The signal is modelled by a sum of two Crystal-Ball functions with common mean.\\ +\ARROW The background is a single exponential.\\ +\ARROW The base parameters are obtained from the proxy channel: $\PBd \to \PJpsi (\mu\mu) \PKstar$.\\ +\ARROW All the parameters are fixed in the signal pdf.\\ +\ARROW Scaling factors for resolution are determined from MC.\\ +\ARROW In fitting the rare mode only the signal, background yield and the slope of the exponential is left floating.\\ +\begin{center} +\includegraphics[angle=-90,width=0.9\textwidth]{images/msignal.pdf}\\ + +\end{center} +\ARROW We found $624\pm30$ candidates in the most interesting $\left[1.1,6.0\right]~\GeV^2/c^4$ region \\ and $2398 \pm 57$ in the full range $\left[ 1.1, 19.\right]~\GeV^2/c^4$. +\column{2.5in} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/FitJpsiKstar_withBDT_withoutPartially}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/Scaling_factor}.pdf}\\ +\ARROW The S-wave fraction is extracted using a \texttt{LASS} model. +\end{columns} + +\end{tiny} +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Monte Carlo corrections} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\ARROW No Monte Carlo simulation is perfect! One needs to correct for remaining differences.\\ +\ARROW We reweighted our $\PBd \to \PKstar \mu \mu$ Monte Carlo accordingly to differences between the $\PBd \to \PKstar \PJpsi$ in data (Splot) and Monte Carlo. +\only<1>{ +\begin{center} +\includegraphics[angle=-90,width=0.38\textwidth]{images/pt.pdf} +\includegraphics[angle=-90,width=0.38\textwidth]{images/vertex.pdf}\\ +\includegraphics[angle=-90,width=0.38\textwidth]{images/nTracks.pdf} +\end{center} +} +\only<2>{ +\begin{center} +\includegraphics[angle=-90,width=0.38\textwidth]{images/eta_logy.pdf} +\includegraphics[angle=-90,width=0.38\textwidth]{images/B0_p.pdf} \\ +\includegraphics[angle=-90,width=0.38\textwidth]{{images/bdt_data_mc_nominalMkpi}.pdf} +\end{center} +} + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +\fi + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Detector acceptance} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} + +\begin{columns} + +\column{0.6\textwidth} +\begin{itemize} +\item Detector distorts our angular distribution. +\item We need to model this effect. +\item 4D function is used: +\begin{align*} +\epsilon (\cos \thetal, \cos \thetak, \phi, q^2) = \\\sum_{ijkl} P_i(\cos \thetal) P_j(\cos \thetak ) P_k(\phi) P_l(q^2), +\end{align*} +where $P_i$ is the Legendre polynomial of order $i$. +\item We use up to $4^{th}, 5^{th}, 6^{th}, 5^{th}$ order for the $\cos \thetal, \cos \thetak, \phi, q^2$. +\item The coefficients were determined using Method of Moments, with a huge simulation sample. +\item The simulation was done assuming a flat phase space and reweighing the $q^2$ distribution to make is flat. +\item To make this work the $q^2$ distribution needs to be reweighted to be flat. +\end{itemize} +%\includegraphics[width=0.75\textwidth]{images/q2PHSP.png} + + + +\column{0.4\textwidth} +\only<1>{ + +\includegraphics[width=0.99\textwidth]{images/det.png} +} +\end{columns} + + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Control channel} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\begin{itemize} +\item We tested our unfolding procedure on $\PB \to \PJpsi \PKstar$. +\item The result is in perfect agreement with other experiments and our different analysis of this decay. +\end{itemize} +\end{footnotesize} +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{images/mlogjpsi.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{images/mkpijpsi.pdf}\\ +\includegraphics[width=0.99\textwidth]{images/angles3.png} +\end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{The columns of New Physics} +{~} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[width=0.94\textwidth]{images/columns.png} + + \end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{The columns of New Physics} +{~} + \begin{minipage}{\textwidth} +\begin{enumerate} +\item Maximum likelihood fit: +\begin{itemize} +\item The most standard way of obtaining the parameters. +\item Suffers from convergence problems, under coverages, etc. in low statistics. +\end{itemize} +\item Method of moments: +\begin{itemize} +\item Less precise then the likelihood estimator ($10-15\%$ larger uncertainties). +\item Does not suffer from the problems of likelihood fit. +\end{itemize} +\item Amplitude fit: +\begin{itemize} +\item Incorporates all the physical symmetries inside the amplitudes! The most precise estimator. +\item Has theoretical assumptions inside! +\end{itemize} +\end{enumerate} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} +{~} +\begin{footnotesize} + + \begin{minipage}{\textwidth} +\ARROW In the maximum likelihood fit one could weight the events accordingly to the $\dfrac{1}{\varepsilon(\cos \thetal, \cos \thetak, \phi, q^2)}$\\ +\ARROW Better alternative is to put the efficiency into the maximum likelihood fit itself: +\begin{align*} +\mathcal{L}=\prod_{i=1}^N \epsilon_i(\Omega_i, q_i^2) \mathcal{P}(\Omega_i, q_i^2) / \int \epsilon(\Omega, q^2) \mathcal{P}(\Omega, q^2) d\Omega dq^2 +\end{align*} +\ARROW Only the relative weights matters!\\ +\ARROW The Procedure was commissioned with TOY MC study.\\ +\ARROW Use Feldmann-Cousins to determine the uncertainties. \\ +\ARROW Angular background component is modelled with $2^{\rm nd }$ order Chebyshev polynomials, which was tested on the side-bands.\\ +\ARROW S-wave component treated as nuisance parameter.\\ +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_Afb3}.pdf} +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_P11}.pdf} +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_P57}.pdf} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} +\iffalse +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} +{~} + \begin{minipage}{\textwidth} +\begin{center} +\only<1>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/FLPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S3Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/S4Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S5Pad.pdf} +} +\only<2>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/AFBPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S7Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/S8Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S9Pad.pdf} +} + + +\end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[angle=-90,width=0.65\textwidth]{images/P5pPadOverlay.pdf}\\ + \end{center} + +\begin{itemize} +\item Tension with $3~\invfb$ gets confirmed! +\item two bins both deviate by $2.8~\sigma$ from SM prediction. +\item Result compatible with previous result. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +\fi + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Method of moments} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} +\ARROW See {\color{blue}{\href{http://arxiv.org/abs/1503.04100}{Phys.Rev.D91(2015)114012}}}, F.Beaujean , M.Chrzaszcz, N.Serra, D. van Dyk for details.\\ +\ARROW The idea behind Method of Moments is simple: Use orthogonality of spherical harmonics, $f_j(\overrightarrow{\Omega})$ to solve for coefficients within a $q^2$ bin: +\begin{align*} +\int f_i(\overrightarrow{\Omega}) f_j(\overrightarrow{\Omega}) = \delta_{ij} +\end{align*} +\begin{align*} +M_i = \int \left( \dfrac{1}{d(\Gamma+ \bar{\Gamma})/dq^2} \right) \dfrac{d^3(\Gamma+\bar{\Gamma})}{d \overrightarrow{\Omega}} f_i(\overrightarrow{\Omega})d \Omega +\end{align*} +\ARROW Don’t have true angular distribution but we ''sample'' it with our data.\\ +\ARROW Therefore: $\int \to \sum$ and $M_i \to \widehat{M}_i$ +\begin{align*} +\hat{M}_i=\dfrac{1}{\sum_e \omega_e} \sum_e \omega_e f_i(\overrightarrow{\Omega}_e) +\end{align*} +\ARROW The weight $\omega$ accounts for the efficiency. Again the normalization of weights does not matter. + + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Method of moments - results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + +\only<3> +{ +\ARROW Method of Moments allowed us to measure for the first time a new observable: +} + +\begin{center} +\only<1>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_FLPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S3Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S4Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S5Pad.pdf} +} +\only<2>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_AFBPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S7Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S8Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S9Pad.pdf} +} +\only<3>{ +\includegraphics[angle=-90,width=0.75\textwidth]{images/S6cPad.pdf} +} + +\end{center} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + + + + + +\begin{frame}{Compatibility with SM} +{~} + + \begin{minipage}{\textwidth} + +\begin{columns} +\column{0.1in} +{~} +\column{2in} +\ARROW Use \texttt{EOS} software package to test compatibility with SM.\\ +\ARROW Perform the $\chi^2$ fit to the measured: +\begin{center} +\begin{align*} +F_L, A_{FB}, S_{3,..., 9} . +\end{align*} +\end{center} +\ARROW Float a vector coupling: $\Re(C_9)$.\\ +\ARROW Best fit is found to be $3.4~\sigma$ away from the SM. + + +\column{3in} +\begin{align*} +\Delta \Re (C_9) \equiv \Re(C_9)^{{\rm fit}} - \Re(C_9)^{{\rm SM}} = -1.03 +\end{align*} +\includegraphics[angle=-90,width=0.95\textwidth]{images/wilsonchi2.pdf} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}\frametitle{Global picture of $P_5^{\prime}$} + +\begin{columns} + +\column{0.4\textwidth} +\only<1>{{\color{gray}{\ARROW 2013 LHCb: \href{https://arxiv.org/pdf/1308.1707.pdf}{arXiv::1308.1707}}}\\} +\only<1>{\ARROW 2015 LHCb: \href{https://arxiv.org/abs/1512.04442}{arXiv::1512.0444}\\} +\only<1>{{\color{red}{\ARROW 2016 Belle: \href{https://arxiv.org/abs/1604.04042}{arXiv::1604.04042}}}\\} +\only<1>{\ARROW 2017: {\color{blue}{\href{https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2017-023/}{ATLAS-CONF-2017-023}}} $(20.5~\rm fb^{-1})$ and {\color{OliveGreen}{\href{http://cds.cern.ch/record/2256738?ln=en}{CMS-PAS-BPH-15-008}}} $(20.8~\rm fb^{-1})$} + + + +\column{0.6\textwidth} +\only<1>{ +\ARROW Theory: +~~DHMV: \href{https://arxiv.org/abs/1407.8526}{arXiv::1407.8526} +~~ASZB: \href{https://arxiv.org/abs/1411.3161}{arXiv::1411.3161} +} +%\includegraphics[width=0.95\textwidth]{images/P5p1.png} +\only<1>{ +\includegraphics[angle=-90,width=0.9\textwidth]{images/P5p.pdf} +} + + +\end{columns} +\only<1>{ + + +} + +\end{frame} + + + +\iffalse + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PLambdab \to \PLambda \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + + \begin{center} + \only<1>{ + \includegraphics[width=0.65\textwidth]{images/Lb_BR.png} +} + \only<2>{ + \includegraphics[width=0.45\textwidth]{images/Lblow.png} +\includegraphics[width=0.45\textwidth]{images/Lbhigh.png} + +} + + + \end{center} + + +\begin{itemize} +\item This years LHCb measurement [JHEP 06 (2015) 115]]. +\item In total $\sim 300$ candidates in data set. +\item Decay not present in the low $q^2$. + +\end{itemize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}{Angular analysis of $\PLambdab \to \PLambda \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item For the bins in which we have $>3~\sigma$ significance the forward backward asymmetry for the hadronic and leptonic system. +\end{itemize} +\begin{center} +\includegraphics[width=0.9\textwidth]{{images/AFB_Lb}.png} +\end{center} +\begin{itemize} +\item $A_{FB}^H$ is in good agreement with SM. +\item $A_{FB}^{\ell}$ always in above SM prediction. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Lepton universality test} +{~} + \begin{minipage}{\textwidth} +\begin{columns} +\column{3.0in} +\begin{itemize} +\item If $\PZprime$ is responsible for the $P'_5$ anomaly, does it couple equally to all flavours? +\includegraphics[width=0.9\textwidth]{images/uni2.png} +\item Challenging analysis due to bremsstrahlung. +\item Migration of events modeled by MC. +\item Correct for bremsstrahlung. +\item Take double ratio with $\PBplus \to \PJpsi \PKplus$ to cancel systematics. +\item In $3\invfb$, LHCb measures $R_K=0.745^{+0.090}_{-0.074}(stat.)^{+0.036}_{-0.036}(syst.)$ +\item Consistent with SM at $2.6\sigma$. + +\end{itemize} +\column{2.0in} +\includegraphics[width=0.99\textwidth]{images/RK.png}\\ +\begin{itemize} +\item \href{http://arxiv.org/abs/1406.6482}{Phys. Rev. Lett. 113, 151601 (2014)} +\end{itemize} +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Angular analysis of $\PBzero \to \PKstar \Pe \Pe$} +{~} +\only<1>{ + \begin{minipage}{\textwidth} + \begin{itemize} + \item With the full data set ($3\invfb$) we performed angular analysis in $0.0004 < q^2 <1~\GeV^2$. + \item Electrons channels are extremely challenging experimentally: + \begin{itemize} + \item Bremsstrahlung. + \item Trigger efficiencies. + \end{itemize} + \item Determine the angular observables: $\FL$, $\ATD$, $\ATRe$, $\ATIm$: + \end{itemize} +\begin{equation} + \label{eq:physPars} + \begin{split} + \FL &=\frac{|A_0|^2}{|A_0|^2+|A_{||}|^2 + |A_\perp|^2}\\ + \ATD &= \frac{|A_\perp|^2-|A_{||}|^2}{|A_\perp|^2+|A_{||}|^2}\\ + \ATRe &= \frac{2\Real(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}\\ + \ATIm &= \frac{2\Imag(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}, +\end{split}\nonumber +\end{equation} + +\end{minipage} +} +\only<2>{ +\begin{center} +\includegraphics[width=0.5\textwidth]{images/Kstee.png}\\ +\end{center} +\begin{itemize} +\item Results in full agreement with the SM. +\item Similar strength on $C_7$ Wilson coefficient as from $\Pbeauty \to \Pstrange \Pphoton$ decays. +\end{itemize} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/Kstee2.png} +\end{center} + +} + \vspace*{2.1cm} +\end{frame} + +\fi + +\begin{frame} +\begin{center} +\begin{Huge} +Global fit to $\Pbeauty \to \Pstrange \ell \ell$ measurements +\end{Huge} +\end{center} + + + + +\end{frame} + + + +\begin{frame}{Link the observables} +\begin{footnotesize} + +\ARROW Fits prepare by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}} + +\begin{itemize} + +\item Inclusive + +\begin{itemize} +\item $B\to X_s\gamma$ {\color{gray}($BR$) +.......................................................... } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} +\item $B\to X_s\ell^+\ell^-$ {\color{gray}($dBR/dq^2$) +............................................ } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} +\end{itemize} + +\item Exclusive leptonic + +\begin{itemize} +\item $B_s\to \ell^+\ell^-$ {\color{gray}($BR$) +........................................................ } {\color{red} $\C{10}^{(\prime)}$} +\end{itemize} + +\item Exclusive radiative/semileptonic +\begin{itemize} +\item $B\to K^*\gamma$ {\color{gray}($BR$, $S$, $A_I$) +................................................ } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $B\to K\ell^+\ell^-$ {\color{gray}($dBR/dq^2$) +.............................................. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $\bf \color{Red} B\to K^*\ell^+\ell^-$ {\color{gray}($dBR/dq^2$, {\bf Optimized Angular Obs.}) +.. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $B_s\to \phi \ell^+\ell^-$ {\color{gray}($dBR/dq^2$, Angular Observables) +.............. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $\Lambda_b\to \Lambda\ell^+\ell^-$ {\color{gray}(None so far)} +\item etc. +\end{itemize} + + + +\end{itemize} +\end{footnotesize} + +\end{frame} + +\frame{ \frametitle{Statistic details} + +\begin{footnotesize} + +\ARROW Frequentist approach: +\medskip + +$$\chi^2(C_i) = [O_\text{exp}- O_\text{th}(C_i)]_j \, [Cov^{-1}]_{jk}\, [O_\text{exp}- O_\text{th}(C_i)]_k$$ + + +\begin{itemize} +\item $\bf Cov = Cov^\text{exp} + Cov^\text{th}$. We have $Cov^\text{exp}$ for the first time +\item Calculate $Cov^\text{th}$: correlated multigaussian scan over all nuisance parameters +\item $Cov^\text{th}$ depends on $C_i$: Must check this dependence\\[5mm] +\end{itemize} +For the Fit: +\begin{itemize} +\item Minimise $\chi^2 \to \chi^2_\text{min} = \chi^2(C_i^0)\quad$ (Best Fit Point = $C_i^0$) +\item Confidence level regions: $\chi^2(C_i) - \chi^2_\text{min} < \Delta\chi_{\sigma,n}$ +%\item Compute pulls by inversion of the above formula +\end{itemize} +\medskip +\ARROW The results from 1D scans:{~}\\{~}\\ +\begin{tiny} +\begin{tabular}{crccc} +%\toprule[1.6pt] +Coefficient ${\cal C}_i^{NP}={\cal C}_i-{\cal C}_i^{SM}$ & Best fit & 1$\sigma$ & 3$\sigma$ & Pull$_{\rm SM}$ \\ \hspace{10mm} \\[5mm] +% \midrule + $\bf\cred\C9^{\rm NP}$ & $ -1.09 $ & $ [-1.29,-0.87] $ & $ [-1.67,-0.39] $ & $\,\,\,\,\,\,\bf 4.5 + \cred \Leftarrow$ \hspace{5mm} \\[3mm] + $\C9^{\rm NP}=-\C{10}^{\rm NP}$ & $ -0.68 $ & $ [-0.85,-0.50] $ & $ [-1.22,-0.18] $ & \bf \quad 4.2 + $\cred\Leftarrow$ \hspace{5mm} \\[3mm] + $\C9^{\rm NP}=-\C{9'}^{\rm NP}$ & $ -1.06 $ & $ [-1.25,-0.86] $ & $ [-1.60,-0.40] $ & \quad \quad \quad \,\,\quad 4.8 + $\cred\Leftarrow$ (no $R_K$)\hspace{5mm} \\[3mm] + + \hspace{5mm} \\[3mm] +% \bottomrule[1.6pt] +\end{tabular} +\end{tiny} +\end{footnotesize} + +} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Theory implications} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item The data can be explained by modifying the $C_9$ Wilson coefficient. +\item Overall there is around $4.5~\sigma$ discrepancy wrt. SM. +\end{itemize} +\includegraphics[width=0.9\textwidth]{images/C9.png} + + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{2D scans} +{~} +\begin{footnotesize} + + \begin{minipage}{\textwidth} +\begin{columns} +\begin{column}{0.5cm} + + +\end{column} +\begin{column}{17cm} + +\renewcommand{\arraystretch}{1.4} + \setlength{\tabcolsep}{13pt} +\begin{tabular}{cccr} +\hline +Coefficient & Best Fit Point & Pull$_{\rm SM}$ \\ \hline + + $(\C7^{\rm NP},\C9^{\rm NP})$ & $(-0.00,-1.07)$ & {\bf 4.1} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{10}^{\rm NP})$ & $(-1.08,0.33)$ & {\bf 4.3} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{7'}^{\rm NP})$ & $(-1.09,0.02)$ & {\bf 4.2} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{9'}^{\rm NP})$ & $(-1.12,0.77)$ & {\bf 4.5} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{10'}^{\rm NP})$ & $(-1.17,-0.35)$ & {\bf 4.5} \hspace{5mm} \\ + $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ & $(-1.15,0.34)$ & \!\!\!\!\!\!\!\!\!\!\! {\bf 4.7} \\ + $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=-\C{10'}^{\rm NP})$ & $(-1.06,0.06)$ & {\bf 4.4} \hspace{5mm} \\ + $(\C{9}^{\rm NP}=\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ & $(-0.64,-0.21)$ & 3.9 \hspace{5mm} \\ + $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=\C{10'}^{\rm NP})$ & $(-0.72,0.29)$ & 3.8 \hspace{5mm} \\ +% $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ & $(-0.66,0.03)$ & 2.0 & 23.0 + %$(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ & $(-0.69,0.05)$ & 1.9 & 22.0 \hspace{5mm} \\ + +\end{tabular} +\end{column} +\end{columns} + + +\medskip +\begin{itemize} +\item $C_9^{NP}$ always play a dominant role +\item All 2D scenarios above 4$\sigma$ are quite indistinguishable. + +\end{itemize} + + + +\end{minipage} + +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%% + + + +\begin{frame}{$B\to K^\ast \ell\ell\ $ Amplitudes} + +\small + +\mbox{ +\includegraphics[width=3cm,height=2cm]{bsg0.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2cm]{bsg1.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2.4cm]{bsg2.jpg} +} + +\vspace{3mm} + +\mbox{ +\hspace{-10mm} +\colorbox{llgray}{ +\hspace{1mm} +$\displaystyle +A_\lambda^{L,R} = N_\lambda\ \bigg\{ +(C_9 \mp C_{10}) {\blue \F_\lambda(q^2)} ++\frac{2m_b M_B}{q^2} \bigg[ C_7 {\blue \F_\lambda^{T}(q^2)} +- 16\pi^2 \frac{M_B}{m_b} {\red \H_\lambda(q^2)} \bigg] +\bigg\} +$ +\hspace{2mm} +} +} + +\vspace{5mm} +{\small + +\hspace{-8mm} \btr {\brown Local (Form Factors) :} \hspace{2mm} {\blue $ \F_\lambda^{(T)}(q^2) = \av{\bar M_\lambda(k)| \,\bar s\, \Gamma_\lambda^{(T)}\, b\, | \bar{ B}(k+q)}$} +\\[5mm] + +\mbox{ +\hspace{-9mm} +\btr {\brown Non-Local :} \hspace{0mm} {\red $\displaystyle \H_\lambda(q^2) = i \,{\cal P}_\mu^\lambda \int d^4 x\ e^{i q\cdot x}\, +\av{\bar{M}_\lambda(k)| +T\big\{ {\cal J}_{\rm em}^\mu(x), \C{i} \, \mathcal{O}(0) \big\} | \bar{B}(q+k)}$} +} + +\vspace{3mm} + +\hspace{-8mm} +\btr CKM structure : \hspace{2mm} $\displaystyle \H_\lambda = {\color{gray}- \frac{\lambda_u}{\lambda_t} \H_\lambda^{(u)}} - \frac{\lambda_c}{\lambda_t} \H_\lambda^{(c)}$ \hspace{5mm} $\Rightarrow\ \mathcal{O} \sim (\bar{ c} b)(\bar{ s} c)$ + +} + +\end{frame} + + + + + +\begin{frame}{Analytic structure of $\H_\lambda(q^2)$} + +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{3mm} + + +Neglecting OZI- and CKM-suppressed contributions : + +\begin{center} +\includegraphics[width=7.5cm]{Analyticq2.png} +\end{center} + + +$\displaystyle { \hat{\mathcal{H}}_\lambda(q^2)} = (q^2 - M_{J/\psi}^2)(q^2 -M_{\psi(2S)}^2) \,{ {\mathcal{H}}_\lambda(q^2)} \quad $ has no poles. + +\end{frame} + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} + +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{2mm} + +\btr Conformal mapping : \hspace{5mm} $q^2 \mapsto \ z\,(q^2) = \frac{\sqrt{t_+ - q^2} - \sqrt{t_+ - t_0}}{\sqrt{t_+ - q^2} + \sqrt{t_+ - t_0}}$ + +\mbox{ +\hspace{-10mm} +\raisebox{8mm}{\includegraphics[width=5.6cm]{Analyticq22.png}} +\hspace{1mm} +\includegraphics[width=6.5cm]{Analyticz.png} +} + +\vspace{-7mm} + +\btr ${\red \hat \H_\lambda (q^2(z))}$ is {\bf analytic in $|z|<1$}\\[3mm] + +\btr Taylor expand $\red \hat{\H}_\lambda(z)$ around $z=0$.\\[3mm] + +\btr Expansion needed for $|z| < 0.52\ $ ( $-7\,\GeV^2 \leq q^2 \leq 14 \GeV^2$ ) + + +\end{frame} + + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} + +\vspace{3mm} + + +\hspace{-5mm} {\bf \brown Some details for actual parametrisation :} + +\mbox{\hspace{-5mm} \btr Try to capture most features of the expansion (better convergence)} + +\mbox{\hspace{-5mm} \btr Parametrize the ratios $\H_\lambda(q^2)/\F_\lambda(q^2)$ instead} + +\mbox{\hspace{-5mm} \btr The poles should not modify the asymptotic behaviour at $|q^2|\to \infty$} + +\begin{eqnarray} +\H_\lambda(z) &=& +\frac{1-z\, z^*_{J/\psi}}{z-z_{J/\psi}} \frac{1-z\,z^*_{\psi(2S)}}{z-z_{\psi(2S)}} \ \hat\H_\lambda(z) +\nonumber\\[2mm] +% +\hat\H_\lambda(z) &=& \Big[ \sum_{k=0}^K \alpha_k^{(\lambda)} z^{k} \Big] \F_\lambda(z) +\nonumber +\end{eqnarray} + + +where $\alpha^{(\lambda)}_k$ are complex coefficients, and the expansion is truncated after the term $z^{K}$. +We will take $K=2$ ({\brown 16} real parameters). + + +\end{frame} + + + + +\begin{frame}{Experimental constraints on $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown Experimental constraints :} + +\mbox{\hspace{-5mm} \btr The residues of the poles are given by $B\to K^* \psi_n$ :} + +$$ +\H_\lambda(q^2 \to M_{\psi_n}^2) \sim +\frac{M_{\psi_n} f^{\,*}_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2 (q^2 - M_{\psi_n}^2)} + \cdots +$$ + +\mbox{\hspace{-5mm} \btr Angular analyses \Cite{Belle, Babar, LHCb} determine : } + +$$ +|r_\perp^{\psi_n}|,\, +|r_\|^{\psi_n}|,\, +|r_0^{\psi_n}|,\, +\arg\{r_\perp^{\psi_n} r_{0}^{\psi_n*}\},\, +\arg\{r_\|^{\psi_n} r_{0}^{\psi_n*}\}, +$$ + +where $\quad \displaystyle r_\lambda^{\psi_n} \equiv \operatorname*{Res}_{q^2\to M^2_{\psi_n}} \frac{\H_\lambda(q^2)}{\F_\lambda(q^2)} +\sim +\frac{M_{\psi_n} f^*_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2\, \F_\lambda(M_{\psi_n}^2)}$\\[3mm] + + +\mbox{\hspace{-5mm} \btr We produce correlated pseudo-observables from a fit (5+5).} + + + +\end{frame} + + + + +\begin{frame}{Prior Fit to $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown (Prior) Fit to Experimental and theoretical pseudo-observables :} + + + +\begin{table}[b] +% \resizebox{.85\textwidth}{!}{% +\centering +\renewcommand{\arraystretch}{1.5} +\renewcommand{\tabcolsep}{3.1mm} +\begin{tabular}{@{}crrr@{}} +\hline +$k$ & 0\hspace{7mm} & 1\hspace{7mm} & 2\hspace{7mm} \\ +\hline +%re perp +${\rm Re}[\alpha_{k}^{(\perp)}]$ & $-0.06 \pm 0.21$ & $-6.77 \pm 0.27$ & $18.96 \pm 0.59$ \\ +%re para +${\rm Re}[\alpha_{k}^{(\parallel)}]$ & $-0.35 \pm 0.62$ & $-3.13 \pm 0.41$ & $12.20 \pm 1.34$ \\ +%re long +${\rm Re}[\alpha_{k}^{(0)}]$ & $0.05 \pm 1.52$ & $17.26 \pm 1.64$ & -- \\ +%im perp +${\rm Im}[\alpha_{k}^{(\perp)}]$ & $-0.21 \pm 2.25$ & $1.17 \pm 3.58$ & $-0.08 \pm 2.24$ \\ +%im para +${\rm Im}[\alpha_{k}^{(\parallel)}]$ & $-0.04 \pm 3.67$ & $-2.14 \pm 2.46$ & $6.03 \pm 2.50$ \\ +%im long +${\rm Im}[\alpha_{k}^{(0)}]$ & $-0.05 \pm 4.99$ & $4.29 \pm 3.14$ & -- \\ +\hline +\end{tabular} +% } +\caption{Mean values and standard deviations (in units of $10^{-4}$) +of the prior PDF for the parameters $\alpha_k^{(\lambda)}$.} +\label{alphak} +\end{table} + +\end{frame} + +\begin{frame}{New Physics Analysis } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown SM predictions and Fit including $B\to K^* \mu^+\mu^-$ data and $\C{9}^{\rm NP}$ :}\\[4mm] + +\mbox{ +\hspace{-10mm} +\includegraphics[width=12cm]{NPFit.png} +} + +The NP hypothesis with {\red $\C{9}^{\bf NP}\sim -1$} is favored strongly in the global fit + +\end{frame} + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Scale of NP?} +{~} + \begin{minipage}{\textwidth} +\includegraphics[width=0.99\textwidth]{15.png} + +\ARROW Stolen from M. Nardecchia +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Conclusions} +{~} + \begin{minipage}{\textwidth} +\begin{itemize} +\item Clear tensions wrt. SM predictions! +\item Measurements cluster in the same direction. +\item We are not opening the champagne yet! +\item Still need improvement both on theory and experimental side. +\item Time will tell if this is QCD+fluctuations or new Physics: +\end{itemize} +\pause +''... when you have eliminated all the\\ +Standard Model explanations, whatever remains,\\ +however improbable, must be New Physics.''\\ +prof. Joaquim Matias + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +{~} + \begin{minipage}{\textwidth} +\begin{center} +\begin{LARGE} +Thank you for the attention! +\end{LARGE} +\includegraphics[width=0.8\textwidth]{images/Joke.jpg} + +\end{center} + + + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +\backupbegin + +\begin{frame}\frametitle{Backup} + + +\end{frame} + + + + +\begin{frame}{Amplitudes method} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + +\ARROW Fit for amplitudes as (continuous) functions of $q^2$ in the region: $q^2 \in \left[ 1.1. 6.0 \right]~\GeV^2/c^4$.\\ +\ARROW Needs some Ansatz: +\begin{align*} +A(q^2) = \alpha + \beta q^2+ \dfrac{\gamma}{q^2} +\end{align*} +\ARROW The assumption is tested extensively with toys.\\ +\ARROW Set of 3 complex parameters $ \alpha, \beta, \gamma $ per vector amplitude:\begin{itemize} +\item {\color{Magenta}{$L, ~R$}}, {\color{Cerulean}{$0 ,~\| ,~\bot$}}, {\color{PineGreen}{$\Re ,~\Im$}} $\rightarrowtail$~~ $3 \times {\color{PineGreen}{2}} \times {\color{Cerulean}{3}} \times {\color{Magenta}{2}} = 36$ DoF. +\item Scalar amplitudes: $+4$ DoF. +\item Symmetries of the amplitudes reduces the total budget to: $28$. +\end{itemize} +\ARROW The technique is described in \href{http://arxiv.org/pdf/1504.00574v2.pdf}{\color{blue}{JHEP06(2015)084}}.\\ +\ARROW Allows to build the observables as continuous functions of $q^2$: +\begin{itemize} +\item At current point the method is limited by statistics. +\item In the future the power of this method will increase. +\end{itemize} +\ARROW Allows to measure the zero-crossing points for free and with smaller errors than previous methods. +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Amplitudes - results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} +\begin{center} +\begin{columns} +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_AFBOverlay}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S4Overlay}.pdf} + +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S5Overlay}.pdf}\\ +{~}\\{~}\\{~}\\{~}\\ +\begin{large} +Zero crossing points: +\end{large} +\begin{align*} +q_0(S_4) & <2.65 & {\rm{~at~}} & 95\% ~CL \\ +q_0(S_5) & \in \left[ 2.49,3.95 \right] & {\rm{~at~}} & 68\% ~CL \\ +q_0(A_{FB}) & \in \left[ 3.40, 4.87 \right] & {\rm{~at~}} & 68\% ~CL +\end{align*} + + +\end{columns} +\end{center} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\backupend + +\end{document} diff --git a/Seminars/FCAL/mchrzasz.toc b/Seminars/FCAL/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Seminars/FCAL/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/Seminars/FCAL/tikzfeynman.sty b/Seminars/FCAL/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ b/Seminars/FCAL/tikzfeynman.sty @@ -0,0 +1,43 @@ +% Tikz Feynman Diagrams +% by Flip Tanedo +% 4 January 2011, work in progress + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% TIKZ - for drawing Feynman diagrams %%%% +%%% ... use with pdflatex %%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/Seminars/India_IMSC_2018/Makefile b/Seminars/India_IMSC_2018/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/Seminars/India_IMSC_2018/Makefile @@ -0,0 +1,9 @@ +all: mchrzasz.pdf + +mchrzasz.pdf: mchrzasz.tex + xelatex mchrzasz.tex +# bibtex mchrzasz + xelatex mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out *.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/Seminars/India_IMSC_2018/beamercolorthemeFlip.sty b/Seminars/India_IMSC_2018/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/Seminars/India_IMSC_2018/beamercolorthemeFlip.sty @@ -0,0 +1,179 @@ +% Color style file for the BEAMER FLIP THEME +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + + + +\mode +\newif\ifbeamer@Flip@dark +\beamer@Flip@darkfalse +\DeclareOptionBeamer{dark}{\beamer@Flip@darktrue} +\ProcessOptionsBeamer + + +% These are a few colors that I like. + +\definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +\definecolor{darkcharcoal}{RGB}{25,25,25} % Darker gray +\definecolor{charcoal}{RGB}{51,51,51} % Darker gray +\definecolor{ash}{RGB}{100,100,100} % medium gray +\definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +\definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +\definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +\definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +\definecolor{regal}{RGB}{90,0,120} % A more neutral purple +\definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% Define some "invariant colors" so that a color that doen't work with a +% light/dark background will automatically be substituted with one that does. +% These will be rewritten in beamercolorthemeFlipDark + +\ifbeamer@Flip@dark + \definecolor{FlipSand}{RGB}{204,204,102} % paleale, Only for dark BG + \definecolor{FlipGreen}{RGB}{0,255,0} % Neon-like green, only for dark BG +\else + \definecolor{FlipSand}{RGB}{140,110,10} % lager, Only for light BG + \definecolor{FlipGreen}{RGB}{51,153,0} % turtlegreen, works for both +\fi + +%% Future revision: It would be nice to define these in terms of the palette. + + +\ifbeamer@Flip@dark + \setbeamercolor{normal text}{fg=white, bg=black} + \setbeamercolor{structure}{fg=gray, bg=black} % fg controls bullets + \setbeamercolor*{footerlike}{fg=white,bg=black} % Controls the footerline +\else + % Default to black on white + \setbeamercolor*{footerlike}{fg=white,bg=charcoal} % for charcoal footer + \setbeamercolor{structure}{fg=charcoal, bg=white} % fg controls bullets + % \setbeamercolor{normal text}{fg=white, bg=black} +\fi + + + + + +% These defined colors can be used in \textcolor{colorname}{text in that color}. + +% Colors for Keynote background: DARK +\definecolor{keynotebottom}{rgb}{0.32,0.3,0.38} +\definecolor{keynotemiddle}{rgb}{0.08,0.08,0.16} +\definecolor{keynotetop}{rgb}{0,0,0} +%%% Example of usage: +%% \setbeamertemplate{background canvas}[vertical shading] +%% [bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + + + +% ALERT AND COMMENT COLORS (just copies of the above colors) +% (I don't know how ot do this more elegantly) +\ifbeamer@Flip@dark + \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{alert}{RGB}{204,204,102} % paleale + \definecolor{charcoal}{RGB}{51,51,51} % charcoal + \definecolor{comment}{RGB}{80,80,80} % light charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\else +% \definecolor{ALERT}{RGB}{153,0,0} % crimsonred + \definecolor{ALERT}{RGB}{28,134,238} % DodgerBlue2 +% \definecolor{Alert}{RGB}{51,153,0} % turtlegreen + \definecolor{Alert}{RGB}{255,127,36} % chocolate1 +% \definecolor{alert}{RGB}{140,110,10} % lager + \definecolor{alert}{RGB}{0,205,102} % SpringGreen3 + \definecolor{charcoal}{RGB}{80,80,80} % light charcoal + \definecolor{comment}{RGB}{51,51,51} % charcoal + \definecolor{Comment}{RGB}{100,100,100} % ash + \definecolor{COMMENT}{RGB}{80,20,120} % regal +\fi + + +% \definecolor{crimsonred}{RGB}{153,0,0} % Neurtal red, good for dark or light bg +% \definecolor{charcoal}{RGB}{51,51,51} % Darker gray +% \definecolor{ash}{RGB}{100,100,100} % medium gray +% \definecolor{paleblue}{RGB}{0,102,102} % More of an `ocean' color +% \definecolor{turtlegreen}{RGB}{51,153,0} % A more neutral green +% \definecolor{paleale}{RGB}{204,204,102} % Only for dark BG +% \definecolor{lager}{RGB}{140,110,10} % Use instead of pale ale for white BG +% \definecolor{regal}{RGB}{90,0,120} % A more neutral purple +% \definecolor{jeans}{RGB}{20,30,150} % A more neutral blue + + +% A few useful colors +\setbeamercolor{alerted text}{fg=alert} + +%% I would like ot use these colors, but there seems to be a bug in Beamer +%% where the footnote color infects the normal text color +%% See: http://tex.stackexchange.com/questions/8264/beamer-changing-the-footnote-color-also-changes-the-normal-text-color/8268#8268 + +% \setbeamercolor{footnote}{parent=normal text, fg=FlipSand} +% \setbeamercolor{footnote mark}{parent=normal text, fg=FlipSand} + +% Blocks +\setbeamercolor{block title}{fg=gray!30!white,bg=charcoal} +\setbeamercolor{block body}{parent=normal text,bg=gray, fg=white} + +\setbeamercolor{block title example}{fg=turtlegreen!30!white,bg=turtlegreen!40!black} +\setbeamercolor{block body example}{parent=normal text,bg=turtlegreen, fg=white} +% +\setbeamercolor{block title alerted}{fg=crimsonred!30!white,bg=crimsonred!40!black} +\setbeamercolor{block body alerted}{parent=normal text,bg=crimsonred, fg=white} + + + +% These "setbeamercolor" commands are more standardized. + + +%% From the Beamer User Guide: +% Outer themes base the color of navigational elements and, possibly, also of other elements, on the +% four palette colors. The “primary” palette should be used for the most important navigational elements, +% which are usually the ones that change most often and hence require the most attention by the audience. +% The “secondary” and “tertiary” are less important, the “quaternary” one is least important. +% By default, the palette colors do not have a background and the foreground ranges from structure.fg to black. +% For the sidebar, there is an extra set of palette colors, see palette sidebar primary. + +\setbeamercolor*{palette primary}{fg=crimsonred,bg=charcoal} +\setbeamercolor*{palette secondary}{fg=paleale,bg=lager} +\setbeamercolor*{palette tertiary}{fg=turtlegreen,bg=jeans} +\setbeamercolor*{palette quaternary}{fg=paleblue,bg=regal} + +% \setbeamercolor*{palette primary}{fg=crimsonred,bg=white} +% \setbeamercolor*{palette secondary}{fg=charcoal,bg=white} +% \setbeamercolor*{palette tertiary}{fg=paleblue,bg=white} +% \setbeamercolor*{palette quaternary}{fg=turtlegreen,bg=white} + + + +%% These are some structures that I define for use in the outer theme. + +\setbeamercolor*{crimsontown}{fg=paleblue,bg=crimsonred} +\setbeamercolor*{bluetown}{fg=white,bg=DodgerBlue2} +%\setbeamercolor*{titlelike}{fg=crimsonred} +\setbeamercolor*{titlelike}{fg=DodgerBlue2} +\setbeamercolor*{topbarlike}{fg=white, bg=charcoal} + + + + + +%% Some old definitions that I might want to get back to +% +% \setbeamercolor*{frametitle}{bg=white,fg=charcoal} +% \setbeamercolor*{part title}{bg=white,fg=charcoal} +% \setbeamercolor*{item}{fg=charcoal, bg=white} +% +% \setbeamercolor*{separation line}{} +% \setbeamercolor*{fine separation line}{} + + + + + +\mode + diff --git a/Seminars/India_IMSC_2018/beamerinnerthemeFlip.sty b/Seminars/India_IMSC_2018/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/Seminars/India_IMSC_2018/beamerinnerthemeFlip.sty @@ -0,0 +1,95 @@ +% Inner style file for the BEAMER FLIP THEME +% Copyright 2010 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerinnerthemeFlip by Marco Barisione + +\mode + +% % Use alternative title page style. +% \DeclareOptionBeamer{alternativetitlepage}[true]{\def\beamer@Flip@alternativetitlepage{#1}} + +% Logo to use in the alternative title page. +% \def\beamer@Flip@titlepagelogo{} +% \DeclareOptionBeamer{titlepagelogo}{\def\beamer@Flip@titlepagelogo{#1}} + +% Bullet shape. +\DeclareOptionBeamer{bullet}{\def\beamer@Flip@bullet{#1}} +\DeclareOptionBeamer{shadow}[true]{\def\beamer@themerounded@shadow{#1}} +\ExecuteOptionsBeamer{shadow=false} + + +% \ExecuteOptionsBeamer{alternativetitlepage=false,bullet=square} +\ProcessOptionsBeamer + + + +% Margins. +\newlength{\beamer@Flip@normalmargin} +\setlength{\beamer@Flip@normalmargin}{.06\paperwidth} +\setbeamersize{text margin left=\beamer@Flip@normalmargin} +\setbeamersize{text margin right=\beamer@Flip@normalmargin} +\setlength\leftmargini{.6\beamer@Flip@normalmargin} +\setlength\leftmarginii{.6\beamer@Flip@normalmargin} +\setlength\leftmarginiii{.6\beamer@Flip@normalmargin} + +% Normal title page. +\defbeamertemplate*{title page normal}{Flip theme}[1][] +{ + \vbox{} + \vfill + \begin{centering} + \begin{beamercolorbox}[wd=\paperwidth,sep=8pt,center,#1]{title page header} + \usebeamerfont{title}\inserttitle\par% + \ifx\insertsubtitle\@empty% + \else% + \vskip0.25em% + {\usebeamerfont{subtitle}\usebeamercolor[fg]{subtitle}\insertsubtitle\par}% + \fi% + \end{beamercolorbox}% + \vskip1em\par + \begin{beamercolorbox}[sep=8pt,center,#1]{author} + \usebeamerfont{author}\insertauthor + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{institute} + \usebeamerfont{institute}\insertinstitute + \end{beamercolorbox} + \begin{beamercolorbox}[sep=8pt,center,#1]{date} + \usebeamerfont{date}\insertdate + \end{beamercolorbox}\vskip0.5em + {\usebeamercolor[fg]{titlegraphic}\inserttitlegraphic\par} + \end{centering} + \vfill +} + + +% Items. +\defbeamertemplate{itemize item}{squarealt}% +{\tiny\raise.5ex\hbox{\donotcoloroutermaths$\blacksquare$}} +\defbeamertemplate{itemize subitem}{squarealt}% +{\tiny\raise.4ex\hbox{\donotcoloroutermaths$\square$}} +\defbeamertemplate{itemize subsubitem}{squarealt}% +{\tiny\raise.3ex\hbox{\donotcoloroutermaths$\blacksquare$}} +% +\defbeamertemplate{itemize item}{circlealt}% +{\small\raise.2ex\hbox{\donotcoloroutermaths$\bullet$}} +\defbeamertemplate{itemize subitem}{circlealt}% +{\small\raise.1ex\hbox{\donotcoloroutermaths$\circ$}} +\defbeamertemplate{itemize subsubitem}{circlealt}% +{\scriptsize\raise.1ex\hbox{\donotcoloroutermaths$\bullet$}} +\setbeamertemplate{items}[circlealt] +% +\def\circletext{circle} +\ifx\beamer@Flip@bullet\circletext + \setbeamertemplate{items}[circlealt] +\else + \setbeamertemplate{items}[squarealt] +\fi + +\setbeamertemplate{blocks}[rounded][shadow=\beamer@themerounded@shadow] + + +\mode + diff --git a/Seminars/India_IMSC_2018/beamerouterthemeFlip.sty b/Seminars/India_IMSC_2018/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/Seminars/India_IMSC_2018/beamerouterthemeFlip.sty @@ -0,0 +1,189 @@ +% Outer style file for the BEAMER FLIP THEME 212 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Based on: beamerouterthemesplit by Till Tantau + + +\mode + +% Watermark +\DeclareOptionBeamer{watermark}{\def\beamer@Flip@watermark{#1}} +\ExecuteOptionsBeamer{watermark=} % Default value is empty + + +\newif\ifbeamer@Flip@bigpagenumber +\beamer@Flip@bigpagenumberfalse +\DeclareOptionBeamer{bigpagenumber}{\beamer@Flip@bigpagenumbertrue} + + +\def\beamer@Flip@truetext{true} % Kludge for true/false so I can use ifx + +\DeclareOptionBeamer{topline}[true]{\def\beamer@Flip@topline{#1}} +\ExecuteOptionsBeamer{topline=false} % Default + + + +% \ExecuteOptionsBeamer{topline=} % Default value is empty + + +\ProcessOptionsBeamer + + +\usepackage{tikz} % For fancy decorations + + +% I should fix these up to be more robust against color changes +\setbeamercolor{section in head/foot}{parent=footerlike} +\setbeamercolor{subsection in head/foot}{parent=footerlike} +\setbeamercolor{author in head/foot}{parent=footerlike} +\setbeamercolor{title in head/foot}{parent=footerlike} + + +% \setbeamercolor{author in head/foot}{parent=section in head/foot} +% \setbeamercolor{title in head/foot}{parent=subsection in head/foot} + +%\setbeamercolor{topbar}{parent=crimsontown} +\setbeamercolor{topbar}{parent=bluetown} + + + + +\usesectionheadtemplate + {\hfill\insertsectionhead} + {\hfill\color{fg!50!bg}\insertsectionhead} + + +%%%%%%%%%%%%%%%%%% +% The footer bar % +%%%%%%%%%%%%%%%%%% + +\defbeamertemplate*{footline}{Flip theme} +{% + \leavevmode% +% OBSERVATION: the "%" symbols inside hbox are all very important here. +% The \hbox enviroment will insert spaces whenever there's whitespace +% Adding a % at the END of each line ensures that any hard returns aren't +% interpreted as white space. This allows the color boxes to be flush against +% one another. If a faint white line appears one could probably do something like +% hspace{-1px} and add an additional pixel-or-two wide beamercolorbox. + +\hbox{% +\begin{beamercolorbox}[wd=.4\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm, rightskip=.3cm plus1fil]{author in head/foot}% + \usebeamerfont{author in head/foot}\insertshortauthor \end{beamercolorbox}% +% +\begin{beamercolorbox}[wd=.6\paperwidth,ht=2.5ex,dp=1.125ex,leftskip=.3cm,rightskip=.3cm plus1fil]{title in head/foot}% + \usebeamerfont{title in head/foot}{\textit \insertshorttitle}% + \hskip2ex plus1fill% + % \insertpagenumber\,/\,\insertpresentationendpage %% Want FRAME, not SLIDE number + \insertframenumber/\inserttotalframenumber + \end{beamercolorbox}% +}% + +% This is a complete kludge for the faint white line which appears +% between the beamer color boxes above. (It doesnt appear in presentation mode +% but sometimes looks funny when the pdfs are viewed in a window) +\begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[thick] (0,3.625ex) -- (\paperwidth,3.625ex); + \draw (.4\paperwidth,0) -- (.4\paperwidth,3.625ex); + \draw[thick] (0,0) -- (\paperwidth,0); +\end{tikzpicture} + + + +\ifbeamer@Flip@bigpagenumber + \begin{tikzpicture}[overlay] + \usebeamercolor[bg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (6ex); + \usebeamercolor[fg]{author in head/foot} + \draw[fill] (\paperwidth-5ex,3.625ex) circle (5ex); + \usebeamercolor[bg]{author in head/foot} + \node at (\paperwidth-5ex,4ex) {\small$^\text{\insertframenumber}/_\text{\inserttotalframenumber}$}; + \end{tikzpicture} +\fi +} + + + +\defbeamertemplate*{frametitle}{Flip theme}[1][left] +{ +% \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% +\@tempdima=\textwidth% +\advance\@tempdima by\beamer@leftmargin% +\advance\@tempdima by\beamer@rightmargin% + +\vbox{}\vskip-3.5ex% +% +\begin{beamercolorbox}[sep=0.3cm,#1,wd=\the\@tempdima]{titlelike} + \usebeamerfont{frametitle}% + \vbox{}\vskip-1ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + % \strut{\bf\insertframetitle}\strut\par% %% Include the \bf + \strut{\insertframetitle}\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else + {\usebeamerfont{framesubtitle} + \usebeamercolor[fg]{framesubtitle} + \insertframesubtitle\strut\par}% + \fi + }% + % + \vskip-1ex% + \if@tempswa\else\vskip-.3cm\fi% set inside beamercolorbox... evil here... +\end{beamercolorbox}% +%% + +% \def\beamer@fteright{\vskip0.35cm\advance\leftskip by 1.7cm\advance\rightskip by1.7cm} +} + + + + +% Sidebar right is important: anything placed here will be +% visible *behind* the main text. This is where to put any +% interesting watermarks. +% +% +\defbeamertemplate*{sidebar right}{Flip theme} +{ +% \llap{\includegraphics[width=50px]{footdecoration}} +% \llap{\includegraphics[width=\paperwidth,height=\paperheight]{upperleft_watermark_transp}} +% +% THIS WOULD BE A NICE WAY TO PUT THE PARTICLE BUBBLE CHAMBER BG +% ... make a png of the background with TRANSPARENT BG +% ... then put the image here (use \hfill to get it on the left) +% Now one can FURTHER apply a slight gradient in the BG +% +% +% % Top Line +\ifx\beamer@Flip@topline\beamer@Flip@truetext + \begin{tikzpicture}[overlay] + \usebeamercolor[fg]{titlelike} % alternately, topbarlike would be a good beamercolor +% \usebeamercolor[fg]{topbarlike} % alternately, topbarlike would be a good beamercolor + \draw[fill] (-\paperwidth,0) rectangle (0,-3pt); + \end{tikzpicture} +\fi +% +% + \vskip.2\beamer@leftmargin% + %\llap{\insertlogo\hskip.5\beamer@leftmargin}% + \llap{\insertlogo\hskip.08\beamer@leftmargin}% + \vfill% + \if \beamer@Flip@watermark\@empty + % This is kind of a kludge since if I put anything in here, I automatically get errors + % Somehow LaTeX wants to read the \else part! + \else% + \llap{\includegraphics[width=\paperwidth,height=\paperheight]{\beamer@Flip@watermark}} + \fi +} + + + +\mode +\endinput + + diff --git a/Seminars/India_IMSC_2018/beamerouterthemedecolines.sty b/Seminars/India_IMSC_2018/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/Seminars/India_IMSC_2018/beamerouterthemedecolines.sty @@ -0,0 +1,168 @@ +% Copyright 2007 by Marco Barisione +% +% This file may be distributed and/or modified +% +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. + +\mode + +% String used between the current page and the total page count. +\def\beamer@decolines@pageofpages{/} +\DeclareOptionBeamer{pageofpages}{\def\beamer@decolines@pageofpages{#1}} + +% Show a line below the frame title. +\DeclareOptionBeamer{titleline}[true]{\def\beamer@decolines@titleline{#1}} + +% Image used for the watermark. +\def\beamer@decolines@watermarkorig{} +\DeclareOptionBeamer{watermark}{\def\beamer@decolines@watermarkorig{#1}} + +% Height of the watermark. +\def\beamer@decolines@watermarkheight{100px} +\DeclareOptionBeamer{watermarkheight}{\def\beamer@decolines@watermarkheight{#1}} + +% The original image height is watermarkheightmult * watermarkheight. +\def\beamer@decolines@watermarkheightmult{1} +\DeclareOptionBeamer{watermarkheightmult}{\def\beamer@decolines@watermarkheightmult{#1}} + +\ExecuteOptionsBeamer{titleline=false} +\ProcessOptionsBeamer + +% Enable/disable the watermark. +\def\watermarkon{% + \def\beamer@decolines@watermark{\beamer@decolines@watermarkorig}% +} +\def\watermarkoff{\def\beamer@decolines@watermark{}} + +% Initially enable the watermark. +\watermarkon + +% Colors. +\setbeamercolor*{lineup}{parent=palette primary} +\setbeamercolor*{linemid}{parent=palette secondary} +\setbeamercolor*{linebottom}{parent=palette tertiary} +\setbeamercolor*{page header}{parent=titlelike} + +% Lengths +\newlength{\headerheight} +\setlength{\headerheight}{.045\paperheight} +\newlength{\beamer@decolines@lineup} +\setlength{\beamer@decolines@lineup}{.025\paperheight} +\newlength{\beamer@decolines@linemid} +\setlength{\beamer@decolines@linemid}{.015\paperheight} +\newlength{\beamer@decolines@linebottom} +\setlength{\beamer@decolines@linebottom}{.01\paperheight} + +% The height of the watermark part below the 3 bottom lines. +\newlength{\beamer@decolines@watermarkheightbottom} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@lineup} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linemid} +\addtolength{\beamer@decolines@watermarkheightbottom}{\beamer@decolines@linebottom} + +% The height of the watermark part over the 3 bottom lines before shrinking. +\newlength{\beamer@decolines@watermarkheightupperorig} +\setlength{\beamer@decolines@watermarkheightupperorig}{\beamer@decolines@watermarkheight} +\addtolength{\beamer@decolines@watermarkheightupperorig}{-\beamer@decolines@watermarkheightbottom} +\multiply\beamer@decolines@watermarkheightupperorig by \beamer@decolines@watermarkheightmult + +% % Footer. +% \defbeamertemplate*{footline}{decolines theme} +% { +% \leavevmode% +% % Page number. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=0ex,dp=0ex,center]{}% +% \usebeamerfont{palette primary}\insertframenumber{} \beamer@decolines@pageofpages{} \inserttotalframenumber% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=0ex,dp=0ex]{}% +% \end{beamercolorbox}% +% } % +% % First line. +% \hbox{% +% \begin{beamercolorbox}[wd=.2\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.8\paperwidth,ht=\beamer@decolines@lineup,dp=0pt]{lineup}% +% \end{beamercolorbox}% +% } % +% % Second line. +% \hbox{% +% \begin{beamercolorbox}[wd=\paperwidth,ht=\beamer@decolines@linemid,dp=0pt]{linemid}% +% \end{beamercolorbox}% +% } % +% % Third line. +% \hbox{% +% \begin{beamercolorbox}[wd=.1\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{}% +% \end{beamercolorbox}% +% \begin{beamercolorbox}[wd=.9\paperwidth,ht=\beamer@decolines@linebottom,dp=0pt]{linebottom}% +% \end{beamercolorbox}% +% }% +% % This seems to fix some alignment problems with the watermark. It has to be +% % always applied if you do not want to see the footer moving up and down when +% % moving from a page with watermark to a page without or vice versa. +% \vskip-.5px% +% % Watermark. +% \if\beamer@decolines@watermark\@empty\else% +% \vskip-\beamer@decolines@watermarkheightbottom% +% \llap{\includegraphics[height=\beamer@decolines@watermarkheightbottom,clip=true,% +% trim=0pt 0pt 0pt \beamer@decolines@watermarkheightupperorig]{\beamer@decolines@watermark}\hskip-\paperwidth}% +% \fi% +% } + +\defbeamertemplate*{headline}{decolines theme} +{ + \leavevmode% + \hbox{% + \begin{beamercolorbox}[wd=\paperwidth,ht=\headerheight,dp=0pt]{page header}% + \end{beamercolorbox}% + } % + \vskip0pt% +} + +\defbeamertemplate*{frametitle}{decolines theme}[1][left] +{ + \ifbeamercolorempty[bg]{frametitle}{}{\nointerlineskip}% + \@tempdima=\textwidth% + \advance\@tempdima by\beamer@leftmargin% + \advance\@tempdima by\beamer@rightmargin% + \vbox{}\vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[sep=\beamer@leftmargin,#1,wd=\the\@tempdima]{} + \usebeamerfont{frametitle}\usebeamercolor[bg]{framesubtitle}% + \vbox{}\vskip0ex% + \if@tempswa\else\csname beamer@fte#1\endcsname\fi% + \strut\insertframetitle\strut\par% + {% + \ifx\insertframesubtitle\@empty% + \else% + {\usebeamerfont{framesubtitle}\usebeamercolor[bg]{framesubtitle}\insertframesubtitle\strut\par}% + \fi + }% + \vskip-1ex% + \if@tempswa\else\vskip-\beamer@leftmargin\fi + \end{beamercolorbox}% + \def\beamer@decolines@truetext{true}% + \ifx\beamer@decolines@titleline\beamer@decolines@truetext% + \vskip-.5\beamer@leftmargin% + \begin{beamercolorbox}[wd=\textwidth,ht=.1ex,dp=0ex]{linemid}% + \end{beamercolorbox}% + \fi +} + +% Frame title continuations, default +\defbeamertemplate*{frametitle continuation}{decolines theme}{(\insertcontinuationcount)} + + + +\defbeamertemplate*{sidebar right}{decolines theme} +{ + \vskip.1\beamer@leftmargin% + \llap{\insertlogo\hskip.5\beamer@leftmargin}% + \vfill% + \if\beamer@decolines@watermark\@empty\else% + \llap{\includegraphics[height=\beamer@decolines@watermarkheight]{\beamer@decolines@watermark}}% + \vskip-\beamer@decolines@watermarkheightbottom% + \fi +} + +\mode + diff --git a/Seminars/India_IMSC_2018/beamerthemeFlip.sty b/Seminars/India_IMSC_2018/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/Seminars/India_IMSC_2018/beamerthemeFlip.sty @@ -0,0 +1,59 @@ +% Main style file for the BEAMER FLIP THEME 2012 +% Copyright 2012 by Flip Tanedo +% This file may be distributed and/or modified +% 1. under the LaTeX Project Public License and/or +% 2. under the GNU Public License. +% +% Comments: This is still a work in progress. +% A good way to present: http://www.cs.hmc.edu/~oneill/freesoftware/pdftokeynote.html + +% \usepackage{beamerthemesplit} +\mode + + +%% These are the options that are fed in through the driver file +%% Some of them get passed on to the other theme files +\DeclareOptionBeamer{bullet}{\PassOptionsToPackage{bullet=#1}{beamerinnerthemeFlip}} +\DeclareOptionBeamer{bigpagenumber}{\PassOptionsToPackage{bigpagenumber}{beamerouterthemeFlip}} +\DeclareOptionBeamer{topline}[true]{\PassOptionsToPackage{topline=#1}{beamerouterthemeFlip}} +\DeclareOptionBeamer{shadow}[false]{\PassOptionsToPackage{shadow=#1}{beamerinnerthemeFlip}} + +\DeclareOptionBeamer{watermark}{\PassOptionsToPackage{watermark=#1}{beamerouterthemeFlip}} + +\ProcessOptionsBeamer + +\useinnertheme{Flip} % Calls beamerinnerthemeFlip.sty +\useoutertheme{Flip} % Calls beamerouterthemeFlip.sty +\usecolortheme{Flip} % Calls beamercolorthemeFlip.sty + + + +%%%%%%%%%%%%%%%%%%%%%%%% +% Background Gradient % +%%%%%%%%%%%%%%%%%%%%%%%% + + +%% Usually I would leave this on +%% However, there seems to be problems with XeLaTeX +%% http://tex.stackexchange.com/questions/29497/xelatex-preventing-beamer-from-using-different-backgrounds +\setbeamertemplate{background canvas}[vertical shading][bottom=blue!.1, middle=white, top=white] + +%% HOWEVER: it seems to make it impossible to change this later on in the document + + +%% For a dark background: +% \setbeamertemplate{background canvas}[vertical shading][bottom=keynotebottom, middle=keynotemiddle, top=keynotetop] + + +%% An alternate way: \beamertemplateshadingbackground{blue!.1}{red!2} +%% In general: you want the gradient to be subtle! + + +%%%%%%%%%%%%%%%%%%%%%%% +% Navigation symbols % +%%%%%%%%%%%%%%%%%%%%%%% + +\setbeamertemplate{navigation symbols}{} % Turns off PDF navigation symbols + +\mode +\endinput \ No newline at end of file diff --git a/Seminars/India_IMSC_2018/distracted_ilissa-ocko-cartoon.jpg b/Seminars/India_IMSC_2018/distracted_ilissa-ocko-cartoon.jpg new file mode 100644 index 0000000..5f007b0 --- /dev/null +++ b/Seminars/India_IMSC_2018/distracted_ilissa-ocko-cartoon.jpg Binary files differ diff --git a/Seminars/India_IMSC_2018/images/1.png b/Seminars/India_IMSC_2018/images/1.png new file 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Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% + +\def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} + +\usepackage{gmp} +\usepackage[final]{feynmp-auto} + +\usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} +\bibliography{bib} +\setbeamertemplate{bibliography item}[text] + +\makeatletter\let\frametextheight\beamer@frametextheight\makeatother + +% suppress frame numbering for backup slides +% you always need the appendix for this! +\newcommand{\backupbegin}{ + \newcounter{framenumberappendix} + \setcounter{framenumberappendix}{\value{framenumber}} +} +\newcommand{\backupend}{ + \addtocounter{framenumberappendix}{-\value{framenumber}} + \addtocounter{framenumber}{\value{framenumberappendix}} +} + + +\definecolor{links}{HTML}{2A1B81} +%\hypersetup{colorlinks,linkcolor=,urlcolor=links} + +% For shapo's formulas: +\def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} +\newcommand{\lsim}{\mathop{\lsi}} +\newcommand{\gsim}{\mathop{\gsi}} +\newcommand{\wt}{\widetilde} +%\newcommand{\ol}{\overline} +\newcommand{\Tr}{\rm{Tr}} +\newcommand{\tr}{\rm{tr}} +\newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} +\newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} +\newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} +\newcommand{\eV}{\rm{eV}} +\newcommand{\keV}{\rm{keV}} +\newcommand{\GeV}{\rm{GeV}} +\newcommand{\MeV}{\rm{MeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\re}{{\rm Re}} +\newcommand{\invfb}{\rm{fb^{-1}}} +\newcommand{\fixme}{\rm{{\color{red}{FIXME!}}}} +\newcommand{\thetal}{\theta_l} +\newcommand{\thetak}{\theta_k} +\newcommand{\nn}{\nonumber} +\newcommand{\eq}[1]{\begin{equation} #1 \end{equation}} +%\newcommand{\eqn}[1]{\begin{displaymath} #1 \end{displaymath}} +\newcommand{\eqa}[1]{\begin{eqnarray} #1 \end{eqnarray}} +\newcommand{\apeL}{{A_\perp^L}} +\newcommand{\apeR}{{A_\perp^R}} +\newcommand{\ape}{{A_\perp}} +\newcommand{\apeLR}{{A_\perp^{L,R}}} +\newcommand{\apaL}{{A_\|^L}} +\newcommand{\apaR}{{A_\|^R}} +\newcommand{\apa}{{A_\|}} +\newcommand{\apaLR}{{A_\|^{L,R}}} +\newcommand{\azeL}{{A_0^L}} +\newcommand{\azeR}{{A_0^R}} +\newcommand{\aze}{{A_0}} + +\newcommand{\azeLR}{{A_0^{L,R}}} +\newcommand{\Real}{\ensuremath{\mathcal{R}e}\xspace} +\newcommand{\Imag}{\ensuremath{\mathcal{I}m}\xspace} + +\renewcommand{\C}[1]{{\cal C}_{#1}} +\newcommand{\Ceff}[1]{{\cal C}^{\rm eff}_{#1}} +\newcommand{\Cpeff}[1]{{\cal C}^{\rm eff\prime}_{#1}} +\newcommand{\Cp}[1]{{\cal C}^{\prime}_{#1}} +\def\FL {\ensuremath{F_{\mathrm{L}}}\xspace} +\def\ATDPH {\ensuremath{A_{\mathrm{T,PR}}^{(2)}}\xspace} +\def\ATImPH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Im}}}\xspace} +\def\ATRePH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Re}}}\xspace} +\def\FLPH {\ensuremath{F_{\mathrm{L,PR}}}\xspace} +\def\ATDKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{(2)}}\xspace} +\def\ATImKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Im}}}\xspace} +\def\ATReKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Re}}}\xspace} +\def\FLKG {\ensuremath{F_{\mathrm{L,\Kstarz \gamma}}}\xspace} +\def\ATD {\ensuremath{A_{\mathrm{T}}^{(2)}}\xspace} +\def\ATIm {\ensuremath{A_{\mathrm{T}}^{\mathrm{Im}}}\xspace} +\def\ATRe {\ensuremath{A_{\mathrm{T}}^{\mathrm{Re}}}\xspace} +\def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} + + + +\def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} + + + +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\mathcal{B}}} + +\newcommand{\av}[1]{\langle #1 \rangle} +% particles +\def\LstFTTT {\ensuremath{\PLambda^{*}(1520)^{0}}\xspace} +\def\dll {\ensuremath{\mathrm{DLL}}\xspace} + \def\Lb {\ensuremath{\PLambda_b}} + + +% useful decays +\def\BdToKpimm {\decay{\Bd}{\Kp\pim\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsToJPsiKst {\decay{\Bs}{\jpsi\Kstarz}} +\def\BdTopsitwosKst {\decay{\Bd}{\psitwos\Kstarz}} +\def\LstFTTTT {\decay{\LstFTTT}{p\Km}} +%\def\LbToLstmm {\decay{\Lb}{\PLambda^{*}(1520)^{0} \mumu}} +\def\LbTopKmm {\decay{\Lb}{p\Km\mumu}} +\def\BuToKmm {\decay{\Bu}{\Kp\mumu}} +\def\BsTophimm {\decay{\Bs}{\Pphi\mumu}} + +% interesting variables +\def\mkpi {\ensuremath{m_{K\pi}}\xspace} +\def\mkpimm{\ensuremath{m_{K\pi\mu\mu}}\xspace} + +%% peaking background mass hypotheses +\def\mkmm {\ensuremath{m_{K\mu\mu}}\xspace} +\def\mSwappKmm {\ensuremath{m_{(\pi\to p)K\mu\mu}}\xspace} +\def\mSwappiK {\ensuremath{m_{(\pi\to K)K}}\xspace} +\def\mSwappiKmm {\ensuremath{m_{(\pi\to K)K\mu\mu}}\xspace} +\def\mSwappK {\ensuremath{m_{(\pi\to p)K}}\xspace} +\def\mDoubleSwappKmm {\ensuremath{m_{(K\to p)(\pi\to K)\mu\mu}}\xspace} +\def\mDoubleSwappK {\ensuremath{m_{(K\to p)(\pi\to K)}}\xspace} +\def\mSwapKst {\ensuremath{m_{K\leftrightarrow\pi}}\xspace} + +%% some other decays +\def\BsToPhimm {\decay{\Bs}{\phi\mumu}} +\def\BsToPhimmFULL {\decay{\Bs}{\phi(\to\!K^{+}K^{-})\mumu}} +\def\BsToKKmm {\decay{\Bs}{\Kp\Km\mumu}} + +\newcommand{\delC}[1]{\delta {\cal C}_{#1}} +\newcommand{\dC}[1]{{\cal C}_{#1}^{\rm NP}} +\newcommand{\dCp}[1]{{\cal C}_{#1^\prime}^{\rm NP}} + + + + +\definecolor{green}{rgb}{0.2,0.6,0.2} +\definecolor{lightgreen}{rgb}{0.4,1,0.4} +\definecolor{verylightgreen}{rgb}{0.7,1,0.7} +\def\cgreen{\color{green}} +\definecolor{brown}{rgb}{0.4,0.2,0.0} +\def\cbrown{\color{brown}} +\def\cred{\color{red}} +\definecolor{darkblue}{rgb}{0.0,0.0,1.0} +\def\cdarkblue{\color{darkblue}} +\definecolor{darkgrey}{rgb}{0.4,0.4,0.4} +\definecolor{lightgrey}{rgb}{0.7,0.7,0.7} +\definecolor{verylightblue}{rgb}{0.8,0.8,1.0} +\definecolor{lightblue}{rgb}{0.6,0.6,1.0} +\definecolor{verylightyellow}{rgb}{1.0,1.0,0.5} +\definecolor{lightyellow}{rgb}{1.0,0.7,0.3} +\definecolor{darkred}{rgb}{0.6,0.0,0.0} + +\definecolor{green}{rgb}{0.3,0.6,0.2} +\definecolor{green}{rgb}{0.3,0.7,0.4} + + + +\definecolor{indigo}{RGB}{100,0,100} +\definecolor{dgray}{RGB}{80,80,80} +\definecolor{lgray}{RGB}{220,220,220} +\definecolor{dred}{RGB}{190,0,0} +\definecolor{dgreen}{RGB}{0,110,0} +\definecolor{lyellow}{RGB}{245,245,210} +\definecolor{bblue}{RGB}{93,93,255} +\definecolor{bbrown}{RGB}{150,85,52} +\definecolor{llgray}{RGB}{230,230,230} + + + +\newcommand{\F}{\mathcal{F}} +\newcommand{\A}{\mathcal{A}} +\newcommand{\N}{\mathcal{N}} +\renewcommand{\H}{\mathcal{H}} +\newcommand{\Leff}{\mathcal{L}_{\rm eff}} +\newcommand{\heff}{\mathcal{H}_{\rm eff}} +\newcommand{\Lag}{\mathcal{L}} +\newcommand{\red}{\color{red}} +\newcommand{\blue}{\color{blue}} +\newcommand{\indigo}{\color{indigo}} +\newcommand{\brown}{\color{bbrown}} +\newcommand{\bs}{\mathbf} +\newcommand{\sss}{\scriptscriptstyle} +\newcommand{\btr}{{ $\blacktriangleright\ $}} + + +\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (CERN, IFJ PAN)} +\institute{UZH} +\title[Anomalies in Physics]{Anomalies in Physics} +\date{25 September 2014} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.9\textwidth} + \flushright\fontspec{Trebuchet MS}\bfseries \Huge {Anomalies in Physics or Physics of anomalies?} + \end{column} + \begin{column}{0.2\textwidth} + %\includegraphics[width=\textwidth]{SHiP-2} + \end{column} + \end{columns} +\end{center} + \quad + \vspace{3em} +\begin{columns} +\begin{column}{0.44\textwidth} +\flushright \vspace{-1.8em} {\fontspec{Trebuchet MS} \Large Marcin Chrząszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +\end{column} +\begin{column}{0.53\textwidth} +\includegraphics[height=1.3cm]{cern}{~}{~} +\includegraphics[height=1.1cm]{ifj.png} +\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + \textcolor{normal text.fg!50!Comment}{IMSc seminar \\July 24, 2018} +\end{center} +\end{frame} +} + + +\begin{frame}{Outline} + + \begin{minipage}{\textwidth} +{~}\\ + +\begin{enumerate} +\item Why flavour is important. +\item The flavour anomalies: +\begin{itemize} +\item $R(\PDstar)$ +\item $R_K$ and $R_{\PKstar}$ +\item $P_5^{\prime}$ +\end{itemize} +\item Global fits results. +\item Conclusions. +\end{enumerate} + + + \end{minipage} + \vspace*{2.cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Why flavour physics +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +Why Flavour is important? +\end{Huge} +\end{center} + + + + +\end{frame} + + + +\begin{frame}{A lesson from history - GIM mechanism} + \begin{minipage}{\textwidth} + +\begin{center} +\includegraphics[width=0.62\textwidth]{images/GIM2.png} +\end{center} +\begin{columns} +\column{0.7\textwidth} +\begin{itemize} +\begin{footnotesize} + + +\item Cabibbo angle was successful in explaining dozens of decay rates in the 1960s. +\item There was, however, one that was not observed by experiments: $\PKzero \to \Pmuon \APmuon$. +\item Glashow, Iliopoulos, Maiani (GIM) mechanism was proposed in the 1970 to fix this problem. The mechanism required the existence of a $4^{th}$ quark. +\item At that point most of the people were skeptical about that. Fortunately in 1974 the discovery of the $\PJpsi$ meson silenced the skeptics. +\end{footnotesize} +\end{itemize} +\column{0.3\textwidth} +\begin{center} +\includegraphics[width=0.95\textwidth]{images/GIM3.png}\\ +\includegraphics[width=0.7\textwidth]{images/604.jpg}\\{~}\\{~} +\end{center} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + +\begin{frame}{A lesson from history - CKM matrix} + \begin{minipage}{\textwidth} + +\begin{center} +{~}\\{~}\\ +\includegraphics[width=0.5\textwidth]{images/CKMmatrix.png} + +\end{center} +\begin{columns} +\column{0.6\textwidth} +\begin{itemize} +\begin{small} + + + + +\item Similarly, CP violation was discovered in 1960s in the neutral kaons decays. +\item $2 \times 2$ Cabbibo matrix could not allow for any CP violation. +\item For CP violation to be possible one needs at least a $3 \times 3$ unitary matrix \\ $\looparrowright$ Cabibbo-Kobayashi-Maskawa matrix (1973). +\item It predicts existence of $\Pbottom$ (1977) and $\Ptop$ (1995) quarks. +\end{small} + +\end{itemize} +\column{0.4\textwidth} +\begin{center} +{~} +%\includegraphics[height=2cm]{images/CP.png}\\ +\includegraphics[width=0.96\textwidth]{bottom.jpg} + +\end{center} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{A lesson from history - Weak neutral current} + \begin{minipage}{\textwidth} + +\begin{center} +\includegraphics[height=3cm]{images/weakcurr.png}{~} +\includegraphics[height=3cm]{images/weakcurr2.png} +\end{center} + +\begin{columns} +\column{0.6\textwidth} +\begin{itemize} +\begin{small} + + +\item Weak neutral currents were first introduced in 1958 by Buldman. +\item Later on they were naturally incorporated into unification of weak and electromagnetic interactions. +\item 't Hooft proved that the GWS models was renormalizable. +\item Everything was there on theory side, only missing piece was the experiment, till 1973. +\end{small} + +\end{itemize} +\column{0.4\textwidth} +\begin{center} +{~} +%\includegraphics[height=2cm]{images/CP.png}\\ +\includegraphics[width=0.85\textwidth]{images/bubblecern.png} +\end{center} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + + + +\iffalse + + + +\begin{frame} +\begin{center} +\begin{Huge} +LHCb detector +\end{Huge} +\end{center} + + + + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% DETECTOR +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\only<1>{\frametitle{LHCb detector - tracking} +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/sketch.png} +\end{columns} +\begin{itemize} +\item Excellent Impact Parameter (IP) resolution ($20~\rm \mu m$).\\ +$\Rightarrow$ Identify secondary vertices from heavy flavour decays +\item Proper time resolution $\sim~40~\rm fs$.\\ +$\Rightarrow$ Good separation of primary and secondary vertices. +\item Excellent momentum ($\delta p/p \sim 0.4 - 0.6\%$) and inv. mass resolution.\\ +$\Rightarrow$ Low combinatorial background. + +\end{itemize} + + +} + +\only<2>{\frametitle{LHCb detector - particle identification} +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{images/cher.png} +\end{columns} +\begin{itemize} +\item Excellent Muon identification $\epsilon_{\mu \to \mu} \sim 97\%$, $\epsilon_{\pi \to \mu} \sim 1-3\%$ +\item Good $\PK-\Ppi$ separation via RICH detectors, $\epsilon_{\PK \to \PK} \sim 95\%$, $\epsilon_{\Ppi \to \PK} \sim 5\%$.\\ +$\Rightarrow$ Reject peaking backgrounds. +\item High trigger efficiencies, low momentum thresholds. +Muons: $p_T > 1.76 \GeV$ at L0, $p_T > 1.0 \GeV$ at HLT1,\\ +$B \to \PJpsi X $: Trigger $\sim 90\%$. + +\end{itemize} + + +} + + +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Modern challenges: loops come in to the game} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\item Standard Model contributions suppressed or absent: +\begin{itemize} +\item Flavour Changing Neutral Currents. +\item CP violation +\item Lepton Flavour/Number or Lepton Universality violation. +\end{itemize} +\item In general can probe physics beyond General Purpose Detectors reach. +\end{itemize} +\column{0.5\textwidth} +\includegraphics[width=0.99\textwidth]{{images/TauLFV_UL_2014001_averaged}.png} + + +\end{columns} +\begin{center} +\includegraphics[width=0.75\textwidth]{images/Bsmumu.png} +\includegraphics[width=0.20\textwidth]{{images/bsmumu_SM}.png} +\end{center} +\end{minipage} + + \vspace*{2.1cm} +\end{frame} +\fi + + + + + +\begin{frame}\frametitle{Modern Flavour Physics} +\begin{center} +\only<1>{ +\includegraphics[width=1.05\textwidth]{1.png} +} +\only<2>{ +\includegraphics[width=1.05\textwidth]{2.png} + +} +\end{center} + + + + +\end{frame} + + +\begin{frame}\frametitle{Why semi-leptonic decays?} +\begin{large} +\ARROW A decay is semi-leptonic if its products are part leptons +and part hadrons. +\end{large} + +\begin{center} +\includegraphics[width=0.99\textwidth]{3.png} +\end{center} + +\begin{large} +\ARROW These decays can be factorised into the weak and +strong parts, greatly simplifying theoretical calculations. +\end{large} + + +\end{frame} + + + +\begin{frame}\frametitle{Types of semi-leptonic decays} + +\begin{center} +\includegraphics[width=1.05\textwidth]{4.png} +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Anomalies} +\only<1>{ +\begin{center} +\includegraphics[width=1.05\textwidth]{6.png} +\end{center} +} +\only<2>{ +\ARROW Today I will talk about three anomalies in $\PB$ +decays: +\begin{itemize} +\item $R(\PDstar)$ +\item $R_{\PK/\PKstar}$ +\item $P^{\prime}_5$ +\end{itemize} + +} + +\end{frame} + + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 1\\ +\begin{align*} +R(\PDstar) = \frac{\Br (\PB \to \PDstar \tau \nu )}{\Br(\PB \to \PDstar \mu \nu)} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + +\begin{frame}\frametitle{$R(\PDstar) $} + +\begin{large} + +\ARROW Large rate of charged current decays allow for measurement +in semi-tauonic decays +\end{large} + +\begin{columns} +\column{0.5\textwidth} +\begin{align*} +R(\PDstar) = \frac{\Br (\PB \to \PDstar \tau \nu )}{\Br(\PB \to \PDstar \mu \nu)} +\end{align*} +\column{0.5\textwidth} +\begin{large} +\ARROW Form ratio of decays with different lepton generations.\\ +\ARROW Cancel QCD uncertainties. +\end{large} + +\end{columns} +~\\ +\begin{large} + +\ARROW $R(\PDstar)$ is sensitive to the NP with strong 3rd generation couplings. +\end{large} + +\includegraphics[width=0.8\textwidth]{images/7.png} + + +\end{frame} + +\begin{frame}\frametitle{The Rule of three} + +\begin{center} + +\includegraphics[width=1.\textwidth]{images/8.png} + +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Experimental challenges} +\begin{large} +\ARROW With the $\tau \to \mu \nu \nu$ decay we are missing 3 neutrinos!\\ +\ARROW No sharp peak in any distributions.\\ +\end{large} +{~}\\ +\begin{columns} +\column{0.5\textwidth} +\begin{large} +\ARROW At B-factories, can control this +using tagging technique.\\ +\end{large} + + +\includegraphics[width=0.9\textwidth]{9.png} + +\column{0.5\textwidth} + + +\includegraphics[width=0.9\textwidth]{10.png}\\ +\begin{large} +\ARROW More difficult at LHCb, compensate +using large boost (flight information) +and huge B production\\ +\end{large} +\end{columns} + +\end{frame} + +\begin{frame}\frametitle{Signal fits} +\ARROW Three main backgrounds: +\begin{itemize} +\item $\PB \to \PDstar \ell \nu$. +\item $\PB \to \PD^{\ast \ast} \ell \nu$. +\item $\PB \to \PD \PDstar X$ +\end{itemize} +\begin{center} +\includegraphics[width=0.9\textwidth]{12.png} +\end{center} +\ARROW Fit variables which discriminate between the signal and background modes. + +\end{frame} + +\begin{frame}\frametitle{Results} +\ARROW All experiments see an access w.r.t. to SM prediction: +\begin{center} +\includegraphics[angle=-90,width=0.6\textwidth]{rdrds_summer18.pdf} +\end{center} +\ARROW Theoretical uncertainties negligible.\\ +\ARROW The ball is on the experimental side. + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + + +\begin{frame}\frametitle{Introduction to anomaly 2 \& 3} + +\begin{columns} +\column{4in} +\begin{itemize} +\item The SM allows only the charged interactions to change flavour. +\begin{itemize} +\item Other interactions are flavour conserving. +\end{itemize} +\item One can escape this constraint and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. +\begin{itemize} +\item These kind of processes are suppressed in SM $\to$~Rare decays. +\item New Physics can enter in the loops. +\end{itemize} +\end{itemize} +\begin{center} +\includegraphics[scale=0.3]{lupa.png} +\includegraphics[scale=0.3]{example.png} +\end{center} +\column{1.5in} +\includegraphics[width=0.61\textwidth]{couplings.png} +\end{columns} + +\end{frame} + + +\begin{frame}{Analysis of Rare decays} +\begin{footnotesize} + +%{\Large Since a long time ago...} \\ \medskip +%\hspace*{1.4cm}$\Rightarrow$ $b \to s \gamma$ and $b \to s \ell\ell $ {\bf Flavour Changing Neutral Currents} have been used as {\bf \cred Our Portal} \\ to explore the fundamental theory beyond SM. \\ +%\medskip +%\medskip +%\hfill....... with not much success till 2013.\hspace*{1cm} +%\bigskip + +Analysis of FCNC in a model-independent approach, effective Hamiltonian: +\vspace*{-0.1cm} +\begin{columns} +\begin{column}{1cm} +~ +\end{column} +\begin{column}{8cm} +\begin{equation*} +b\to s\gamma(^*): {\mathcal H}^{SM}_{\Delta F=1} \propto + \sum_{i=1}^{10} V_{ts}^* V_{tb} {\cgreen \C{i}} \alert{ {\cal O}_i} + \ldots +\end{equation*} + +\vspace{-0.2cm} + +\begin{itemize} +\item $\alert{ {\cal O}_7} = \frac{e}{16 \pi^2}m_b\, + (\bar s\sigma^{\mu\nu} P_R b) F_{\mu\nu}\,$ %\quad [real or soft photon] +\item $\alert{ {\cal O}_9}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b)\ (\bar\ell\gamma_\mu\ell)$ + %\quad [$b\to s\mu\mu$ via $Z$/hard $\gamma$] +\item $\alert{ {\cal O}_{10}}=\frac{e^2}{16 \pi^2}(\bar{s}\gamma_\mu P_L b) \ (\bar\ell\gamma_\mu\gamma_5\ell)$, ... +%\quad [$b\to s\mu\mu$ via $Z$] +\end{itemize} +\end{column} +\begin{column}{5.5cm} +\includegraphics[width=3.5cm]{images/qum1.png} +%\includegraphics[width=3cm]{bsll.pdf} +\end{column} +\end{columns} + +%\hspace*{5cm} with no clear success yet... +%\bigskip + + +%\centerline{{\bf Goal}: \underline{Decode the short distance physics to find a smoking gun of BSM}\hspace*{2cm}} + + +\bigskip +\hspace*{0.0cm} $\bullet$ {\bf SM} Wilson coefficients up to NNLO + e.m. corrections at $\mu_{ref}=4.8$ GeV [{\cgreen Misiak et al.}]: $${\cal C}_7^{\rm SM}=-0.29,\, {\cal C}_9^{\rm SM}=4.1,\, {\cal C}_{10}^{\rm SM}=-4.3$$ +%BUT, like in the film there is always the good, the bad and the ugly. +\bigskip +$\bullet$ {\bf NP} changes short distance ${\cal C}_i-{\cal C}_i^{\rm SM}={\cal C}_i^{\rm NP}$ and induce new operators, like ${\cal O}^\prime_{7,9,10}={\cal O}_{7,9,10}\,\, (P_L \leftrightarrow P_R)$ ... also scalars, pseudoescalar, tensor operators...%\bigskip + + +\end{footnotesize} + +\end{frame} + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 2\\ +\begin{align*} +R_{\PK/\PKstar} = \frac{\Br(\PB \to \PK/\PKstar \mu \mu)}{\Br(\PB \to \PK/\PKstar e e)} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + + + +\begin{frame}\frametitle{Measurement at LHCb} + +\ARROW Most precise measurements performed at LHCb.\\ +\ARROW Main challenge is due to electron Bremsstrahlung.\\ +\begin{center} +\includegraphics[width=0.99\textwidth]{13.png} +\end{center} +\ARROW To protect ourself from electron reconstruction issue we use double ratio: +\begin{align*} +R_K = \frac{ \Br(\PB \to \PK \mu \mu ) \times \Br(\PB \to \PK \PJpsi(\to e e)) }{ \Br(\PB \to \PK e e ) \times \Br(\PB \to \PK \PJpsi(\to \mu \mu)) } +\end{align*} + + +\end{frame} + + +\begin{frame}\frametitle{Result} + +\begin{center} +\begin{large} +\begin{align*} +R_K = 0.745^{+0.090}_{-0.074} ({\rm stat.}) \pm 0.036 ({\rm syst}) +\end{align*} +\end{large} + +\includegraphics[width=0.7\textwidth]{images/RK.png}\\ + +\end{center} +\ARROW $2.6~\sigma$ away from SM prediction. +\end{frame} + +\begin{frame}\frametitle{The continuation - $R_{\PKstar}$} +\ARROW The neutral continuation of the $R_K$ measurement is to measure its partner: +\begin{center} +\begin{align*} +R_{\PKstar} = \frac{\Br(\PB \to \PKstar \mu \mu)}{\Br(\PB \to \PKstar e e)} +\end{align*} +\end{center} + + +\begin{columns} +\column{0.4\textwidth} +\ARROW Measurement performed in two $q^2$ bins. \\ +\ARROW Normalized in double ratio to $\PB \to \PKstar \PJpsi$.\\ +\includegraphics[width=0.95\textwidth]{images/plot.png} + + +\column{0.6\textwidth} +\begin{center} +\includegraphics[width=0.95\textwidth]{Fig10a.pdf} +\end{center} + +\end{columns} + + + +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PB \to \PKstar^{\pm} \Pmu \Pmu$} +{~} +\includegraphics[width=0.5\textwidth]{images/ksmumu_BF.png} +\includegraphics[width=0.5\textwidth]{images/kmumu_BF.png} + +\begin{center} +\begin{columns} + +\column{0.4\textwidth} +\begin{itemize} +\item Despite large theoretical errors the results are consistently smaller than SM prediction. +\end{itemize} +\column{0.6\textwidth} +\includegraphics[width=0.87\textwidth]{images/bukst_BF.png} + + +\end{columns} + + + + + + + +\end{center} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PBs \to \Pphi \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[width=0.65\textwidth]{images/bs2phipi.png}\\ + \end{center} + +\begin{itemize} +\item Recent LHCb measurement [JHEPP09 (2015) 179]. +\item Suppressed by $\frac{f_s}{f_d}$. +\item Cleaner because of narrow $\Pphi$ resonance. +\item $3.3~\sigma$ deviation in SM in the $1-6\GeV^2$ bin. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + + + + +\begin{frame} + +\begin{center} + +\begin{Huge} +Anomaly 3\\ +\begin{align*} +P_5^{\prime} = \sqrt{2} \frac{\Re (\apeL \apaL^{\ast} - \apeR \apaR^{\ast} )}{\sqrt{ |\aze|^2 ( |\ape|^2 + |\aze|^2 )}} +\end{align*} +\end{Huge} + + +\end{center} + + +\end{frame} + + +%\azeLR +%\apaLR +%\apeLR + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{$\PBzero \to \PKstar \Pmuon \APmuon$ kinematics} +{~} + \begin{minipage}{\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ The kinematics of $\PBzero \to \PKstar \Pmuon \APmuon$ decay is described by three angles $\thetal$, $\thetak$, $\phi$ and invariant mass of the dimuon system ($q^2)$. + + \only<1>{ +\begin{columns} +\column{0.5\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ $\cos \thetak$: the angle between the direction of the kaon in the $\PKstar$ ($\overline{\PKstar}$) rest frame and the direction of the $\PKstar$ ($\overline{\PKstar}$) in the $\PBzero$ ($\APBzero$) rest frame.\\ +$\color{JungleGreen}{\Rrightarrow}$ $\cos \thetal$: the angle between the direction of the $\Pmuon$ ($\APmuon$) in the dimuon rest frame and the direction of the dimuon in the $\PBzero$ ($\APBzero$) rest frame.\\ +$\color{JungleGreen}{\Rrightarrow}$ $\phi$: the angle between the plane containing the $\Pmuon$ and $\APmuon$ and the plane containing the kaon and pion from the $\PKstar$. + + + +\column{0.5\textwidth} +\includegraphics[width=0.95\textwidth]{images/angles.png} + +\end{columns} + } + \only<2>{ +{\tiny{ +\eqa{\label{dist} +\frac{d^4\Gamma}{dq^2\,d\!\cos\theta_K\,d\!\cos\theta_l\,d\phi}&=&\frac9{32\pi} \bigg[ +J_{1s} \sin^2\theta_K + J_{1c} \cos^2\theta_K + (J_{2s} \sin^2\theta_K + J_{2c} \cos^2\theta_K) \cos 2\theta_l\nn\\[1.5mm] +&&\hspace{-2.7cm}+ J_3 \sin^2\theta_K \sin^2\theta_l \cos 2\phi + J_4 \sin 2\theta_K \sin 2\theta_l \cos\phi + J_5 \sin 2\theta_K \sin\theta_l \cos\phi \nn\\[1.5mm] +&&\hspace{-2.7cm}+ (J_{6s} \sin^2\theta_K + {J_{6c} \cos^2\theta_K}) \cos\theta_l ++ J_7 \sin 2\theta_K \sin\theta_l \sin\phi + J_8 \sin 2\theta_K \sin 2\theta_l \sin\phi \nn\\[1.5mm] +&&\hspace{-2.7cm}+ J_9 \sin^2\theta_K \sin^2\theta_l \sin 2\phi \bigg]\,, +\nonumber} +}} +$\color{JungleGreen}{\Rrightarrow}$ This is the most general expression of this kind of decay.\\ +\pause +\begin{exampleblock}{Credit where it belongs} +First time this eq. was written by prof. R. Sinha in 1996! \href{https://arxiv.org/pdf/hep-ph/9907386.pdf}{hep-ph/9608314} +\end{exampleblock} + + + +} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Transversity amplitudes } +{~} + \begin{minipage}{\textwidth} + +$\color{JungleGreen}{\Rrightarrow}$ One can link the angular observables to transversity amplitudes +{\tiny{ +\eqa{ +J_{1s} & = & \frac{(2+\beta_\ell^2)}{4} \left[|\apeL|^2 + |\apaL|^2 +|\apeR|^2 + |\apaR|^2 \right] + + \frac{4 m_\ell^2}{q^2} \re\left(\apeL\apeR^* + \apaL\apaR^*\right)\,,\nn\\[1mm] +% +J_{1c} & = & |\azeL|^2 +|\azeR|^2 + \frac{4m_\ell^2}{q^2} \left[|A_t|^2 + 2\re(\azeL^{}\azeR^*) \right] + \beta_\ell^2\, |A_S|^2 \,,\nn\\[1mm] +% +J_{2s} & = & \frac{ \beta_\ell^2}{4}\left[ |\apeL|^2+ |\apaL|^2 + |\apeR|^2+ |\apaR|^2\right], +\hspace{0.92cm} J_{2c} = - \beta_\ell^2\left[|\azeL|^2 + |\azeR|^2 \right]\,,\nn\\[1mm] +% +J_3 & = & \frac{1}{2}\beta_\ell^2\left[ |\apeL|^2 - |\apaL|^2 + |\apeR|^2 - |\apaR|^2\right], +\qquad J_4 = \frac{1}{\sqrt{2}}\beta_\ell^2\left[\re (\azeL\apaL^* + \azeR\apaR^* )\right],\nn \\[1mm] +% +J_5 & = & \sqrt{2}\beta_\ell\,\Big[\re(\azeL\apeL^* - \azeR\apeR^* ) - \frac{m_\ell}{\sqrt{q^2}}\, +\re(\apaL A_S^*+ \apaR^* A_S) \Big]\,,\nn\\[1mm] +% +J_{6s} & = & 2\beta_\ell\left[\re (\apaL\apeL^* - \apaR\apeR^*) \right]\,, +\hspace{2.25cm} J_{6c} = 4\beta_\ell\, \frac{m_\ell}{\sqrt{q^2}}\, \re (\azeL A_S^*+ \azeR^* A_S)\,,\nn\\[1mm] +% +J_7 & = & \sqrt{2} \beta_\ell\, \Big[\im (\azeL\apaL^* - \azeR\apaR^* ) + +\frac{m_\ell}{\sqrt{q^2}}\, \im (\apeL A_S^* - \apeR^* A_S)) \Big]\,,\nn\\[1mm] +% +J_8 & = & \frac{1}{\sqrt{2}}\beta_\ell^2\left[\im(\azeL\apeL^* + \azeR\apeR^*)\right]\,, +% +\hspace{1.9cm} J_9 = \beta_\ell^2\left[\im (\apaL^{*}\apeL + \apaR^{*}\apeR)\right] \,, +\label{Js}\nonumber} +}} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Link to effective operators} +{~} + \begin{minipage}{\textwidth} +$\color{JungleGreen}{\Rrightarrow}$ So here is where the magic happens. At leading order the amplitudes can be written as: +{\tiny{ +\eqa{ +\apeLR &=&\sqrt{2} N m_B(1- \hat s)\bigg[ (\Ceff9 + \Cpeff9) \mp (\C{10} + \Cp{10}) ++\frac{2\hat{m}_b}{\hat s} (\Ceff7 + \Cpeff7) \bigg]\xi_{\bot}(E_{K^*}) \nn \\[2mm] +\apaLR &=& -\sqrt{2} N m_B (1-\hat s)\bigg[(\Ceff9 - \Cpeff9) \mp (\C{10} - \Cp{10}) ++\frac{2\hat{m}_b}{\hat s}(\Ceff7 - \Cpeff7) \bigg] \xi_{\bot}(E_{K^*}) \nn \\[2mm] +\azeLR &=& -\frac{N m_B (1-\hat s)^2}{2 \hat{m}_{K^*} \sqrt{\hat s}} \bigg[ (\Ceff9 - \Cpeff9) \mp (\C{10} - \Cp{10}) + 2\hat{m}_b (\Ceff7 - \Cpeff7) \bigg]\xi_{\|}(E_{K^*}), +\label{LargeRecoilAs}\nonumber} +}} +where $\hat s = q^2 /m_B^2$, $\hat{m}_i = m_i/m_B$. The $\xi_{\|,\bot }$ are the form factors. \\ +\pause +$\color{JungleGreen}{\Rrightarrow}$ Now we can construct observables that cancel the $\xi$ form factors at leading order: +\eq{P_5^{\prime} = \dfrac{J_5+\bar{J}_5}{2\sqrt{-(J_2^c+\bar{J}_2^c)(J_2^s+\bar{J}_2^s)} }\nonumber +} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +\begin{center} +\begin{Huge} +LHCb measurement of $\PBd \to \PKstar \Pmu \Pmu$ +\end{Huge} +\end{center} + + + + +\end{frame} +\iffalse + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{LHCbs $\PBzero \to \PKstar \Pmuon \APmuon$, Selection} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\begin{columns} +\column{0.2in} +{~} +\column{2in} +\ARROW Trigger +\begin{itemize} +\item Muon trigger. +\item Topological trigger. +\end{itemize} +\ARROW Good modelling with MC. \\ +\ARROW Selection: +\begin{itemize} +\item As loose as possible. +\item Based on the $\PBzero$ vertex quality, impact parameters, loose Particle identification for the hadrons. +\item The variables were chosen in a way we are sure the are correctly modelled in MC. +\end{itemize} +\column{2.8in} + +\includegraphics[angle=-90,width=0.75\textwidth]{{images/tistos_L0Muon_pt}.pdf}\\ +\includegraphics[angle=-90,width=0.75\textwidth]{{images/tistos_L0Muon_costhetal}.pdf} +\end{columns} + + + +\end{footnotesize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Peaking backgrounds} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\ARROW A number of peaking backgrounds that can mistaken as your signal.\\ +\ARROW There where a specially designed vetoes to fight each of them. +\begin{center} +\begin{tiny} +\hspace{-1cm}\begin{tabular}{ r | c c | c c } + \hline + & \multicolumn{2}{c|}{after preselection, before vetoes} & \multicolumn{2}{c }{after vetoes and selection}\\ + Channel & Estimated events & \% signal & Estimated events & \% signal \\ + \hline + \hline + $\PLambda_b \to \PLambda^{\ast}(1520)^{0} \mu\mu$ &$ (1.0\pm0.5)\times10^3 $&$ 19\pm8 $&$ 51\pm25 $&$ 1.0\pm0.4$\\ + $\PLambda_b \to {\rm p } \PK \mu\mu$ &$ (1.0\pm0.5)\times10^2 $&$ 1.9\pm0.8 $&$ 5.7\pm2.8 $&$ 0.11\pm0.05$ \\ + $\PBd \to \PKplus \mu \mu$ &$ 28\pm7 $&$ 0.55\pm0.06 $&$ 1.6\pm0.5 $&$ 0.031\pm0.006$\\ +$\PBs \to \Pphi \mu \mu$ &$ (3.2\pm1.3)\times10^2 $&$ 6.2\pm2.1 $&$ 17\pm7 $&$ 0.33\pm0.12$\\ +signal swaps &$ (3.6\pm0.9)\times10^2 $&$ 6.9\pm0.6 $&$ 33\pm9 $&$ 0.64\pm0.06$ \\ +$\PBd \to \PKstar \PJpsi$ swaps &$ (1.3\pm0.4)\times10^2 $&$ 2.6\pm0.4 $&$ 2.7\pm2.8 $&$ 0.05\pm0.05$ \\ + + \hline + \end{tabular} +\end{tiny} +\includegraphics[angle=-90,width=0.49\textwidth]{{images/h_Bd_Kstmm_vetoes}.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{{h_Lb_L1520mm_vetoes}.pdf} + +\end{center} + + + + +\end{footnotesize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} +\fi + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate simulation} +{~} + \begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\begin{footnotesize} +\item PID, kinematics and isolation variables used in a Boosted Decision Tree (BDT) to discriminate signal and background. +\item BDT with k-Folding technique. +\item Completely data driven. +\end{footnotesize} +\end{itemize} +\begin{center} +\includegraphics[width=0.70\textwidth]{images/Chopping_Distrib.pdf} +\end{center} + +\column{0.5\textwidth} + +\includegraphics[angle=-90,width=0.82\textwidth]{images/Fig1.pdf} \\ +\includegraphics[width=0.88\textwidth]{images/fold.png} + +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Multivariate simulation, efficiency} +{~} + + \begin{minipage}{\textwidth} + \begin{footnotesize} + +\ARROW BDT was also checked in order not to bias our angular distribution: +\begin{center} +\includegraphics[angle=-90,width=0.8\textwidth]{images/BDT_Eff_Comp.pdf} +\end{center} +\ARROW The BDT has small impact on our angular observables. We will correct for these effects later on. + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\iffalse + +\begin{frame}{Mass modelling} +{~} +\begin{minipage}{\textwidth} +\begin{tiny} +\begin{columns} +\column{0.1in} +{~} +\column{2.5in} +\ARROW The signal is modelled by a sum of two Crystal-Ball functions with common mean.\\ +\ARROW The background is a single exponential.\\ +\ARROW The base parameters are obtained from the proxy channel: $\PBd \to \PJpsi (\mu\mu) \PKstar$.\\ +\ARROW All the parameters are fixed in the signal pdf.\\ +\ARROW Scaling factors for resolution are determined from MC.\\ +\ARROW In fitting the rare mode only the signal, background yield and the slope of the exponential is left floating.\\ +\begin{center} +\includegraphics[angle=-90,width=0.9\textwidth]{images/msignal.pdf}\\ + +\end{center} +\ARROW We found $624\pm30$ candidates in the most interesting $\left[1.1,6.0\right]~\GeV^2/c^4$ region \\ and $2398 \pm 57$ in the full range $\left[ 1.1, 19.\right]~\GeV^2/c^4$. +\column{2.5in} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/FitJpsiKstar_withBDT_withoutPartially}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/Scaling_factor}.pdf}\\ +\ARROW The S-wave fraction is extracted using a \texttt{LASS} model. +\end{columns} + +\end{tiny} +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Monte Carlo corrections} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\ARROW No Monte Carlo simulation is perfect! One needs to correct for remaining differences.\\ +\ARROW We reweighted our $\PBd \to \PKstar \mu \mu$ Monte Carlo accordingly to differences between the $\PBd \to \PKstar \PJpsi$ in data (Splot) and Monte Carlo. +\only<1>{ +\begin{center} +\includegraphics[angle=-90,width=0.38\textwidth]{images/pt.pdf} +\includegraphics[angle=-90,width=0.38\textwidth]{images/vertex.pdf}\\ +\includegraphics[angle=-90,width=0.38\textwidth]{images/nTracks.pdf} +\end{center} +} +\only<2>{ +\begin{center} +\includegraphics[angle=-90,width=0.38\textwidth]{images/eta_logy.pdf} +\includegraphics[angle=-90,width=0.38\textwidth]{images/B0_p.pdf} \\ +\includegraphics[angle=-90,width=0.38\textwidth]{{images/bdt_data_mc_nominalMkpi}.pdf} +\end{center} +} + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + +\fi + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Detector acceptance} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} + +\begin{columns} + +\column{0.6\textwidth} +\begin{itemize} +\item Detector distorts our angular distribution. +\item We need to model this effect. +\item 4D function is used: +\begin{align*} +\epsilon (\cos \thetal, \cos \thetak, \phi, q^2) = \\\sum_{ijkl} P_i(\cos \thetal) P_j(\cos \thetak ) P_k(\phi) P_l(q^2), +\end{align*} +where $P_i$ is the Legendre polynomial of order $i$. +\item We use up to $4^{th}, 5^{th}, 6^{th}, 5^{th}$ order for the $\cos \thetal, \cos \thetak, \phi, q^2$. +\item The coefficients were determined using Method of Moments, with a huge simulation sample. +\item The simulation was done assuming a flat phase space and reweighing the $q^2$ distribution to make is flat. +\item To make this work the $q^2$ distribution needs to be reweighted to be flat. +\end{itemize} +%\includegraphics[width=0.75\textwidth]{images/q2PHSP.png} + + + +\column{0.4\textwidth} +\only<1>{ + +\includegraphics[width=0.99\textwidth]{images/det.png} +} +\end{columns} + + +\end{footnotesize} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Control channel} +{~} + \begin{minipage}{\textwidth} +\begin{footnotesize} +\begin{itemize} +\item We tested our unfolding procedure on $\PB \to \PJpsi \PKstar$. +\item The result is in perfect agreement with other experiments and our different analysis of this decay. +\end{itemize} +\end{footnotesize} +\begin{center} +\includegraphics[angle=-90,width=0.4\textwidth]{images/mlogjpsi.pdf} +\includegraphics[angle=-90,width=0.4\textwidth]{images/mkpijpsi.pdf}\\ +\includegraphics[width=0.99\textwidth]{images/angles3.png} +\end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{The columns of New Physics} +{~} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[width=0.94\textwidth]{images/columns.png} + + \end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{The columns of New Physics} +{~} + \begin{minipage}{\textwidth} +\begin{enumerate} +\item Maximum likelihood fit: +\begin{itemize} +\item The most standard way of obtaining the parameters. +\item Suffers from convergence problems, under coverages, etc. in low statistics. +\end{itemize} +\item Method of moments: +\begin{itemize} +\item Less precise then the likelihood estimator ($10-15\%$ larger uncertainties). +\item Does not suffer from the problems of likelihood fit. +\end{itemize} +\item Amplitude fit: +\begin{itemize} +\item Incorporates all the physical symmetries inside the amplitudes! The most precise estimator. +\item Has theoretical assumptions inside! +\end{itemize} +\end{enumerate} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} +{~} +\begin{footnotesize} + + \begin{minipage}{\textwidth} +\ARROW In the maximum likelihood fit one could weight the events accordingly to the $\dfrac{1}{\varepsilon(\cos \thetal, \cos \thetak, \phi, q^2)}$\\ +\ARROW Better alternative is to put the efficiency into the maximum likelihood fit itself: +\begin{align*} +\mathcal{L}=\prod_{i=1}^N \epsilon_i(\Omega_i, q_i^2) \mathcal{P}(\Omega_i, q_i^2) / \int \epsilon(\Omega, q^2) \mathcal{P}(\Omega, q^2) d\Omega dq^2 +\end{align*} +\ARROW Only the relative weights matters!\\ +\ARROW The Procedure was commissioned with TOY MC study.\\ +\ARROW Use Feldmann-Cousins to determine the uncertainties. \\ +\ARROW Angular background component is modelled with $2^{\rm nd }$ order Chebyshev polynomials, which was tested on the side-bands.\\ +\ARROW S-wave component treated as nuisance parameter.\\ +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_Afb3}.pdf} +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_P11}.pdf} +\includegraphics[angle=-90,width=0.33\textwidth]{{images/FC_P57}.pdf} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} +\iffalse +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} +{~} + \begin{minipage}{\textwidth} +\begin{center} +\only<1>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/FLPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S3Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/S4Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S5Pad.pdf} +} +\only<2>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/AFBPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S7Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/S8Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/S9Pad.pdf} +} + + +\end{center} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[angle=-90,width=0.65\textwidth]{images/P5pPadOverlay.pdf}\\ + \end{center} + +\begin{itemize} +\item Tension with $3~\invfb$ gets confirmed! +\item two bins both deviate by $2.8~\sigma$ from SM prediction. +\item Result compatible with previous result. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +\fi + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Method of moments} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} +\ARROW See {\color{blue}{\href{http://arxiv.org/abs/1503.04100}{Phys.Rev.D91(2015)114012}}}, F.Beaujean , M.Chrzaszcz, N.Serra, D. van Dyk for details.\\ +\ARROW The idea behind Method of Moments is simple: Use orthogonality of spherical harmonics, $f_j(\overrightarrow{\Omega})$ to solve for coefficients within a $q^2$ bin: +\begin{align*} +\int f_i(\overrightarrow{\Omega}) f_j(\overrightarrow{\Omega}) = \delta_{ij} +\end{align*} +\begin{align*} +M_i = \int \left( \dfrac{1}{d(\Gamma+ \bar{\Gamma})/dq^2} \right) \dfrac{d^3(\Gamma+\bar{\Gamma})}{d \overrightarrow{\Omega}} f_i(\overrightarrow{\Omega})d \Omega +\end{align*} +\ARROW Don’t have true angular distribution but we ''sample'' it with our data.\\ +\ARROW Therefore: $\int \to \sum$ and $M_i \to \widehat{M}_i$ +\begin{align*} +\hat{M}_i=\dfrac{1}{\sum_e \omega_e} \sum_e \omega_e f_i(\overrightarrow{\Omega}_e) +\end{align*} +\ARROW The weight $\omega$ accounts for the efficiency. Again the normalization of weights does not matter. + + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Method of moments - results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + +\only<3> +{ +\ARROW Method of Moments allowed us to measure for the first time a new observable: +} + +\begin{center} +\only<1>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_FLPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S3Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S4Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S5Pad.pdf} +} +\only<2>{ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_AFBPad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S7Pad.pdf}\\ +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S8Pad.pdf} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S9Pad.pdf} +} +\only<3>{ +\includegraphics[angle=-90,width=0.75\textwidth]{images/S6cPad.pdf} +} + +\end{center} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + + + + + +\begin{frame}{Compatibility with SM} +{~} + + \begin{minipage}{\textwidth} + +\begin{columns} +\column{0.1in} +{~} +\column{2in} +\ARROW Use \texttt{EOS} software package to test compatibility with SM.\\ +\ARROW Perform the $\chi^2$ fit to the measured: +\begin{center} +\begin{align*} +F_L, A_{FB}, S_{3,..., 9} . +\end{align*} +\end{center} +\ARROW Float a vector coupling: $\Re(C_9)$.\\ +\ARROW Best fit is found to be $3.4~\sigma$ away from the SM. + + +\column{3in} +\begin{align*} +\Delta \Re (C_9) \equiv \Re(C_9)^{{\rm fit}} - \Re(C_9)^{{\rm SM}} = -1.03 +\end{align*} +\includegraphics[angle=-90,width=0.95\textwidth]{images/wilsonchi2.pdf} +\end{columns} + + + +\end{minipage} + + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}\frametitle{Global picture of $P_5^{\prime}$} + +\begin{columns} + +\column{0.4\textwidth} +\only<1>{{\color{gray}{\ARROW 2013 LHCb: \href{https://arxiv.org/pdf/1308.1707.pdf}{arXiv::1308.1707}}}\\} +\only<1>{\ARROW 2015 LHCb: \href{https://arxiv.org/abs/1512.04442}{arXiv::1512.0444}\\} +\only<1>{{\color{red}{\ARROW 2016 Belle: \href{https://arxiv.org/abs/1604.04042}{arXiv::1604.04042}}}\\} +\only<1>{\ARROW 2017: {\color{blue}{\href{https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/CONFNOTES/ATLAS-CONF-2017-023/}{ATLAS-CONF-2017-023}}} $(20.5~\rm fb^{-1})$ and {\color{OliveGreen}{\href{http://cds.cern.ch/record/2256738?ln=en}{CMS-PAS-BPH-15-008}}} $(20.8~\rm fb^{-1})$} + + + +\column{0.6\textwidth} +\only<1>{ +\ARROW Theory: +~~DHMV: \href{https://arxiv.org/abs/1407.8526}{arXiv::1407.8526} +~~ASZB: \href{https://arxiv.org/abs/1411.3161}{arXiv::1411.3161} +} +%\includegraphics[width=0.95\textwidth]{images/P5p1.png} +\only<1>{ +\includegraphics[angle=-90,width=0.9\textwidth]{images/P5p.pdf} +} + + +\end{columns} +\only<1>{ + + +} + +\end{frame} + + + +\iffalse + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Branching fraction measurements of $\PLambdab \to \PLambda \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + + \begin{center} + \only<1>{ + \includegraphics[width=0.65\textwidth]{images/Lb_BR.png} +} + \only<2>{ + \includegraphics[width=0.45\textwidth]{images/Lblow.png} +\includegraphics[width=0.45\textwidth]{images/Lbhigh.png} + +} + + + \end{center} + + +\begin{itemize} +\item This years LHCb measurement [JHEP 06 (2015) 115]]. +\item In total $\sim 300$ candidates in data set. +\item Decay not present in the low $q^2$. + +\end{itemize} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}{Angular analysis of $\PLambdab \to \PLambda \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item For the bins in which we have $>3~\sigma$ significance the forward backward asymmetry for the hadronic and leptonic system. +\end{itemize} +\begin{center} +\includegraphics[width=0.9\textwidth]{{images/AFB_Lb}.png} +\end{center} +\begin{itemize} +\item $A_{FB}^H$ is in good agreement with SM. +\item $A_{FB}^{\ell}$ always in above SM prediction. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Lepton universality test} +{~} + \begin{minipage}{\textwidth} +\begin{columns} +\column{3.0in} +\begin{itemize} +\item If $\PZprime$ is responsible for the $P'_5$ anomaly, does it couple equally to all flavours? +\includegraphics[width=0.9\textwidth]{images/uni2.png} +\item Challenging analysis due to bremsstrahlung. +\item Migration of events modeled by MC. +\item Correct for bremsstrahlung. +\item Take double ratio with $\PBplus \to \PJpsi \PKplus$ to cancel systematics. +\item In $3\invfb$, LHCb measures $R_K=0.745^{+0.090}_{-0.074}(stat.)^{+0.036}_{-0.036}(syst.)$ +\item Consistent with SM at $2.6\sigma$. + +\end{itemize} +\column{2.0in} +\includegraphics[width=0.99\textwidth]{images/RK.png}\\ +\begin{itemize} +\item \href{http://arxiv.org/abs/1406.6482}{Phys. Rev. Lett. 113, 151601 (2014)} +\end{itemize} +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Angular analysis of $\PBzero \to \PKstar \Pe \Pe$} +{~} +\only<1>{ + \begin{minipage}{\textwidth} + \begin{itemize} + \item With the full data set ($3\invfb$) we performed angular analysis in $0.0004 < q^2 <1~\GeV^2$. + \item Electrons channels are extremely challenging experimentally: + \begin{itemize} + \item Bremsstrahlung. + \item Trigger efficiencies. + \end{itemize} + \item Determine the angular observables: $\FL$, $\ATD$, $\ATRe$, $\ATIm$: + \end{itemize} +\begin{equation} + \label{eq:physPars} + \begin{split} + \FL &=\frac{|A_0|^2}{|A_0|^2+|A_{||}|^2 + |A_\perp|^2}\\ + \ATD &= \frac{|A_\perp|^2-|A_{||}|^2}{|A_\perp|^2+|A_{||}|^2}\\ + \ATRe &= \frac{2\Real(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}\\ + \ATIm &= \frac{2\Imag(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}, +\end{split}\nonumber +\end{equation} + +\end{minipage} +} +\only<2>{ +\begin{center} +\includegraphics[width=0.5\textwidth]{images/Kstee.png}\\ +\end{center} +\begin{itemize} +\item Results in full agreement with the SM. +\item Similar strength on $C_7$ Wilson coefficient as from $\Pbeauty \to \Pstrange \Pphoton$ decays. +\end{itemize} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/Kstee2.png} +\end{center} + +} + \vspace*{2.1cm} +\end{frame} + +\fi + +\begin{frame} +\begin{center} +\begin{Huge} +Global fit to $\Pbeauty \to \Pstrange \ell \ell$ measurements +\end{Huge} +\end{center} + + + + +\end{frame} + + + +\begin{frame}{Link the observables} +\begin{footnotesize} + +\ARROW Fits prepare by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}} + +\begin{itemize} + +\item Inclusive + +\begin{itemize} +\item $B\to X_s\gamma$ {\color{gray}($BR$) +.......................................................... } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} +\item $B\to X_s\ell^+\ell^-$ {\color{gray}($dBR/dq^2$) +............................................ } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} +\end{itemize} + +\item Exclusive leptonic + +\begin{itemize} +\item $B_s\to \ell^+\ell^-$ {\color{gray}($BR$) +........................................................ } {\color{red} $\C{10}^{(\prime)}$} +\end{itemize} + +\item Exclusive radiative/semileptonic +\begin{itemize} +\item $B\to K^*\gamma$ {\color{gray}($BR$, $S$, $A_I$) +................................................ } {\color{red} $\C7^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $B\to K\ell^+\ell^-$ {\color{gray}($dBR/dq^2$) +.............................................. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $\bf \color{Red} B\to K^*\ell^+\ell^-$ {\color{gray}($dBR/dq^2$, {\bf Optimized Angular Obs.}) +.. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $B_s\to \phi \ell^+\ell^-$ {\color{gray}($dBR/dq^2$, Angular Observables) +.............. } {\color{red} $\C7^{(\prime)}$, $\C9^{(\prime)}$, $\C{10}^{(\prime)}$}%, {\color{brown} $\C{\rm had}$} + +\item $\Lambda_b\to \Lambda\ell^+\ell^-$ {\color{gray}(None so far)} +\item etc. +\end{itemize} + + + +\end{itemize} +\end{footnotesize} + +\end{frame} + +\frame{ \frametitle{Statistic details} + +\begin{footnotesize} + +\ARROW Frequentist approach: +\medskip + +$$\chi^2(C_i) = [O_\text{exp}- O_\text{th}(C_i)]_j \, [Cov^{-1}]_{jk}\, [O_\text{exp}- O_\text{th}(C_i)]_k$$ + + +\begin{itemize} +\item $\bf Cov = Cov^\text{exp} + Cov^\text{th}$. We have $Cov^\text{exp}$ for the first time +\item Calculate $Cov^\text{th}$: correlated multigaussian scan over all nuisance parameters +\item $Cov^\text{th}$ depends on $C_i$: Must check this dependence\\[5mm] +\end{itemize} +For the Fit: +\begin{itemize} +\item Minimise $\chi^2 \to \chi^2_\text{min} = \chi^2(C_i^0)\quad$ (Best Fit Point = $C_i^0$) +\item Confidence level regions: $\chi^2(C_i) - \chi^2_\text{min} < \Delta\chi_{\sigma,n}$ +%\item Compute pulls by inversion of the above formula +\end{itemize} +\medskip +\ARROW The results from 1D scans:{~}\\{~}\\ +\begin{tiny} +\begin{tabular}{crccc} +%\toprule[1.6pt] +Coefficient ${\cal C}_i^{NP}={\cal C}_i-{\cal C}_i^{SM}$ & Best fit & 1$\sigma$ & 3$\sigma$ & Pull$_{\rm SM}$ \\ \hspace{10mm} \\[5mm] +% \midrule + $\bf\cred\C9^{\rm NP}$ & $ -1.09 $ & $ [-1.29,-0.87] $ & $ [-1.67,-0.39] $ & $\,\,\,\,\,\,\bf 4.5 + \cred \Leftarrow$ \hspace{5mm} \\[3mm] + $\C9^{\rm NP}=-\C{10}^{\rm NP}$ & $ -0.68 $ & $ [-0.85,-0.50] $ & $ [-1.22,-0.18] $ & \bf \quad 4.2 + $\cred\Leftarrow$ \hspace{5mm} \\[3mm] + $\C9^{\rm NP}=-\C{9'}^{\rm NP}$ & $ -1.06 $ & $ [-1.25,-0.86] $ & $ [-1.60,-0.40] $ & \quad \quad \quad \,\,\quad 4.8 + $\cred\Leftarrow$ (no $R_K$)\hspace{5mm} \\[3mm] + + \hspace{5mm} \\[3mm] +% \bottomrule[1.6pt] +\end{tabular} +\end{tiny} +\end{footnotesize} + +} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Theory implications} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item The data can be explained by modifying the $C_9$ Wilson coefficient. +\item Overall there is around $4.5~\sigma$ discrepancy wrt. SM. +\end{itemize} +\includegraphics[width=0.9\textwidth]{images/C9.png} + + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{2D scans} +{~} +\begin{footnotesize} + + \begin{minipage}{\textwidth} +\begin{columns} +\begin{column}{0.5cm} + + +\end{column} +\begin{column}{17cm} + +\renewcommand{\arraystretch}{1.4} + \setlength{\tabcolsep}{13pt} +\begin{tabular}{cccr} +\hline +Coefficient & Best Fit Point & Pull$_{\rm SM}$ \\ \hline + + $(\C7^{\rm NP},\C9^{\rm NP})$ & $(-0.00,-1.07)$ & {\bf 4.1} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{10}^{\rm NP})$ & $(-1.08,0.33)$ & {\bf 4.3} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{7'}^{\rm NP})$ & $(-1.09,0.02)$ & {\bf 4.2} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{9'}^{\rm NP})$ & $(-1.12,0.77)$ & {\bf 4.5} \hspace{5mm} \\ + $(\C9^{\rm NP},\C{10'}^{\rm NP})$ & $(-1.17,-0.35)$ & {\bf 4.5} \hspace{5mm} \\ + $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ & $(-1.15,0.34)$ & \!\!\!\!\!\!\!\!\!\!\! {\bf 4.7} \\ + $(\C{9}^{\rm NP}=-\C{9'}^{\rm NP},\C{10}^{\rm NP}=-\C{10'}^{\rm NP})$ & $(-1.06,0.06)$ & {\bf 4.4} \hspace{5mm} \\ + $(\C{9}^{\rm NP}=\C{9'}^{\rm NP},\C{10}^{\rm NP}=\C{10'}^{\rm NP})$ & $(-0.64,-0.21)$ & 3.9 \hspace{5mm} \\ + $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=\C{10'}^{\rm NP})$ & $(-0.72,0.29)$ & 3.8 \hspace{5mm} \\ +% $(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ & $(-0.66,0.03)$ & 2.0 & 23.0 + %$(\C{9}^{\rm NP}=-\C{10}^{\rm NP},\C{9'}^{\rm NP}=-\C{10'}^{\rm NP})$ & $(-0.69,0.05)$ & 1.9 & 22.0 \hspace{5mm} \\ + +\end{tabular} +\end{column} +\end{columns} + + +\medskip +\begin{itemize} +\item $C_9^{NP}$ always play a dominant role +\item All 2D scenarios above 4$\sigma$ are quite indistinguishable. + +\end{itemize} + + + +\end{minipage} + +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%% + + + +\begin{frame}{$B\to K^\ast \ell\ell\ $ Amplitudes} + +\small + +\mbox{ +\includegraphics[width=3cm,height=2cm]{bsg0.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2cm]{bsg1.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2.4cm]{bsg2.jpg} +} + +\vspace{3mm} + +\mbox{ +\hspace{-10mm} +\colorbox{llgray}{ +\hspace{1mm} +$\displaystyle +A_\lambda^{L,R} = N_\lambda\ \bigg\{ +(C_9 \mp C_{10}) {\blue \F_\lambda(q^2)} ++\frac{2m_b M_B}{q^2} \bigg[ C_7 {\blue \F_\lambda^{T}(q^2)} +- 16\pi^2 \frac{M_B}{m_b} {\red \H_\lambda(q^2)} \bigg] +\bigg\} +$ +\hspace{2mm} +} +} + +\vspace{5mm} +{\small + +\hspace{-8mm} \btr {\brown Local (Form Factors) :} \hspace{2mm} {\blue $ \F_\lambda^{(T)}(q^2) = \av{\bar M_\lambda(k)| \,\bar s\, \Gamma_\lambda^{(T)}\, b\, | \bar{ B}(k+q)}$} +\\[5mm] + +\mbox{ +\hspace{-9mm} +\btr {\brown Non-Local :} \hspace{0mm} {\red $\displaystyle \H_\lambda(q^2) = i \,{\cal P}_\mu^\lambda \int d^4 x\ e^{i q\cdot x}\, +\av{\bar{M}_\lambda(k)| +T\big\{ {\cal J}_{\rm em}^\mu(x), \C{i} \, \mathcal{O}(0) \big\} | \bar{B}(q+k)}$} +} + +\vspace{3mm} + +\hspace{-8mm} +\btr CKM structure : \hspace{2mm} $\displaystyle \H_\lambda = {\color{gray}- \frac{\lambda_u}{\lambda_t} \H_\lambda^{(u)}} - \frac{\lambda_c}{\lambda_t} \H_\lambda^{(c)}$ \hspace{5mm} $\Rightarrow\ \mathcal{O} \sim (\bar{ c} b)(\bar{ s} c)$ + +} + +\end{frame} + + + + + +\begin{frame}{Analytic structure of $\H_\lambda(q^2)$} + +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{3mm} + + +Neglecting OZI- and CKM-suppressed contributions : + +\begin{center} +\includegraphics[width=7.5cm]{Analyticq2.png} +\end{center} + + +$\displaystyle { \hat{\mathcal{H}}_\lambda(q^2)} = (q^2 - M_{J/\psi}^2)(q^2 -M_{\psi(2S)}^2) \,{ {\mathcal{H}}_\lambda(q^2)} \quad $ has no poles. + +\end{frame} + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} + +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{2mm} + +\btr Conformal mapping : \hspace{5mm} $q^2 \mapsto \ z\,(q^2) = \frac{\sqrt{t_+ - q^2} - \sqrt{t_+ - t_0}}{\sqrt{t_+ - q^2} + \sqrt{t_+ - t_0}}$ + +\mbox{ +\hspace{-10mm} +\raisebox{8mm}{\includegraphics[width=5.6cm]{Analyticq22.png}} +\hspace{1mm} +\includegraphics[width=6.5cm]{Analyticz.png} +} + +\vspace{-7mm} + +\btr ${\red \hat \H_\lambda (q^2(z))}$ is {\bf analytic in $|z|<1$}\\[3mm] + +\btr Taylor expand $\red \hat{\H}_\lambda(z)$ around $z=0$.\\[3mm] + +\btr Expansion needed for $|z| < 0.52\ $ ( $-7\,\GeV^2 \leq q^2 \leq 14 \GeV^2$ ) + + +\end{frame} + + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} + +\vspace{3mm} + + +\hspace{-5mm} {\bf \brown Some details for actual parametrisation :} + +\mbox{\hspace{-5mm} \btr Try to capture most features of the expansion (better convergence)} + +\mbox{\hspace{-5mm} \btr Parametrize the ratios $\H_\lambda(q^2)/\F_\lambda(q^2)$ instead} + +\mbox{\hspace{-5mm} \btr The poles should not modify the asymptotic behaviour at $|q^2|\to \infty$} + +\begin{eqnarray} +\H_\lambda(z) &=& +\frac{1-z\, z^*_{J/\psi}}{z-z_{J/\psi}} \frac{1-z\,z^*_{\psi(2S)}}{z-z_{\psi(2S)}} \ \hat\H_\lambda(z) +\nonumber\\[2mm] +% +\hat\H_\lambda(z) &=& \Big[ \sum_{k=0}^K \alpha_k^{(\lambda)} z^{k} \Big] \F_\lambda(z) +\nonumber +\end{eqnarray} + + +where $\alpha^{(\lambda)}_k$ are complex coefficients, and the expansion is truncated after the term $z^{K}$. +We will take $K=2$ ({\brown 16} real parameters). + + +\end{frame} + + + + +\begin{frame}{Experimental constraints on $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown Experimental constraints :} + +\mbox{\hspace{-5mm} \btr The residues of the poles are given by $B\to K^* \psi_n$ :} + +$$ +\H_\lambda(q^2 \to M_{\psi_n}^2) \sim +\frac{M_{\psi_n} f^{\,*}_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2 (q^2 - M_{\psi_n}^2)} + \cdots +$$ + +\mbox{\hspace{-5mm} \btr Angular analyses \Cite{Belle, Babar, LHCb} determine : } + +$$ +|r_\perp^{\psi_n}|,\, +|r_\|^{\psi_n}|,\, +|r_0^{\psi_n}|,\, +\arg\{r_\perp^{\psi_n} r_{0}^{\psi_n*}\},\, +\arg\{r_\|^{\psi_n} r_{0}^{\psi_n*}\}, +$$ + +where $\quad \displaystyle r_\lambda^{\psi_n} \equiv \operatorname*{Res}_{q^2\to M^2_{\psi_n}} \frac{\H_\lambda(q^2)}{\F_\lambda(q^2)} +\sim +\frac{M_{\psi_n} f^*_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2\, \F_\lambda(M_{\psi_n}^2)}$\\[3mm] + + +\mbox{\hspace{-5mm} \btr We produce correlated pseudo-observables from a fit (5+5).} + + + +\end{frame} + + + + +\begin{frame}{Prior Fit to $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown (Prior) Fit to Experimental and theoretical pseudo-observables :} + + + +\begin{table}[b] +% \resizebox{.85\textwidth}{!}{% +\centering +\renewcommand{\arraystretch}{1.5} +\renewcommand{\tabcolsep}{3.1mm} +\begin{tabular}{@{}crrr@{}} +\hline +$k$ & 0\hspace{7mm} & 1\hspace{7mm} & 2\hspace{7mm} \\ +\hline +%re perp +${\rm Re}[\alpha_{k}^{(\perp)}]$ & $-0.06 \pm 0.21$ & $-6.77 \pm 0.27$ & $18.96 \pm 0.59$ \\ +%re para +${\rm Re}[\alpha_{k}^{(\parallel)}]$ & $-0.35 \pm 0.62$ & $-3.13 \pm 0.41$ & $12.20 \pm 1.34$ \\ +%re long +${\rm Re}[\alpha_{k}^{(0)}]$ & $0.05 \pm 1.52$ & $17.26 \pm 1.64$ & -- \\ +%im perp +${\rm Im}[\alpha_{k}^{(\perp)}]$ & $-0.21 \pm 2.25$ & $1.17 \pm 3.58$ & $-0.08 \pm 2.24$ \\ +%im para +${\rm Im}[\alpha_{k}^{(\parallel)}]$ & $-0.04 \pm 3.67$ & $-2.14 \pm 2.46$ & $6.03 \pm 2.50$ \\ +%im long +${\rm Im}[\alpha_{k}^{(0)}]$ & $-0.05 \pm 4.99$ & $4.29 \pm 3.14$ & -- \\ +\hline +\end{tabular} +% } +\caption{Mean values and standard deviations (in units of $10^{-4}$) +of the prior PDF for the parameters $\alpha_k^{(\lambda)}$.} +\label{alphak} +\end{table} + +\end{frame} + +\begin{frame}{New Physics Analysis } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown SM predictions and Fit including $B\to K^* \mu^+\mu^-$ data and $\C{9}^{\rm NP}$ :}\\[4mm] + +\mbox{ +\hspace{-10mm} +\includegraphics[width=12cm]{NPFit.png} +} + +The NP hypothesis with {\red $\C{9}^{\bf NP}\sim -1$} is favored strongly in the global fit + +\end{frame} + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Scale of NP?} +{~} + \begin{minipage}{\textwidth} +\includegraphics[width=0.99\textwidth]{15.png} + +\ARROW Stolen from M. Nardecchia +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Conclusions} +{~} + \begin{minipage}{\textwidth} +\begin{itemize} +\item Clear tensions wrt. SM predictions! +\item Measurements cluster in the same direction. +\item We are not opening the champagne yet! +\item Still need improvement both on theory and experimental side. +\item Time will tell if this is QCD+fluctuations or new Physics: +\end{itemize} +\pause +''... when you have eliminated all the\\ +Standard Model explanations, whatever remains,\\ +however improbable, must be New Physics.''\\ +prof. Joaquim Matias + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +{~} + \begin{minipage}{\textwidth} +\begin{center} +\begin{LARGE} +Thank you for the attention! +\end{LARGE} +\includegraphics[width=0.8\textwidth]{images/Joke.jpg} + +\end{center} + + + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +\backupbegin + +\begin{frame}\frametitle{Backup} + + +\end{frame} + + + + +\begin{frame}{Amplitudes method} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + +\ARROW Fit for amplitudes as (continuous) functions of $q^2$ in the region: $q^2 \in \left[ 1.1. 6.0 \right]~\GeV^2/c^4$.\\ +\ARROW Needs some Ansatz: +\begin{align*} +A(q^2) = \alpha + \beta q^2+ \dfrac{\gamma}{q^2} +\end{align*} +\ARROW The assumption is tested extensively with toys.\\ +\ARROW Set of 3 complex parameters $ \alpha, \beta, \gamma $ per vector amplitude:\begin{itemize} +\item {\color{Magenta}{$L, ~R$}}, {\color{Cerulean}{$0 ,~\| ,~\bot$}}, {\color{PineGreen}{$\Re ,~\Im$}} $\rightarrowtail$~~ $3 \times {\color{PineGreen}{2}} \times {\color{Cerulean}{3}} \times {\color{Magenta}{2}} = 36$ DoF. +\item Scalar amplitudes: $+4$ DoF. +\item Symmetries of the amplitudes reduces the total budget to: $28$. +\end{itemize} +\ARROW The technique is described in \href{http://arxiv.org/pdf/1504.00574v2.pdf}{\color{blue}{JHEP06(2015)084}}.\\ +\ARROW Allows to build the observables as continuous functions of $q^2$: +\begin{itemize} +\item At current point the method is limited by statistics. +\item In the future the power of this method will increase. +\end{itemize} +\ARROW Allows to measure the zero-crossing points for free and with smaller errors than previous methods. +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Amplitudes - results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} +\begin{center} +\begin{columns} +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_AFBOverlay}.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S4Overlay}.pdf} + +\column{0.45\textwidth} +\includegraphics[angle=-90,width=0.95\textwidth]{{images/amplitudes_S5Overlay}.pdf}\\ +{~}\\{~}\\{~}\\{~}\\ +\begin{large} +Zero crossing points: +\end{large} +\begin{align*} +q_0(S_4) & <2.65 & {\rm{~at~}} & 95\% ~CL \\ +q_0(S_5) & \in \left[ 2.49,3.95 \right] & {\rm{~at~}} & 68\% ~CL \\ +q_0(A_{FB}) & \in \left[ 3.40, 4.87 \right] & {\rm{~at~}} & 68\% ~CL +\end{align*} + + +\end{columns} +\end{center} + +\end{minipage} +\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\backupend + +\end{document} diff --git a/Seminars/India_IMSC_2018/mchrzasz.toc b/Seminars/India_IMSC_2018/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Seminars/India_IMSC_2018/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse 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+ blx-compat.def + biblatex_legacy.def + numeric-comp.bbx + numeric.bbx + standard.bbx + numeric-comp.cbx + biblatex.cfg + english.lbx + + + + bibtex + + bibtex + + mchrzasz + + + mchrzasz.aux + + + mchrzasz.bbl + + + mchrzasz.bbl + + + mchrzasz.aux + mchrzasz-blx.bib + + + bib.bib + + + biblatex.bst + + + diff --git a/Seminars/UJ/mchrzasz.snm b/Seminars/UJ/mchrzasz.snm new file mode 100644 index 0000000..2d9bf93 --- /dev/null +++ b/Seminars/UJ/mchrzasz.snm @@ -0,0 +1,4 @@ +\beamer@slide {Js}{15} +\beamer@slide {LargeRecoilAs}{16} +\beamer@slide {alphak}{68} +\beamer@slide {eq:physPars}{75} diff --git a/Seminars/UJ/mchrzasz.synctex.gz b/Seminars/UJ/mchrzasz.synctex.gz deleted file mode 100644 index eb89c83..0000000 --- a/Seminars/UJ/mchrzasz.synctex.gz +++ /dev/null Binary files differ diff --git a/Seminars/UJ/mchrzasz.tex b/Seminars/UJ/mchrzasz.tex index bd13526..9295ee5 100644 --- a/Seminars/UJ/mchrzasz.tex +++ b/Seminars/UJ/mchrzasz.tex @@ -20,17 +20,8 @@ \usepackage[utf8]{inputenc} -\usefonttheme{professionalfonts} -\usepackage[no-math]{fontspec} -\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly -\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font -\setsansfont{Gillius ADF} % This is the font that beamer will use by default -% \setmainfont{Gill Sans Light} % Prettier, but harder to read -\setbeamerfont{title}{family=\fontspec{Gillius ADF}} - -\input t1augie.fd %\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font %\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font @@ -307,6 +298,7 @@ +<<<<<<< HEAD \author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich, IFJ PAN)} \institute{UZH} @@ -316,12 +308,54 @@ \begin{document} \tikzstyle{every picture}+=[remember picture] +======= +\definecolor{indigo}{RGB}{100,0,100} +\definecolor{dgray}{RGB}{80,80,80} +\definecolor{lgray}{RGB}{220,220,220} +\definecolor{dred}{RGB}{190,0,0} +\definecolor{dgreen}{RGB}{0,110,0} +\definecolor{lyellow}{RGB}{245,245,210} +\definecolor{bblue}{RGB}{93,93,255} +\definecolor{bbrown}{RGB}{150,85,52} +\definecolor{llgray}{RGB}{230,230,230} + + + +\newcommand{\F}{\mathcal{F}} +\newcommand{\A}{\mathcal{A}} +\newcommand{\N}{\mathcal{N}} +\renewcommand{\H}{\mathcal{H}} +\newcommand{\Leff}{\mathcal{L}_{\rm eff}} +\newcommand{\heff}{\mathcal{H}_{\rm eff}} +\newcommand{\Lag}{\mathcal{L}} +\newcommand{\red}{\color{red}} +\newcommand{\blue}{\color{blue}} +\newcommand{\indigo}{\color{indigo}} +\newcommand{\brown}{\color{bbrown}} +\newcommand{\bs}{\mathbf} +\newcommand{\sss}{\scriptscriptstyle} + + +\newcommand{\btr}{{ $\blacktriangleright\ $}} +\institute{UZH} +\title[New Physics signatures in Rare $\PB$ decays?]{New Physics signatures in Rare $\PB$ decays?} +\date{25 September 2014} + +\author{ Marcin Chrzaszcz (CERN, IFJ PAN)} + + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 { \setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} \begin{frame}[c]%{\phantom{title page}} \begin{center} \begin{center} \begin{columns} +<<<<<<< HEAD \begin{column}{0.9\textwidth} \flushright\fontspec{Trebuchet MS}\bfseries \Huge {Recent results on angular analysis of decay $\PB \to \PKstar \Pmu \Pmu$ at LHCb} @@ -329,22 +363,51 @@ \begin{column}{0.2\textwidth} %\includegraphics[width=\textwidth]{SHiP-2} \end{column} +======= + \begin{column}{0.75\textwidth} + \flushright \bfseries \huge {New Physics signatures \\in Rare $\PB$ decays} + \end{column} + \begin{column}{0.02\textwidth} + {~} + \end{column} + \begin{column}{0.23\textwidth} + % \hspace*{-1.cm} + \vspace*{-3mm} + \includegraphics[width=0.6\textwidth]{lhcb-logo} + \end{column} + +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{columns} \end{center} \quad \vspace{3em} \begin{columns} \begin{column}{0.44\textwidth} +<<<<<<< HEAD \flushright \vspace{-1.8em} {\fontspec{Trebuchet MS} \Large Marcin Chrząszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} \end{column} \begin{column}{0.53\textwidth} \includegraphics[height=1.3cm]{uzh-transp}{~}{~} \includegraphics[height=1.1cm]{ifj.png} +======= +%\flushright \vspace{-2.8em} { \fontspec{Zapfino} Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + +\flushright \vspace{-2.8em} { \Large Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} + + +\end{column} +\begin{column}{0.53\textwidth} +\hspace{2.0cm} +\includegraphics[height=1.6cm]{cern}~~ +\includegraphics[height=1.3cm]{ifj} + +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{column} \end{columns} \vspace{1em} +<<<<<<< HEAD % \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ \vspace{0.5em} \textcolor{normal text.fg!50!Comment}{University of Padova \\March 22, 2016} @@ -353,6 +416,14 @@ } +======= + + + \textcolor{normal text.fg!50!Comment}{WFAIS Seminar, Krakow\\January 8, 2018} +\end{center} +\end{frame} +} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \begin{frame}{Outline} \begin{minipage}{\textwidth} @@ -362,7 +433,11 @@ \item Why flavour is important. \item LHCb detector. \item $\Pbeauty \to \Pstrange \ell \ell$ theory in a nutshell. +<<<<<<< HEAD \item LHCb measurements of $\PBd \to \PKstar \Pmu \Pmu$ +======= +\item LHCb measurements of $\PB \to \PKstar \Pmu \Pmu$ +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \begin{itemize} \item Maximum likelihood fit. \item Method of moments. @@ -811,7 +886,11 @@ %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +<<<<<<< HEAD \begin{frame}{$\PBzero \to \PKstar \Pmuon \APmuon$ kinematics} +======= +\begin{frame}{$\PB \to \PKstar \Pmuon \APmuon$ kinematics} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 {~} \begin{minipage}{\textwidth} @@ -843,7 +922,25 @@ &&\hspace{-2.7cm}+ J_9 \sin^2\theta_K \sin^2\theta_l \sin 2\phi \bigg]\,, \nonumber} }} +<<<<<<< HEAD $\color{JungleGreen}{\Rrightarrow}$ This is the most general expression of this kind of decay. +======= +$\color{JungleGreen}{\Rrightarrow}$ This is the most general expression of this kind of decay.\\ +\pause + +$\color{JungleGreen}{\Rrightarrow}$ In practice as experimentalist we do not measure $J_i$ but: +\begin{columns} +\column{0.5\textwidth} +\ARROW Branching fraction: +$\mathcal{B}(\PB \to \PKstar \Pmuon \APmuon) = 3J_{1c}+6J_{1s} - J_{2c} -2 J_{2s}$ +\column{0.5\textwidth} +\ARROW \small Normalized angular observables: +\begin{equation} +S_i= \frac{J_i}{3J_{1c}+6J_{1s} - J_{2c} -2 J_{2s}} \nonumber +\end{equation} + +\end{columns} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 } @@ -929,7 +1026,11 @@ %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +<<<<<<< HEAD \begin{frame}{LHCbs $\PBzero \to \PKstar \Pmuon \APmuon$, Selection} +======= +\begin{frame}{LHCbs $\PB \to \PKstar \Pmuon \APmuon$, Selection} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 {~} \begin{minipage}{\textwidth} \begin{footnotesize} @@ -980,12 +1081,21 @@ Channel & Estimated events & \% signal & Estimated events & \% signal \\ \hline \hline +<<<<<<< HEAD $\PLambda_b \to \PLambda^{\ast}(1520)^{0} \mu\mu$ &$ (1.0\pm0.5)\times10^3 $&$ 19\pm8 $&$ 51\pm25 $&$ 1.0\pm0.4$\\ $\PLambda_b \to {\rm p } \PK \mu\mu$ &$ (1.0\pm0.5)\times10^2 $&$ 1.9\pm0.8 $&$ 5.7\pm2.8 $&$ 0.11\pm0.05$ \\ $\PBd \to \PKplus \mu \mu$ &$ 28\pm7 $&$ 0.55\pm0.06 $&$ 1.6\pm0.5 $&$ 0.031\pm0.006$\\ $\PBs \to \Pphi \mu \mu$ &$ (3.2\pm1.3)\times10^2 $&$ 6.2\pm2.1 $&$ 17\pm7 $&$ 0.33\pm0.12$\\ signal swaps &$ (3.6\pm0.9)\times10^2 $&$ 6.9\pm0.6 $&$ 33\pm9 $&$ 0.64\pm0.06$ \\ $\PBd \to \PKstar \PJpsi$ swaps &$ (1.3\pm0.4)\times10^2 $&$ 2.6\pm0.4 $&$ 2.7\pm2.8 $&$ 0.05\pm0.05$ \\ +======= + $\Lambda_b \to \Lambda^{\ast}(1520)^{0} \mu\mu$ &$ (1.0\pm0.5)\times10^3 $&$ 19\pm8 $&$ 51\pm25 $&$ 1.0\pm0.4$\\ + $\Lambda_b \to {\rm p } \PK \mu\mu$ &$ (1.0\pm0.5)\times10^2 $&$ 1.9\pm0.8 $&$ 5.7\pm2.8 $&$ 0.11\pm0.05$ \\ + $\PB \to \PKplus \mu \mu$ &$ 28\pm7 $&$ 0.55\pm0.06 $&$ 1.6\pm0.5 $&$ 0.031\pm0.006$\\ +$\PBs \to \Pphi \mu \mu$ &$ (3.2\pm1.3)\times10^2 $&$ 6.2\pm2.1 $&$ 17\pm7 $&$ 0.33\pm0.12$\\ +signal swaps &$ (3.6\pm0.9)\times10^2 $&$ 6.9\pm0.6 $&$ 33\pm9 $&$ 0.64\pm0.06$ \\ +$\PB \to \PKstar \PJpsi$ swaps &$ (1.3\pm0.4)\times10^2 $&$ 2.6\pm0.4 $&$ 2.7\pm2.8 $&$ 0.05\pm0.05$ \\ +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \hline \end{tabular} @@ -1073,7 +1183,11 @@ \ARROW Scaling factors for resolution are determined from MC.\\ \ARROW In fitting the rare mode only the signal, background yield and the slope of the exponential is left floating.\\ \begin{center} +<<<<<<< HEAD \includegraphics[angle=-90,width=0.9\textwidth]{images/msignal.pdf}\\ +======= +\includegraphics[angle=-90,width=0.8\textwidth]{images/msignal.pdf}\\ +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{center} \ARROW We found $624\pm30$ candidates in the most interesting $\left[1.1,6.0\right]~\GeV^2/c^4$ region \\ and $2398 \pm 57$ in the full range $\left[ 1.1, 19.\right]~\GeV^2/c^4$. @@ -1567,7 +1681,11 @@ %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +<<<<<<< HEAD \begin{frame}{Branching fraction measurements of $\PLambdab \to \PLambda \Pmu \Pmu$} +======= +\begin{frame}{Branching fraction measurements of $\Lambda_b \to \Lambda \Pmu \Pmu$} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 {~} \begin{minipage}{\textwidth} @@ -1601,7 +1719,11 @@ %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +<<<<<<< HEAD \begin{frame}{Angular analysis of $\PLambdab \to \PLambda \Pmu \Pmu$} +======= +\begin{frame}{Angular analysis of $\Lambda_b \to \Lambda \Pmu \Pmu$} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 {~} \begin{minipage}{\textwidth} @@ -1631,7 +1753,11 @@ \begin{columns} \column{3.0in} \begin{itemize} +<<<<<<< HEAD \item If $\PZprime$ is responsible for the $P'_5$ anomaly, does it couple equally to all flavours? +======= +\item If we attribute the deviations to NP, is it Lepton Universal? +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \includegraphics[width=0.9\textwidth]{images/uni2.png} \item Challenging analysis due to bremsstrahlung. \item Migration of events modeled by MC. @@ -1655,6 +1781,7 @@ \end{frame} +<<<<<<< HEAD %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% @@ -1704,6 +1831,41 @@ \begin{center} \begin{Huge} Global fit to $\Pbeauty \to \Pstrange \ell \ell$ measurements +======= +\begin{frame}\frametitle{There is more!} +%https://indico.cern.ch/event/580620/ +\ARROW We followed this path...\\ +\ARROW We measured the ratio: +\begin{equation*} +R_{\PKstar}= \frac{\mathcal{B}( \PB \to \PKstar \Pmu \Pmu)}{\mathcal{B}( \PB \to \PKstar \Pe \Pe)} +\end{equation*} +\pause + +\begin{columns} +\column{0.4\textwidth} +\ARROW Measurement performed in two $q^2$ bins. \\ +\ARROW Normalized in double ratio to $\PB \to \PKstar \PJpsi$.\\ +\includegraphics[width=0.95\textwidth]{images/plot.png} + + +\column{0.6\textwidth} +\begin{center} +\includegraphics[width=0.95\textwidth]{images/RKstar.png} +\end{center} + +\end{columns} + + + +\end{frame} + + + +\begin{frame} +\begin{center} +\begin{Huge} +Global analysis of $\Pbeauty \to \Pstrange \ell \ell$ measurements +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{Huge} \end{center} @@ -1717,7 +1879,11 @@ \begin{frame}{Link the observables} \begin{footnotesize} +<<<<<<< HEAD \ARROW Fits prepare by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}} +======= +\ARROW Fits prepare by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, \href{https://arxiv.org/abs/1704.05340}{\color{blue}{arXiv::1704.05340}} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \begin{itemize} @@ -1785,6 +1951,10 @@ \end{itemize} \medskip \ARROW The results from 1D scans:{~}\\{~}\\ +<<<<<<< HEAD +======= +\iffalse +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \begin{tiny} \begin{tabular}{crccc} %\toprule[1.6pt] @@ -1801,6 +1971,13 @@ % \bottomrule[1.6pt] \end{tabular} \end{tiny} +<<<<<<< HEAD +======= + +\fi +\includegraphics[width=0.99\textwidth]{images/table1.png} + +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{footnotesize} } @@ -1816,7 +1993,11 @@ \begin{itemize} \item The data can be explained by modifying the $C_9$ Wilson coefficient. +<<<<<<< HEAD \item Overall there is around $4.5~\sigma$ discrepancy wrt. SM. +======= +\item Overall there is around $4-5~\sigma$ discrepancy wrt. SM. +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{itemize} \includegraphics[width=0.9\textwidth]{images/C9.png} @@ -1930,6 +2111,7 @@ \end{minipage} \vspace*{2.1cm} \end{frame} +<<<<<<< HEAD %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{There is more!} {~} @@ -1952,6 +2134,8 @@ \vspace*{2.1cm} \end{frame} +======= +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% @@ -1976,7 +2160,11 @@ %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +<<<<<<< HEAD \begin{frame}{Disclaimer, credit to J.Matias!} +======= +\begin{frame}{Disclaimer} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 {~} \begin{footnotesize} @@ -1990,6 +2178,7 @@ $$H_\lambda \to H_\lambda + h_\lambda \,\, {\rm where} \,\, h_{\lambda}=h_{\lambda}^{(0)}+h_{\lambda}^{(1)} q^2 + h_{\lambda}^{(2)} q^4 \quad {\rm and} \quad h_{\lambda}^{(0)}\to C_7^{NP}, h_{\lambda}^{(1)}\to C_9^{\rm NP}$$ with ($\lambda=0,\pm$)\hfill(copied from JC'14).\\ {\bf Complications:} complete lack of theory input/output $\Rightarrow$ {\bf no predictivity} with 18 free parameters (any shape). Specific problems... +<<<<<<< HEAD \item One has to go back and look at the symmetries of the amplitudes. They imply the Matias-Serra relations: \begin{align*} P_2^{rel}=\frac{1}{2} \left[ P_4^\prime P_5^\prime + \delta_a+ \frac{1}{\beta}\sqrt{(-1 +P_1 +P_4^{\prime 2}) (-1 - P_1 + \beta^2 P_5^{\prime 2}) + \delta_b} \right] @@ -1997,6 +2186,10 @@ \hfill where $\delta_a$ and $\delta_b$ are function of product of tiny $P_6^\prime$, $P_8^\prime$, $P_3$.\medskip\\ \ARROW {\it This is truly independently of any crazy non-factorizable, factorizable, or New Physics (with no weak phases) that is included inside the $H_\lambda$ (or $A_{\perp,\|,0}$)} +======= +\item The correlator $H_\lambda $ has poles that correspond to the photon the $\PJpsi$. Clearly a 3rd order polynomial cannot approximate this well enough! + +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{itemize} @@ -2005,14 +2198,20 @@ \end{frame} +<<<<<<< HEAD %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{Disclaimer, credit to J.Matias!} +======= +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{More robust calculation of correlator} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 {~} \begin{footnotesize} +<<<<<<< HEAD \ARROW Using theory predictions (DHMV'15, JHEP 1412 (2014) 125) for {\bf bin [4,6]} one has: \begin{center} @@ -2055,12 +2254,85 @@ \end{footnotesize} \vspace*{2.1cm} +======= + + \begin{minipage}{\textwidth} +\begin{center} +\includegraphics[width=0.5\textwidth]{images/Tom.png} +\end{center} +\ARROW Calculate non-local ME at {negative $q^2$} \\[3mm] +\ARROW Extrapolate to $q^2>0$ via some type of {analytic continuation} \\[3mm] +\ARROW Use data, when possible, to constrain the extrapolation + +{ \footnotesize + +$\qquad \square\ $ We will use $B\to K^* \psi_n$ + +$\qquad \square\ $ Cannot use $B\to K^*\mu^+\mu^-$ if $\C9^{\rm NP}$ unknown + +} + + \end{minipage}\end{footnotesize} + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{$B\to K^\ast \ell\ell\ $ Amplitudes} + +\small + +\mbox{ +\includegraphics[width=3cm,height=2cm]{bsg0.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2cm]{bsg1.jpg}\hspace{5mm} +\includegraphics[width=3cm,height=2.4cm]{bsg2.jpg} +} + +\vspace{3mm} + +\mbox{ +\hspace{-10mm} +\colorbox{llgray}{ +\hspace{1mm} +$\displaystyle +A_\lambda^{L,R} = N_\lambda\ \bigg\{ +(C_9 \mp C_{10}) {\blue \F_\lambda(q^2)} ++\frac{2m_b M_B}{q^2} \bigg[ C_7 {\blue \F_\lambda^{T}(q^2)} +- 16\pi^2 \frac{M_B}{m_b} {\red \H_\lambda(q^2)} \bigg] +\bigg\} +$ +\hspace{2mm} +} +} + +\vspace{5mm} +{\small + +\hspace{-8mm} \btr {\brown Local (Form Factors) :} \hspace{2mm} {\blue $ \F_\lambda^{(T)}(q^2) = \av{\bar M_\lambda(k)| \,\bar s\, \Gamma_\lambda^{(T)}\, b\, | \bar{ B}(k+q)}$} +\\[5mm] + +\mbox{ +\hspace{-9mm} +\btr {\brown Non-Local :} \hspace{0mm} {\red $\displaystyle \H_\lambda(q^2) = i \,{\cal P}_\mu^\lambda \int d^4 x\ e^{i q\cdot x}\, +\av{\bar{M}_\lambda(k)| +T\big\{ {\cal J}_{\rm em}^\mu(x), \C{i} \, \mathcal{O}(0) \big\} | \bar{B}(q+k)}$} +} + +\vspace{3mm} + +\hspace{-8mm} +\btr CKM structure : \hspace{2mm} $\displaystyle \H_\lambda = {\color{gray}- \frac{\lambda_u}{\lambda_t} \H_\lambda^{(u)}} - \frac{\lambda_c}{\lambda_t} \H_\lambda^{(c)}$ \hspace{5mm} $\Rightarrow\ \mathcal{O} \sim (\bar{ c} b)(\bar{ s} c)$ + +} + +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{frame} +<<<<<<< HEAD %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}\frametitle{Disclaimer } \ARROW arXiv::1603.04355 @@ -2088,6 +2360,202 @@ \includegraphics[width=0.9\textwidth]{images/reson.png}\\ \end{columns} +======= +\begin{frame}{Analytic structure of $\H_\lambda(q^2)$} + +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{3mm} + + +Neglecting OZI- and CKM-suppressed contributions : + +\begin{center} +\includegraphics[width=7.5cm]{Analyticq2.png} +\end{center} + + +$\displaystyle { \hat{\mathcal{H}}_\lambda(q^2)} = (q^2 - M_{J/\psi}^2)(q^2 -M_{\psi(2S)}^2) \,{ {\mathcal{H}}_\lambda(q^2)} \quad $ has no poles. + +\end{frame} + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} + +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{2mm} + +\btr Conformal mapping : \hspace{5mm} $q^2 \mapsto \ z\,(q^2) = \frac{\sqrt{t_+ - q^2} - \sqrt{t_+ - t_0}}{\sqrt{t_+ - q^2} + \sqrt{t_+ - t_0}}$ + +\mbox{ +\hspace{-10mm} +\raisebox{8mm}{\includegraphics[width=5.6cm]{Analyticq22.png}} +\hspace{1mm} +\includegraphics[width=6.5cm]{Analyticz.png} +} + +\vspace{-7mm} + +\btr ${\red \hat \H_\lambda (q^2(z))}$ is {\bf analytic in $|z|<1$}\\[3mm] + +\btr Taylor expand $\red \hat{\H}_\lambda(z)$ around $z=0$.\\[3mm] + +\btr Expansion needed for $|z| < 0.52\ $ ( $-7\,\GeV^2 \leq q^2 \leq 14 \GeV^2$ ) + + +\end{frame} + + + + +\begin{frame}{Accessing $q^2 > 0$ : $\ z\ $ expansion} +\small +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} + +\vspace{3mm} + + +\hspace{-5mm} {\bf \brown Some details for actual parametrisation :} + +\mbox{\hspace{-5mm} \btr Try to capture most features of the expansion (better convergence)} + +\mbox{\hspace{-5mm} \btr Parametrize the ratios $\H_\lambda(q^2)/\F_\lambda(q^2)$ instead} + +\mbox{\hspace{-5mm} \btr The poles should not modify the asymptotic behaviour at $|q^2|\to \infty$} + +\begin{eqnarray} +\H_\lambda(z) &=& +\frac{1-z\, z^*_{J/\psi}}{z-z_{J/\psi}} \frac{1-z\,z^*_{\psi(2S)}}{z-z_{\psi(2S)}} \ \hat\H_\lambda(z) +\nonumber\\[2mm] +% +\hat\H_\lambda(z) &=& \Big[ \sum_{k=0}^K \alpha_k^{(\lambda)} z^{k} \Big] \F_\lambda(z) +\nonumber +\end{eqnarray} + + +where $\alpha^{(\lambda)}_k$ are complex coefficients, and the expansion is truncated after the term $z^{K}$. +We will take $K=2$ ({\brown 16} real parameters). + + +\end{frame} + + + + +\begin{frame}{Experimental constraints on $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\Cite{Bobeth, Chrzaszcz, van Dyk, Virto 1707.07305} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown Experimental constraints :} + +\mbox{\hspace{-5mm} \btr The residues of the poles are given by $B\to K^* \psi_n$ :} + +$$ +\H_\lambda(q^2 \to M_{\psi_n}^2) \sim +\frac{M_{\psi_n} f^{\,*}_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2 (q^2 - M_{\psi_n}^2)} + \cdots +$$ + +\mbox{\hspace{-5mm} \btr Angular analyses \Cite{Belle, Babar, LHCb} determine : } + +$$ +|r_\perp^{\psi_n}|,\, +|r_\|^{\psi_n}|,\, +|r_0^{\psi_n}|,\, +\arg\{r_\perp^{\psi_n} r_{0}^{\psi_n*}\},\, +\arg\{r_\|^{\psi_n} r_{0}^{\psi_n*}\}, +$$ + +where $\quad \displaystyle r_\lambda^{\psi_n} \equiv \operatorname*{Res}_{q^2\to M^2_{\psi_n}} \frac{\H_\lambda(q^2)}{\F_\lambda(q^2)} +\sim +\frac{M_{\psi_n} f^*_{\psi_n} \A^{\psi_n}_\lambda}{M_B^2\, \F_\lambda(M_{\psi_n}^2)}$\\[3mm] + + +\mbox{\hspace{-5mm} \btr We produce correlated pseudo-observables from a fit (5+5).} + + + +\end{frame} + + + + +\begin{frame}{Prior Fit to $\ z\ $ parametrisation } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown (Prior) Fit to Experimental and theoretical pseudo-observables :} + + + +\begin{table}[b] +% \resizebox{.85\textwidth}{!}{% +\centering +\renewcommand{\arraystretch}{1.5} +\renewcommand{\tabcolsep}{3.1mm} +\begin{tabular}{@{}crrr@{}} +\hline +$k$ & 0\hspace{7mm} & 1\hspace{7mm} & 2\hspace{7mm} \\ +\hline +%re perp +${\rm Re}[\alpha_{k}^{(\perp)}]$ & $-0.06 \pm 0.21$ & $-6.77 \pm 0.27$ & $18.96 \pm 0.59$ \\ +%re para +${\rm Re}[\alpha_{k}^{(\parallel)}]$ & $-0.35 \pm 0.62$ & $-3.13 \pm 0.41$ & $12.20 \pm 1.34$ \\ +%re long +${\rm Re}[\alpha_{k}^{(0)}]$ & $0.05 \pm 1.52$ & $17.26 \pm 1.64$ & -- \\ +%im perp +${\rm Im}[\alpha_{k}^{(\perp)}]$ & $-0.21 \pm 2.25$ & $1.17 \pm 3.58$ & $-0.08 \pm 2.24$ \\ +%im para +${\rm Im}[\alpha_{k}^{(\parallel)}]$ & $-0.04 \pm 3.67$ & $-2.14 \pm 2.46$ & $6.03 \pm 2.50$ \\ +%im long +${\rm Im}[\alpha_{k}^{(0)}]$ & $-0.05 \pm 4.99$ & $4.29 \pm 3.14$ & -- \\ +\hline +\end{tabular} +% } +\caption{Mean values and standard deviations (in units of $10^{-4}$) +of the prior PDF for the parameters $\alpha_k^{(\lambda)}$.} +\label{alphak} +\end{table} + +\end{frame} + +\begin{frame}{New Physics Analysis } +\small + +\vspace{-1mm} +\hspace{-5mm} +\vspace{1mm} + +\hspace{-5mm} {\bf \brown SM predictions and Fit including $B\to K^* \mu^+\mu^-$ data and $\C{9}^{\rm NP}$ :}\\[4mm] + +\mbox{ +\hspace{-10mm} +\includegraphics[width=12cm]{NPFit.png} +} + +The NP hypothesis with {\red $\C{9}^{\bf NP}\sim -1$} is favored strongly in the global fit + +\end{frame} + + +\begin{frame}{If NP, what kind?} + +\begin{center} +\includegraphics[width=0.75\textwidth]{images/criv.png} +\end{center} + + +\ARROW Stolen from A.Crivelin \\ +\ARROW For more comprehensive review see G.Isidori talk:\\ +\href{https://indico.cern.ch/event/646856/contributions/2716924/attachments/1556310/2447567/Implication17b.pdf}{\color{blue}LHCb implications Workshop 2017} +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{frame} @@ -2107,7 +2575,10 @@ ''... when you have eliminated all the\\ Standard Model explanations, whatever remains,\\ however improbable, must be New Physics.''\\ +<<<<<<< HEAD prof. Joaquim Matias +======= +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \end{minipage} \vspace*{2.1cm} @@ -2143,6 +2614,52 @@ +<<<<<<< HEAD +======= +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Angular analysis of $\PBzero \to \PKstar \Pe \Pe$} +{~} +\only<1>{ + \begin{minipage}{\textwidth} + \begin{itemize} + \item With the full data set ($3\invfb$) we performed angular analysis in $0.0004 < q^2 <1~\GeV^2$. + \item Electrons channels are extremely challenging experimentally: + \begin{itemize} + \item Bremsstrahlung. + \item Trigger efficiencies. + \end{itemize} + \item Determine the angular observables: $\FL$, $\ATD$, $\ATRe$, $\ATIm$: + \end{itemize} +\begin{equation} + \label{eq:physPars} + \begin{split} + \FL &=\frac{|A_0|^2}{|A_0|^2+|A_{||}|^2 + |A_\perp|^2}\\ + \ATD &= \frac{|A_\perp|^2-|A_{||}|^2}{|A_\perp|^2+|A_{||}|^2}\\ + \ATRe &= \frac{2\Real(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}\\ + \ATIm &= \frac{2\Imag(A_{||L}A^*_{\perp L} + A_{||R}A^*_{\perp R})}{|A_{||}|^2 + |A_\perp|^2}, +\end{split}\nonumber +\end{equation} + +\end{minipage} +} +\only<2>{ +\begin{center} +\includegraphics[width=0.5\textwidth]{images/Kstee.png}\\ +\end{center} +\begin{itemize} +\item Results in full agreement with the SM. +\item Similar strength on $C_7$ Wilson coefficient as from $\Pbeauty \to \Pstrange \Pphoton$ decays. +\end{itemize} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/Kstee2.png} +\end{center} + +} + \vspace*{2.1cm} +\end{frame} + +>>>>>>> 9c58c1659aaebab98c7c85048cc51a00edd80a75 \backupend \end{document} diff --git a/Seminars/UJ/mchrzasz.toc b/Seminars/UJ/mchrzasz.toc new file mode 100644 index 0000000..baf3b21 --- /dev/null +++ b/Seminars/UJ/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.36pt} +\defcounter 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