diff --git a/PTF2016/Makefile b/PTF2016/Makefile new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/PTF2016/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/PTF2016/beamercolorthemeFlip.sty b/PTF2016/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/PTF2016/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/PTF2016/beamerinnerthemeFlip.sty b/PTF2016/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/PTF2016/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/PTF2016/beamerouterthemeFlip.sty b/PTF2016/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/PTF2016/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/PTF2016/beamerouterthemedecolines.sty b/PTF2016/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/PTF2016/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/PTF2016/beamerthemeFlip.sty b/PTF2016/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/PTF2016/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/PTF2016/hql/AFBPad.pdf b/PTF2016/hql/AFBPad.pdf new file mode 100644 index 0000000..50ecb99 --- /dev/null +++ b/PTF2016/hql/AFBPad.pdf Binary files differ diff --git a/PTF2016/hql/BDT.png b/PTF2016/hql/BDT.png new file mode 100644 index 0000000..c39c321 --- /dev/null +++ b/PTF2016/hql/BDT.png Binary files differ diff --git a/PTF2016/hql/P5pPad.pdf 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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[absolute,overlay]{textpos} + +\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{\apeLR}{{A_\perp^{L,R}}} +\newcommand{\apaL}{{A_\|^L}} +\newcommand{\apaR}{{A_\|^R}} +\newcommand{\apaLR}{{A_\|^{L,R}}} +\newcommand{\azeL}{{A_0^L}} +\newcommand{\azeR}{{A_0^R}} +\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\cgreen{\color{green}} +\definecolor{green}{rgb}{0.2,0.6,0.2} + + +\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} + +\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{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich, IFJ PAN)} +\institute{UZH, IFJ PAN} +\title[Overview of LHCb results]{Overview of LHCb results} +\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 \LARGE {Overview of LHCb results} + \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}{on behalf of the LHCb collaboration,\\ Universit\"{a}t Z\"{u}rich, \\ Institute of Nuclear Physics, Polish Academy of Science}\normalsize\\ +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{Katowice, 13-15 May 2016} +\end{center} +\end{frame} +} + + + + +\begin{frame}{Flavour Physics, WHAT, WHY HOW?} + + \begin{minipage}{\textwidth} +\begin{footnotesize} +{~}\\ +\ARROW WHAT: Quarks and leptons exists in 6 ''flavours'' (u,c,t,d,s,b) and (e,$\mu$, $\tau$, $\nu_e$, $\nu_{\mu}$, $\nu_{\tau}$).\\ +\ARROW WHY: +\begin{itemize} +\item Flavour is the heart of SM. It involves $22$ from $28$ free parameters, like masses mixing and CP violation. +\item Flavour physics loop processes (box and penguins) are sensitive to energy scales well beyond the ones of the accelerators, thanks to virtual contributions. +\end{itemize} +\begin{center} +\includegraphics[width=0.8\textwidth]{images/mglass.png} +\end{center} +\ARROW HOW: +\begin{itemize} +\item Compare precise theoretical predictions with precise experimental measurements. +\item LHCb, Belle, BaBar, ATLAS, CMS, NA62, BESIII, neutrinos experiments,... +\end{itemize} + + + +\end{footnotesize} +\end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\iffalse + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{Why rare decays?} +\begin{columns} +\column{4in} +\begin{itemize} +\item In SM allows only the charged interactions to change flavour. +\begin{itemize} +\item Other interactions are flavour conserving. +\end{itemize} +\item One can escape this constrain and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. +\begin{itemize} +\item This 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]{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} + + +\fi + +\begin{frame}{Searching for New Physics} + \begin{minipage}{\textwidth} +\begin{footnotesize} +{~}\\{~}\\ +\ARROW The fundamental questions: +\begin{itemize} +\item Why 3 generations? Why such hierarchy structure? +\item Stability of the Higgs vacum? Dark Matter? +\item Baryon asymmetry of the universe? CP in SM is to small! +\end{itemize} +\pause +\ARROW Two ways to answer them: +\begin{itemize} +\item Direct searches: try to produce directly new real particles ''on-shell'', but we don’t +know their mass or lifetime and we are limited by the center-of-mass energy of +accelerator. +\item Indirect searches: study the effect of “off-shell” (virtual) particles within quantum +loop. Compare precise theoretical predictions with precise experimental measurements. Not limited by the center-of-mass energy of accelerator. It happened in the past: +\begin{itemize} +\item CP violation in the Kaon system: existence of $\Pbeauty$ and $\Ptop$ quarks. +\item Lack of observation of $\PKs \to \mu \mu$: existence of $\Pcharm$ quark. +\item Neutral weak currents: existence of $\PZ$ boson. +\end{itemize} +\item Very powerful tool! +\end{itemize} +\end{footnotesize} +\end{minipage} + \vspace*{2.cm} +\end{frame} + + + +\begin{frame}{Selected physics results:} + \begin{minipage}{\textwidth} +\begin{footnotesize} +{~}\\{~}\\ +\begin{itemize} +\item Rare Decays +\begin{itemize} +\item $\PBs/ \PBd \to \Pmu \Pmu$ +\item $\PBd \to \PKstar \Pmu \Pmu$, $\PBs \to \Pphi \Pmu \Pmu$, $\PLambdab \to \PLambda \Pmu \Pmu$. +\end{itemize} +\item Tests of lepton universalities: +\begin{itemize} +\item $R_k=\mathcal{B}(\PBplus \to \PKplus \Pmu \Pmu) / \mathcal{B}(\PBplus \to \PKplus \Pe \Pe)$ +\item $R(\PD),~ R(\PDstar)$ +\end{itemize} +\item CP violation: +\begin{itemize} +\item CP violation in $\PBd $ and $\PBs$ +\item CP violation in charm +\item $V_{ub}$ +\end{itemize} +%\item Tetra\&Pentaquarks +\end{itemize} + + +\end{footnotesize} +\end{minipage} + \vspace*{2.cm} +\end{frame} + + +\begin{frame} +\begin{center} +\begin{Huge} +Rare decays +\end{Huge} +\end{center} + + +\end{frame} + + +\begin{frame}\frametitle{Tools} +\begin{itemize} +\item \textbf{Operator Product Expansion and Effective Field Theory} +\end{itemize} +\begin{columns} +\column{0.1in}{~} +\column{1.2in} +\begin{small} +\begin{align*} +H_{eff} = - \dfrac{4G_f}{\sqrt{2}} V V^{\prime \ast}\ \sum_i \left[\underbrace{C_i(\mu)O_i(\mu)}_\text{left-handed} +\underbrace{C'_i(\mu)O'_i(\mu)}_\text{right-handed}\right], +\end{align*} +\end{small} +\column{1.8in} +\begin{tiny} +\begin{description} + \item[i=1,2] Tree + \item[i=3-6,8] Gluon penguin + \item[i=7] Photon penguin + \item[i=9,10] EW penguin + \item[i=S] Scalar penguin + \item[i=P] Pseudoscalar penguin + \end{description} + +\end{tiny} +\end{columns} +where $C_i$ are the Wilson coefficients and $O_i$ are the corresponding effective operators. +\begin{center} +\includegraphics[width=0.85\textwidth,height=3cm]{images/all.png} + +\end{center} + + +\end{frame} + + + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PB_{d,s} \rightarrow \Pmu^+ \Pmu^-$} +\begin{columns} +\column{3.2in} + +\begin{itemize} +\item Clean theoretical prediction, GIM and helicity suppressed in the SM: +\begin{itemize} +\item $\mathcal{B}(\PBs \to \Pmuon \APmuon) = (3.65 \pm 0.23)\times 10^{-9}$ +\item $\mathcal{B}(\PBzero \to \Pmuon \APmuon) = (1.06 \pm 0.09)\times 10^{-10}$ +\end{itemize} +\item Sensitive to contributions from scalar and pesudoscalar couplings. +\item Probing: MSSM, higgs sector, etc. +\item In MSSM: $\mathcal{B}(\PBs \to \Pmuon \APmuon) \sim \tan^6 \beta /m_A^4$ +\item Theory errors dominated by the form factors! Will go down in the future. +\end{itemize} + +\column{1.5in} +{~} +\includegraphics[width=0.95\textwidth]{hql/bs2mumu1.png}\\ +\includegraphics[width=0.95\textwidth]{hql/bs2mumu2.png}\\ +\includegraphics[width=0.6\textwidth]{hql/higgspen.png} +\end{columns} + + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PBzero \rightarrow \Pmu^+ \Pmu^-$ Results} + + + +\begin{columns} +\column{2.in} +\begin{itemize} +\item Nov. 2012: +\begin{itemize} +\item First evidence $3.5\sigma$ for $B^0 \rightarrow \mu^+ \mu^-$. with $2.1~\rm fb^{-1}$. +\end{itemize} +\item Summer 2013: +\begin{itemize} +\item Full data sample: $3~\rm fb^{-1}$. +\end{itemize} +\end{itemize} +\column{3.0in} + +\includegraphics[width=0.95\textwidth]{hql/mass2.png} + +\end{columns} +\begin{itemize} +\item Measured BF:\\ $\mathcal{B}(\PBs \to \Pmuon \APmuon) =(2.9^{+1.1}_{-1.0}(stat.)^{+0.3}_{-0.1}(syst.))\times 10^{-9}$ +\item $4.0 \sigma$ significance! +\item $\mathcal{B}(\PBzero \to \Pmuon \APmuon) < 7 \times 10^{-10}$ at $95\%$ CL +%\item \href{http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.110.021801}{\color{blue} PRL 110 (2013) 021801 } +\item \href{http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.111.101805}{\color{blue} CMS result: PRL 111 (2013) 101805} +\end{itemize} + +\textref{ PRL 110 (2013) 021801} +\end{frame} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{LHCb+CMS Combination} +\begin{columns} +\column{3in} +\begin{large} +\begin{center} +$\mathcal{B}(\PBs \to \Pmuon \APmuon) =(2.8^{+0.7}_{-0.6} )\times 10^{-9}$\\ +$\mathcal{B}(\PBzero \to \Pmuon \APmuon) =(3.9^{+1.6}_{-1.4} )\times 10^{-10}$ +\end{center} +\end{large} +\column{2in} +\includegraphics[width=0.95\textwidth]{images/nature.png} +\end{columns} + + +\includegraphics[width=0.95\textwidth]{hql/bs2mumu_comb.png} +\ARROW $2.3~\sigma$ compatibility with SM! + + +\textref{Nature 522 (2015) 68} + +\end{frame} + + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{$\PBd \to \PKstar \Pmu \Pmu$} +\begin{footnotesize} + +{~}\\ +\begin{minipage}{\textwidth} +\ARROW The decay of $\PBd \to \PKstar \Pmu \Pmu$ has number of angular observables that are sensitive to different Wilson coefficients: $C_7^{(\prime)},~C_9^{(\prime)},~C_{10}^{(\prime)}$.\\ +\ARROW The complete angular expression is given by: +\iffalse +{\tiny{ +\begin{align*} +\label{dist} + \dfrac{1}{d \Gamma /dq^2} \frac{d^4\Gamma}{dq^2\,d\!\cos\theta_K\,d\!\cos\theta_l\,d\phi} = \frac9{32\pi}[ \frac{3}{4}(1- {\color{red}{F_L}} \sin^2\theta_K + {\color{red}{F_L}} \cos^2\theta_K + \\ \frac{1}{4} (1-{\color{red}{F_L }} )\sin^2\theta_K \cos 2\theta_l \\ - {\color{red}{F_L}} \cos^2\theta_K \cos 2\theta_l + {\color{red}{S_3}} \sin^2\theta_K \sin^2\theta_l \cos 2\phi + {\color{red}{S_4}} \sin 2\theta_K \sin 2\theta_l \cos\phi + {\color{red}{S_5}} \sin 2\theta_K \sin\theta_l \cos\phi \\ + ({\color{red}{S_{6s}}} \sin^2\theta_K + {\color{red}{{S_{6c}}}} \cos^2\theta_K) \cos\theta_l + {\color{red}{S_7}} \sin 2\theta_K \sin\theta_l \sin\phi + {\color{red}{S_8}} \sin 2\theta_K \sin 2\theta_l \sin\phi + {\color{red}{S_9}} \sin^2\theta_K \sin^2\theta_l \sin 2\phi ] +\end{align*} +}} +\fi +\begin{center} +\includegraphics[width=0.85\textwidth]{images/angles4.png} +\end{center} +\ARROW Furthermore, one can construct a form factor free observables: +\begin{align*} +P_5^{\prime}=\frac{S_5}{F_L(1-F_L)} +\end{align*} + + +\end{minipage} +\vspace*{2.1cm} + \vspace*{2.1cm} + \end{footnotesize} +\textref{JHEP, 1305:137, (2013)} + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + +\begin{frame}{$\PBd \to \PKstar \Pmu \Pmu$ results} +{~} +\begin{footnotesize} + \begin{minipage}{\textwidth} + + +\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}\\ +\ARROW $S_7$, $S_8$, $S_9$ are zero in the SM! + +} + + +\end{center} + +\end{minipage} +\end{footnotesize} + \textref{JHEP 02 (2016) 104} + + \vspace*{2.1cm} +\end{frame} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{$\PBd \to \PKstar \Pmu \Pmu$ results} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[width=0.65\textwidth]{images/p5pbelle.png}\\ + \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 results and Belle! +\item SM: \href{http://arxiv.org/abs/1407.8526}{\color{blue}JHEP12(2014)125} +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} + \textref{arxiv:1604.04042} + +\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} + \textref{JHEP 02 (2016) 104} + + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{BF 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} + \textref{JHEP 07 (2012) 133} + + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{BF of $\PBs \to \Pphi \Pmu \Pmu$} +{~} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[width=0.65\textwidth]{images/bs2phipi.png}\\ + \end{center} + +\begin{itemize} +\item Last years LHCb measurement. %\href{http://arxiv.org/abs/1506.08777}{{\color{blue}{JHEP09 (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} +\textref{JHEP09 (2015) 179} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{BF 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=0.55\textwidth]{images/Lblow.png} +\includegraphics[width=0.55\textwidth]{images/Lbhigh.png} + +} + + + \end{center} + + +\begin{itemize} +\item Last years LHCb measurement.% [{\color{blue}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} +\textref{JHEP 06 (2015) 115} + \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} +\textref{JHEP 06 (2015) 115} + + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Lepton Universlaity tests +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame} +{~} + \begin{minipage}{\textwidth} + +\begin{center} +\begin{Huge} +Lepton Universality tests +\end{Huge} +\end{center} + + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Lepton universality test} +{~} + \begin{minipage}{\textwidth} +\begin{columns} +\column{3.0in} +\begin{itemize} +\item Does the NP couple equally to all flavours? +\includegraphics[width=0.99\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}\\ +\includegraphics[width=0.95\textwidth]{images/diagramsRK.png} + +\end{columns} + + + +\end{minipage} + \vspace*{2.1cm} +\textref{Phys. Rev. Lett. 113, 151601 (2014)} + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{More Lepton universality tests} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item There is one other LUV decay recently measured by LHCb. +\item $R(\PDstar)=\dfrac{\mathcal{B}(\PB \to \PDstar \Ptau \Pnu)}{\mathcal{B}(\PB \to \PDstar \Pmu \Pnu)}$ +\item Clean SM prediction: $R(\PDstar)=0.252(3)$, PRD 85 094025 (2012) +\item LHCb result: $R(\PDstar)= 0.336 \pm 0.027 \pm 0.030$ +\item HFAG average: $R(\PDstar)=0.322 \pm 0.022$ +\item $4.0~\sigma$ discrepancy wrt. SM. +\end{itemize} + +\begin{center} + +\includegraphics[width=0.48\textwidth]{images/RDstar.png} + +\end{center} +%\textref{http://www.slac.stanford.edu/xorg/hfag/index.html} + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Explanation of anomalies} +{~} + \begin{minipage}{\textwidth} + \ARROW Thanks to S. Descotes-Genon, L.Hofer, J.Matias, J.Virto we have a global fit to the anomalies.\\ + \begin{center} + \includegraphics[width=0.75\textwidth]{images/quim2.png} + \end{center} +\ARROW The fit prefer a modification of $C_9$ Wilson coefficient with a value of $C_9^{NP}=-1$, with a significance over $4\sigma$.\\ +%\ARROW Many theories link might accommodate the observed deviations. + +\textref{arXiv:1510.04239} + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Explanation of anomalies} +{~} + \begin{minipage}{\textwidth} + +\begin{itemize} +\item We are not there yet! +\item There might be something not taken into account in the theory. +\item Resonances ($\PJpsi$, $\Ppsi(2S)$) tails can mimic NP effects. +\item There might be some non factorizable QCD corrections.\\ +'' However, the central value of this effect would have to be significantly larger than expected on the basis of existing estimates'' \texttt{D.Straub, 1503.06199} +. +\end{itemize} + +\includegraphics[width=0.9\textwidth]{images/charmloop.png} + + + + \end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%% CP violation +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +\begin{frame}{Mixing induced CPV in $\PBs$} +{~} +\begin{small} + + \begin{minipage}{\textwidth} +\ARROW Interference between $\PBs$ decaying to $\PJpsi \Pphi$ either directly or by oscillations gives rise to CP violation phase: $\phi_s^{\PJpsi \Pphi}$ +\begin{center} +\includegraphics[width=0.85\textwidth]{images/phis.png} +\end{center} +\ARROW In the SM $\phi_s \approx -2 \beta_s = -(0.0376^{+0.0007}_{-0.0008})~\rm rad$, where $\beta_s=\arg \left(- \frac{V_{ts}V_{tb}^{\ast}}{V_{cs} V_{cb}^{\ast}} \right)$\\ +\ARROW At the leading order same phase is expected $\PBs \to \PDs \PDs$ and $\PB \to \PJpsi \Ppi \Ppi$.\\ +\ARROW NP can enter in the $\PBs$ mixing!\\ +\ARROW Measured by simultaneous fit to $\PBs$ and $\bar{\PBs}$ decay rates: +\begin{center} +\includegraphics[width=0.9\textwidth]{images/phis2.png} + +\end{center} + + \end{minipage} + \end{small} + + + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Mixing induced CPV in $\PBs$} +{~} +\begin{footnotesize} + + + \begin{minipage}{\textwidth} +\ARROW Unbinned maximum likelihood fit (time, mass, angles, initial flavour): +\begin{center} +\includegraphics[width=0.6\textwidth]{images/Bsmix.png} +\end{center} +\begin{itemize} +\item $\phi_s=-0.058 \pm 0.049 \pm 0.006$ rad. +\item $\Gamma_s=(\Gamma_L+\Gamma_H)/2=0.6603\pm 0.0027 \pm 0.0015~ {\rm ps}^{-1}$ +\item $\Delta \Gamma_s=\Gamma_L-\Gamma_H=0.0805 \pm 0.0091 \pm 0.0032~ {\rm ps}^{-1}$ +\item Combined with $\PBs \to \PJpsi \pi \pi$: $\phi_s=-0.010 \pm 0.039$ rad. +\end{itemize} + + \end{minipage} +\end{footnotesize} + +\textref{PRL 114, 041801 (2015)} + \vspace*{2.1cm} +\end{frame} + + + + +\begin{frame}{Mixing induced CPV in $\PBs$} +{~} +\begin{footnotesize} + +\begin{center} +\includegraphics[width=0.7\textwidth]{images/hfagccs.png} +\end{center} +\ARROW LHCb is dominating the world average!\\ +\ARROW $\phi_s^{ \rm HFAG}=-0.034 \pm 0.033$.\\ +\ARROW Compatible with SM, but there is still plenty room for NP!\\ +\ARROW Penguin pollution constrained from $\PBzero \to \PJpsi \Prho$ and $\PBs \to \PJpsi \bar{\PKstar}$ + +\end{footnotesize} + + \vspace*{2.1cm} +\end{frame} + + + + +\begin{frame}{$V_{ub}$} +{~} +\begin{footnotesize} + +\ARROW Since a long time the smallest of the CKM matrix elements $V_{ub}$ has been determined in two ways: +\begin{itemize} +\item inclusively: $\Pbeauty \to \Pup \ell \nu$, $\vert V_{ub} \vert=(4.41 \pm 0.15^{+0.15}_{-0.17})\times 10^{-3}$ +\item exclusively: $\PB \to \pi \ell \nu$, $\vert V_{ub} \vert=(3.28 \pm 0.29)\times 10^{-3}$ +\item $3~\sigma$ tensions! +\end{itemize} +\ARROW LHCb perspectively enters the game with baryons decay: $\PLambdab \to \Pproton \mu \nu$. +\begin{center} +\includegraphics[width=0.45\textwidth]{images/vub.png} +\end{center} +where $R_{FF}$ is a ratio of form factors, that can be calculated using lattice QCD [arxiv:1503.01421]. +\end{footnotesize} + +\textref{Nature Physics 11, 743-747 (2015)} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{$V_{ub}$} +{~} +\begin{footnotesize} + +\ARROW $\vert V_{ub}\vert = (3.27 \pm0.15 \pm 0.16 \pm 0.06(V_{cb})) \times 10^{-3}$ + +\begin{center} +\includegraphics[width=0.95\textwidth]{images/vub2.png} +\end{center} + +\begin{itemize} +\item LHCbs measurement makes the discrepancy larger and is spot on the Exclusive B-factories results. +\item Disfavor NP models with significant right handed current +\item Debatable world averages, depending on the input used (theory, BR of control mode, ...) +\end{itemize} + + + +\end{footnotesize} + +\textref{Nature Physics 11, 743-747 (2015)} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{CP violation in charm} +{~} +\begin{footnotesize} + +\ARROW The $A_{CP}$ asymmetry is defined as: +\begin{align*} +A_{CP}(\PDzero \to f) = \frac{\Gamma(\PDzero \to f)-\Gamma(\bar{\PDzero} \to f) }{\Gamma(\PDzero \to f)+\Gamma(\bar{\PDzero} \to f) },~~~f=\PK^+ \PK^- ,\Ppi^+ \Ppi^- +\end{align*} +\begin{center} +\includegraphics[width=0.65\textwidth]{images/charmCP.png} +\end{center} +\ARROW New world average: +\begin{align*} +a_{CP}^{ \rm ind}=(0.056 \pm 0.040)\% \\ +a_{CP}^{ \rm dir}=(-0.137 \pm 0.070)\% +\end{align*} +\ARROW Results consistent with no CPV at $6.5~\%$ CL. +\end{footnotesize} + +\textref{LHCb-PAPER-2015-055, PLB 753 (2016) 412} + + \vspace*{2.1cm} +\end{frame} + + + + + + +\begin{frame}{Conclusions} +{~} +\begin{small} + +\ARROW Flavour physics is still playing an important role for hunting new physics!\\ +\ARROW Anomalies in the electroweak penguin and lepton universality combine to over $4\sigma$ significance discrepancy for NP.\\ +\ARROW The dominant anomaly was recently confirmed by Belle experiment!\\ +\ARROW Most precise measurements of CP violations in $\PBs$ system.\\ +\ARROW First $V_{ub}$ determination from baryon decays!\\ +\ARROW Stay tuned as there are plenty of more results in the pipe line! + + + +\end{small} + + \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}{Theory implications} +{~} + \begin{minipage}{\textwidth} + +\includegraphics[height=0.9\textheight]{images/table.png} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{If not NP?} +{~} +\begin{minipage}{\textwidth} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +\begin{itemize} +\item How about our clean $P_i$ observables? +\item The QCD cancel as mentioned only at leading order. +\item Comparison to normal observables with the optimised ones. +\end{itemize} +\includegraphics[width=0.9\textwidth]{images/C9_S_P.png} + + +\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 (soft form factors): +{\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}{Mass modelling} +{~} +\begin{minipage}{\textwidth} +\begin{small} + +\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.\\ +\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} +\begin{center} +\includegraphics[angle=-90,width=0.9\textwidth]{images/msignal.pdf}\\ + +\end{center} +\ARROW The S-wave fraction is extracted using a \texttt{LASS} model. +\end{columns} + +\end{small} +\end{minipage} + \vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\iffalse +%%%%%%%%%%%%%%% +\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. + +\end{itemize} +%\includegraphics[width=0.75\textwidth]{images/q2PHSP.png} + + + +\column{0.4\textwidth} +%\only<1>{ +%\includegraphics[width=0.99\textwidth]{images/q2PHSP.png}\\ +%\includegraphics[width=0.99\textwidth]{images/q2PHSPw.png} +%} + +\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}{$\PBd \to \PKstar \Pmu \Pmu$ 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} +\textref{JHEP 02 (2016) 104} + + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Maximum likelihood fit - Results} +{~} + \begin{minipage}{\textwidth} +\begin{center} +\only<1>{ +\includegraphics[angle=-90,width=0.45\textwidth]{images/FLPad.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{images/S3Pad.pdf}\\ +\includegraphics[angle=-90,width=0.45\textwidth]{images/S4Pad.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{images/S5Pad.pdf} +} +\only<2>{ +\includegraphics[angle=-90,width=0.45\textwidth]{images/AFBPad.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{images/S7Pad.pdf}\\ +\includegraphics[angle=-90,width=0.45\textwidth]{images/S8Pad.pdf} +\includegraphics[angle=-90,width=0.45\textwidth]{images/S9Pad.pdf} +} + + +\end{center} + \ARROW SM: \href{http://arxiv.org/abs/1411.3161}{ {\color{blue}Eur.Phys.J. C75 (2015) no.8, 382 }} + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\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}{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}}, U. Egede, M. Patel, K.A. Petridis.\\ +\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} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PBzero \rightarrow \Pmu^+ \Pmu^-$ searches} + + +\begin{columns} +\column{5in} + +\begin{itemize} +\item Background rejection power is a key feature of rare decays $\rightarrow$ use multivariate classifiers (BDT) and strong PID. +\end{itemize} +\column{0.1in}{~} + +\end{columns} +\begin{columns} +\column{2.5in} +\includegraphics[width=0.95\textwidth]{hql/BDT.png} + +\column{2.5in} + +\includegraphics[width=0.95\textwidth]{hql/mass.png} + +\end{columns} + +\begin{itemize} +\item Normalize the BF to $\PBplus \to \PJpsi(\mu\mu) \PKplus$ and $\PBzero \to \PK \Ppi$. +\end{itemize} +\textref{ PRL 111 (2013) 101805} + +\end{frame} + + + + + +\begin{frame}{Tetra\&Petraquarks} +{~} +\ARROW Idea of this multi quark states started in the $1960$s: +\begin{center} +\includegraphics[width=0.7\textwidth]{images/gelman.png} +\end{center} +\ARROW Searches for years and many “discoveries” not confirmed + \vspace*{2.1cm} +\end{frame} + + + +\iffalse +\begin{frame}{X(3872)} +{~} +\begin{footnotesize} + + +\begin{columns} +\column{0.1in} +{~}\\ +\column{2.5in} +\ARROW First observed by Belle in $\PB^+ \to X(\PJpsi \pi \pi) \PK^+$, above the $\PUpsilon(2S)$. [PRL 91 (2003) 262001]\\ +\ARROW Confirmed by several experiments: BaBar, CDF, D0, LHCb, CMS.\\ +\ARROW LHCb determined its quantum numbers: $J^{PC}=1^{++}$ using angular analysis [PRL 110, 222001 (2013)].\\ +{~}\\ +\ARROW The nature of this state is still unclear. It is compatible with a tetraquark, $\PD\PDstar$ molecule or a $\chi_{c1}(2^3P_1)$ hypothesis.\\ +\ARROW Never LHCb measurements disfavour the $\PD\PDstar$ molecule by $4.4~\sigma$ [Nucl. Phys. B886 (2014) 665]. + +\column{2.5in} +\includegraphics[width=0.95\textwidth]{images/x3872.png} +\end{columns} +\end{footnotesize} + + \vspace*{2.1cm} +\end{frame} +\fi + + +\begin{frame}{$Z(4430)^-$} +{~} +\begin{footnotesize} + + +\begin{columns} +\column{0.1in} +{~}\\ +\column{2.5in} +\ARROW $Z(4430)^-$ special “tetraquark candidate”,because charged: cannot be a $\Pcharm \bar{\Pcharm}$ state!\\ +\ARROW Belle discovered it in $\PBzero \to \PUpsilon(2S)\PK \Ppi$, with evidence of $J^{P}=1^+$ [PRD 88 (2013) 074026]. \\ +\ARROW Using method of moments, Babar claimed they do not need the $Z(4430)^-$ to described their data [PRD 79 (2009) 112001].\\ +\ARROW LHCb reproduced BaBar moments analysis with the full Run1 sample ($3~\invfb$) and clearly something mote was needed to describe the data [PRL 112, 222002 (2014)].\\ + +\column{2.5in} +\includegraphics[width=0.95\textwidth]{images/Z4430.png} +\end{columns} +\end{footnotesize} + + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{$Z(4430)^-$} +{~} +\begin{footnotesize} +\ARROW LHCb unbinned amplitude analysis of $\PBzero \to \Ppsi(2S) \PK^+ \Ppi^-$, $m=4475 \pm 7 ^{+15}_{-25}~\MeV/c^2$, $\Gamma=172 \pm 13^{37}_{34}~\MeV/c^2$\\ +\ARROW $J^P$ is confirmed to be $1^+$ and Argand plot shows the typical pattern for resonances.\\ +\ARROW Minimal quark content $\Pcharm \APcharm \Pdown \APup$. + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/Z44301.png} +\end{center} + + +\end{footnotesize} +\textref{LHCb, PRL 112, 222002 (2014)} + \vspace*{2.1cm} +\end{frame} + + +\begin{frame}{Pentaquarks in $\PLambdab \to \PJpsi \Pproton \PK$} +{~} +\begin{footnotesize} +\ARROW $\PLambdab \to \PJpsi \Pproton \PK$ was studied initially for a precise $\PLambdab$ lifetime .\\ +\ARROW Close look at the Dalitz: $m(\PK\Pproton)-m(\PJpsi \Pproton)$ +\begin{itemize} +\item $m(\PK\Pproton)$ has a rich structure of excited $\PLambda$ states. +\item $m(\PJpsi \Pproton)$ has something inside! +\end{itemize} + +\begin{center} +\includegraphics[width=0.9\textwidth]{images/penta.png} +\end{center} + + +\end{footnotesize} +\textref{[LHCb, PRL 115 (2015) 072001]} + + \vspace*{2.1cm} +\end{frame} + + + +\begin{frame}{Pentaquarks in $\PLambdab \to \PJpsi \Pproton \PK$} +{~} +\begin{footnotesize} +\ARROW Super complex fit needed to describe the data: $5$ decay angles, $14$ possible $\PLambda^{\ast}$ resonances for $m(\PK \Ppi)$ and two brand new pentaquarks for $m(\PJpsi \Pproton)$: +\begin{itemize} +\item $P_c(4380)^+$: $4380\pm 8 \pm 29~\MeV/c^2$, $\Gamma=205 \pm 18 \pm 86~\MeV/c^2$, $J^P=\frac{3}{2}^-$ +\item $P_c(4450)^+$: $4449,8\pm 1.7 \pm 2.5~\MeV/c^2$, $\Gamma=39 \pm 5 \pm 19~\MeV/c^2$, $J^P=\frac{5}{2}^+$ +\end{itemize} + +\begin{center} +\includegraphics[width=0.95\textwidth]{images/penta2.png} +\end{center} + + +\end{footnotesize} +\textref{[LHCb, PRL 115 (2015) 072001]} + + \vspace*{2.1cm} +\end{frame} + + + + + + +\begin{frame}{Pentaquarks in $\PLambdab \to \PJpsi \Pproton \PK$} +{~} +\begin{footnotesize} +\begin{columns} +\column{3in} +\begin{itemize} +\item Angrad plots show the phase motion for the resonances. +\item The $P_c(4380)$ has one point off by a $2\sigma$. +\end{itemize} + +\column{2in} +\begin{itemize} +\item The interference patterns confirm the opposite parities. +\end{itemize} + +\end{columns} +\begin{center} +\includegraphics[width=0.99\textwidth]{images/penta3.png} +\end{center} + +\ARROW The significance was evaluated with a TOY MC: +\begin{itemize} +\item $P_c(4380)^+:~9\sigma$ +\item $P_c(4450)^+:~12\sigma$ +\end{itemize} +\ARROW The states are consistent with $\Pcharm \APcharm \Pup \Pup \Pdown$.\\ + + +\end{footnotesize} +\textref{[LHCb, PRL 115 (2015) 072001]} + + \vspace*{2.1cm} +\end{frame} + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +% Lepton non universality +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + + + + + + +\backupend +\end{document} diff --git a/PTF2016/mchrzasz.tex~ b/PTF2016/mchrzasz.tex~ new file mode 100644 index 0000000..55f44a1 --- /dev/null +++ b/PTF2016/mchrzasz.tex~ @@ -0,0 +1,1284 @@ +\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 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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}} 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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} + + + +\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, IFJ PAN} +\title[Anomalies in Flavour physics]{Anomalies in Flavour 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}{0.75\textwidth} + \flushright\fontspec{Trebuchet MS}\bfseries \LARGE {Anomalies in Flavour physics} + \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}{Universit\"{a}t Z\"{u}rich, \\ Institute of Nuclear Physics, Polish Academy of Science}\normalsize\\ +\vspace{0.5em} + + \textcolor{normal text.fg!50!Comment}{$5^{th}$ KEK Flavour Factory Workshop \\October 26-27,\\ Tokyo 2015} +\end{center} +\end{frame} +} + + + + +\iffalse + +\begin{frame}{Outline} + + \begin{minipage}{\textwidth} + +\begin{enumerate} +\item Why flavour is important. +\item $\Pbeauty \to \Pstrange \ell \ell$ theory in a nutshell. +\item LHCb measurements of $\Pbeauty \to \Pstrange \ell \ell$. +\item Global fit to $\Pbeauty \to \Pstrange \ell \ell$ measurements. +\item Conclusions. +\end{enumerate} + + +\end{minipage} + \vspace*{2.cm} +\end{frame} + +\fi + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{Why rare decays?} +\begin{columns} +\column{4in} +\begin{itemize} +\item In SM allows only the charged interactions to change flavour. +\begin{itemize} +\item Other interactions are flavour conserving. +\end{itemize} +\item One can escape this constrain and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. +\begin{itemize} +\item This 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]{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}\frametitle{Tools} +\begin{itemize} +\item \textbf{Operator Product Expansion and Effective Field Theory} +\end{itemize} +\begin{columns} +\column{0.1in}{~} +\column{3.2in} +\begin{align*} +H_{eff} = - \dfrac{4G_f}{\sqrt{2}} V V^{\prime \ast}\ \sum_i \left[\underbrace{C_i(\mu)O_i(\mu)}_\text{left-handed} +\underbrace{C'_i(\mu)O'_i(\mu)}_\text{right-handed}\right], +\end{align*} + +\column{2in} +\begin{tiny} +\begin{description} + \item[i=1,2] Tree + \item[i=3-6,8] Gluon penguin + \item[i=7] Photon penguin + \item[i=9.10] EW penguin + \item[i=S] Scalar penguin + \item[i=P] Pseudoscalar penguin + \end{description} + +\end{tiny} +\end{columns} +where $C_i$ are the Wilson coefficients and $O_i$ are the corresponding effective operators. +\begin{center} +\includegraphics[width=0.85\textwidth,height=3cm]{images/all.png} + +\end{center} + + +\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 $\sim~40~\rm fs$.\\ +$\Rightarrow$ 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}{Recent measurements} +{~} +\only<1>{ + + \begin{minipage}{\textwidth} + + +\begin{columns} + +\column{0.5\textwidth} +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Branching fractions:}} +\begin{description} +\item [$\PB^{0,\pm} \to \PK^{0,\pm} \Pmuon \APmuon$] {~}{~}LHCb, Mar 14 +\item [$\PB^{0} \to \PKstar \Pmuon \APmuon$] {~}{~}CMS, Jul 15 +\item [$\PBs \to \Pphi \Pmuon \APmuon$] {~}{~}{~}LHCb, Jun 15 +\item [$\PB^{\pm} \to \Ppi^{\pm} \Pmuon \APmuon$] {~}LHCb, Sep 15 +\item [$\PLambdab \to \PLambda \Pmuon \APmuon$] {~}{~}{~}{~}LHCb, Mar 15 +\item [$\PB \to\Pmuon \APmuon$] {~}{~}{~}{~}{~}CMS+LHCb, Jun 15 +\end{description} + +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{CP asymmetry:}} +\begin{description} +\item [$\PB^{\pm} \to \Ppi^{\pm} \Pmuon \APmuon$] {~}{~}LHCb, Sep 15 +\end{description} + +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Isospin asymmetry:}} +\begin{description} +\item [$\PB \to \PK \Pmuon \APmuon$] {~}{~}{~}{~}{~}LHCb, Mar 14 +\end{description} + + +\column{0.5\textwidth} +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Lepton Universality:}} +\begin{description} +\item [$\PB^{\pm} \to \PK^{\pm} \Plepton \APlepton$] {~}{~}LHCb, Jun 14 +\end{description} + + +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Angular:}} +\begin{description} +\item [$\PB^{0} \to \PK^{\ast} \Plepton \APlepton$] {~}{~}{~}LHCb, Jan 15 +\item [$\PB^{\pm} \to \PK^{\ast,\pm} \Plepton \APlepton$] BaBar, Aug 15 +\item [$\PBs \to \Pphi \Plepton \APlepton$] {~}{~}{~}LHCb, Jun 15 +\item [$\PLambdab \to \PLambda \Pmuon \APmuon$] {~}{~}LHCb, Mar 15 +\end{description} + + + + + +\end{columns} + +\end{minipage} +} +\only<2>{ + + \begin{minipage}{\textwidth} + + +\begin{columns} + +\column{0.5\textwidth} +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Branching fractions:}} +\begin{description} +\item [{\color{red}{$\PB^{0,\pm} \to \PK^{0,\pm} \Pmuon \APmuon$}}] {~}{~}{\color{red}{LHCb, Mar 14}} +\item [$\PB^{0} \to \PKstar \Pmuon \APmuon$] {~}{~}CMS, Jul 15 +\item [{\color{red}{$\PBs \to \Pphi \Pmuon \APmuon$}}] {~}{~}{~}{\color{red}{LHCb, Jun 15}} +\item [$\PB^{\pm} \to \Ppi^{\pm} \Pmuon \APmuon$] {~}LHCb, Sep 15 +\item [$\PLambdab \to \PLambda \Pmuon \APmuon$] {~}{~}{~}{~}LHCb, Mar 15 +\item [{\color{red}{$\PB \to\Pmuon \APmuon$}}] {~}{~}{~}{~}{~}{\color{red}{CMS+LHCb, Jun 15}} +\end{description} + +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{CP asymmetry:}} +\begin{description} +\item [$\PB^{\pm} \to \Ppi^{\pm} \Pmuon \APmuon$] {~}{~}LHCb, Sep 15 +\end{description} + +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Isospin asymmetry:}} +\begin{description} +\item [$\PB \to \PK \Pmuon \APmuon$] {~}{~}{~}{~}{~}LHCb, Mar 14 +\end{description} + + +\column{0.5\textwidth} +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Lepton Universality:}} +\begin{description} +\item [{\color{red}{$\PB^{\pm} \to \PK^{\pm} \Plepton \APlepton$}}] {~}{~}{\color{red}{LHCb, Jun 14}} +\end{description} + + +$\color{JungleGreen}{\Rrightarrow}$ {\color{WildStrawberry}{Angular:}} +\begin{description} +\item [{\color{red}{$\PB^{0} \to \PK^{\ast} \Plepton \APlepton$}}] {~}{~}{~}LHCb, Jan 15 +\item [{\color{red}{$\PB^{\pm} \to \PK^{\ast,\pm} \Plepton \APlepton$}}] {\color{red}{BaBar, Aug 15}} +\item [$\PBs \to \Pphi \Plepton \APlepton$] {~}{~}{~}LHCb, Jun 15 +\item [{\color{red}{$\PLambdab \to \PLambda \Pmuon \APmuon$}}] {~}{~}{\color{red}{LHCb, Mar 15}} +\end{description} + +\begin{alertblock}{} +$>2~\sigma$ deviations from SM + +\end{alertblock} + +\end{columns} + +\end{minipage} +} + +\vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\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.\\ +$\color{JungleGreen}{\Rrightarrow}$ The $CP$ averaged angular observables are defined:\\ +\eq{ +S_i = \dfrac{J_i+ \bar{J}_i}{(d \Gamma + d \bar{\Gamma})/dq^2}\nonumber +} + +} + +\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} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +% symmetries +\begin{frame}{Symmetries in $\PB \to \PKstar \Pmu \Pmu$} +{~} +\begin{minipage}{\textwidth} +$\color{JungleGreen}{\Rrightarrow}$ We have 12 angular coefficients ($S_i$).\\ +$\color{JungleGreen}{\Rrightarrow}$ There exists 4 symmetry transformations that leave the angular distributions non changed: +\begin{tiny} +\eq{ +n_\|=\binom{A_\|^L}{A_\|^{R*}}\ ,\quad +n_\bot=\binom{A_\bot^L}{-A_\bot^{R*}}\ ,\quad +n_0=\binom{A_0^L}{A_0^{R*}}\ .\nonumber +} +\end{tiny} +\begin{tiny} +\eq{ + n_i^{'} = U n_i= + \left[ + \begin{array}{ll} + e^{i\phi_L} & 0 \\ + 0 & e^{-i \phi_R} + \end{array} + \right] + \left[ + \begin{array}{rr} + \cos \theta & -\sin \theta \\ + \sin \theta & \cos \theta + \end{array} + \right] + \left[ + \begin{array}{rr} + \cosh i \tilde{\theta} & -\sinh i \tilde{\theta} \\ + - \sinh i \tilde{\theta} & \cosh i \tilde{\theta} + \end{array} + \right] + n_i \,. + \label{symmassless}\nonumber} +\end{tiny} +$\color{JungleGreen}{\Rrightarrow}$ Using this symmetries one can show that there are 8 independent observables. The pdf can be wrote as: +\begin{tiny} +\begin{align*} +\left.\frac{1}{{\rm d}(\Gamma+\bar{\Gamma})/{\rm d}q^2}\frac{{\rm d}(\Gamma+\bar{\Gamma})}{{\rm dcos}\thetal\,{\rm dcos}\thetak\,{\rm d}\phi}\right|_{\rm P} = +\tfrac{9}{32\pi}\bigl[ +&\tfrac{3}{4} (1-{F_{\rm L}})\sin^2\thetak \label{eq:pdfpwave}\\[-0.75em] +&+ {F_{\rm L}}\cos^2\thetak + \tfrac{1}{4}(1-{F_{\rm L}})\sin^2\thetak\cos 2\thetal\nonumber\\ +&- {F_{\rm L}} \cos^2\thetak\cos 2\thetal + {S_3}\sin^2\thetak \sin^2\thetal \cos 2\phi\nonumber\\ +&+ {S_4} \sin 2\thetak \sin 2\thetal \cos\phi + {S_5}\sin 2\thetak \sin \thetal \cos \phi\nonumber\\ +&+ \tfrac{4}{3} {A_{\rm FB}} \sin^2\thetak \cos\thetal + {S_7} \sin 2\thetak \sin\thetal \sin\phi\nonumber\\ +&+ {S_8} \sin 2\thetak \sin 2\thetal \sin\phi + {S_9}\sin^2\thetak \sin^2\thetal \sin 2\phi \nonumber +\bigr]. +%\end{split} +%\bigr],\ +\end{align*} +\end{tiny} + +\end{minipage} +\vspace*{2.1cm} +\end{frame} + + + + + + + + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{LHCb update of the $\PBzero \to \PKstar \Pmuon \APmuon$, Selection} +{~} +\begin{minipage}{\textwidth} +\begin{columns} + +\column{0.5\textwidth} +\begin{itemize} +\item \href{https://lhcb.web.cern.ch/lhcb/Physics-Results/LHCb-CONF-2015-002.pdf}{{\color{blue}{LHCb-CONF-2015-002}}} +\item PID, kinematics and isolation variables used in a Boosted Decision Tree (BDT) to reject background. +\item Reject the regions of $\PJpsi$ and $\Ppsi(2S)$. +\item Specific vetos for backgrounds: $\PLambdab \to \Pproton \PK \Pmu \Pmu$, $\PBs \to \Pphi \Pmu \Pmu$, etc. +\item Using k-Fold technique and signal proxy $\PB \to \PJpsi \PKstar$ for training the BDT. +\item Improved selection allowed for finer binning than the $1\invfb$ analysis. +\end{itemize} + + +\column{0.5\textwidth} + +\includegraphics[width=0.88\textwidth]{images/Fig1.pdf} \\ +\includegraphics[width=0.88\textwidth]{images/fold.png} + +\end{columns} + + + +\end{minipage} +\vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{LHCb update of the $\PBzero \to \PKstar \Pmuon \APmuon$, Selection} +{~} +\begin{minipage}{\textwidth} + +\begin{itemize} +\item Signal modelled by a sum of two Crystal-Ball functions. +\item Shape is defined using $\PB \to \PJpsi \PKstar$ and corrected for $q^2$ dependency. +\item Combinatorial background modelled by exponent. +\end{itemize} + +\begin{columns} +\column{0.5\textwidth} +\begin{itemize} +\item $\PK \Ppi$ system: +\begin{itemize} +\item Rel. Breit Wigner for P-wave +\item Lass model for the S-wave. +\item Linear model for background. +\item Reduced the systematic compared to previous analysis. +\end{itemize} +\end{itemize} + +\column{0.5\textwidth} + +\includegraphics[width=0.88\textwidth]{images/pbkg} + +\end{columns} + +\begin{large} +\begin{itemize} +\item In total we found $2398\pm57$ candidates in the $(0.1,19)~\GeV^2$ $q^2$ region. +\item $624 \pm 30$ candidates in the theoretically the most interesting $(1.1-6.0)~\GeV^2$ region. +\end{itemize} +\end{large} + + + + +\end{minipage} +\vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Detector acceptance} +{~} +\begin{minipage}{\textwidth} +\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} c_{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 $\cos \thetal, \cos \thetak, \phi, q^2$. +\end{itemize} + + + + +\column{0.4\textwidth} +\includegraphics[width=0.99\textwidth]{images/det.png} +\end{columns} + + +\end{minipage} +\vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Control channel} +{~} +\begin{minipage}{\textwidth} + + +\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} + +\begin{columns} + +\column{0.5\textwidth} + +\includegraphics[width=0.95\textwidth]{images/mlogjpsi.png} +\column{0.5\textwidth} +\includegraphics[width=0.95\textwidth]{images/mkpijpsi.png} + +\end{columns} + + +\includegraphics[width=0.99\textwidth]{images/angles2.png} + + + +\end{minipage} +\vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{$\PBzero \rightarrow \PK^{\ast} \Pmu \Pmu$ results} + \begin{minipage}{\textwidth} +\begin{columns} +\column{2.5in} +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig5a.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig5c.pdf} +\column{2.5in} +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig5b.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig5d.pdf} +\end{columns} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{$\PBzero \rightarrow \PK^{\ast} \Pmu \Pmu$ results} + \begin{minipage}{\textwidth} +\begin{columns} +\column{2.5in} +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig5e.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig5f.pdf} +\column{2.5in} +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig5g.pdf}\\ +\includegraphics[angle=-90,width=0.95\textwidth]{images/Fig5h.pdf} +\end{columns} +\end{minipage} + \vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Results in $\PB \to \PKstar \Pmu \Pmu$} + \begin{minipage}{\textwidth} + \begin{center} + \includegraphics[angle=-90,width=0.65\textwidth]{images/Fig17.pdf}\\ + \end{center} + +\begin{itemize} +\item Tension with $3~\invfb$ gets confirmed! +\item The two bins deviate both in $2.8~\sigma$ from SM prediction. +\item Result compatible with previous result. +\end{itemize} + + +\end{minipage} + \vspace*{2.1cm} +\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 then 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[height=4cm]{images/bs2phipi.png} + \includegraphics[height=4cm]{images/BsSel.png} + \end{center} + +\begin{itemize} +\item Recent LHCb measurement, \href{https://cds.cern.ch/record/2029820/files/JHEP09-179.pdf}{{\color{blue}{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. +\item Angular part in agreement with SM ($S_5$ is not accessible). +\end{itemize} + + +\end{minipage} +\vspace*{2.1cm} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\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 \href{http://arxiv.org/abs/1503.07138}{{\color{blue}{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}{{\color{blue}{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 $0.0004 < q^2 <1~\GeV^2$, \href{http://arxiv.org/abs/1503.07138}{{\color{blue}{JHEP 04 (2015) 064}}}. + \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} +\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} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Theory implications} +{~} +\begin{minipage}{\textwidth} + +\begin{itemize} +\item A preliminary fit prepared by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, presented in \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}} +\item Took into the fit: +\begin{itemize} +\item $\mathcal{B} ( \PB \to X_s \Pphoton) = (3.36 \pm 0.23) \times 10^{-4} $, Misiak et. al. 2015. +\item $\mathcal{B} ( \PB \to\Pmu \Pmu)$, theory: Bobeth et al 2013, experiment: LHCb+CMS average (2015) +\item $\mathcal{B} ( \PB \to X_s \Pmu \Pmu$), Huber et al 2015 +\item $\mathcal{B} ( \PB \to \PK \Pmu \Pmu$),Bouchard et al 2013, 2015 +\item $\PB_{(s)} \to \PKstar(\Pphi) \Pmu \Pmu$, Horgan et al 2013 +\item $\PB \to \PK \Pe \Pe$, $\PB \to \PKstar \Pe \Pe$ and $R_k$. +\end{itemize} +%\item Overall there is $>4~\sigma$ discrepancy wrt. SM. +\end{itemize} + + + + + +\end{minipage} +\vspace*{2.1cm} +\end{frame} +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{Theory implications} +{~} +\begin{minipage}{\textwidth} + +\begin{itemize} +\item A preliminary fit prepared by \texttt{S. Descotes-Genon, L. Hofer, J. Matias, J. Virto}, presented in \href{http://arxiv.org/abs/1510.04239}{\color{blue}{arXiv::1510.04239}} +\item The data can be explained by modifying the $C_9$ Wilson coefficient. +\item Overall there is around $>4.~\sigma$ discrepancy wrt. SM. +\end{itemize} +\includegraphics[width=0.9\textwidth]{images/C9.png} + + + + +\end{minipage} +\vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{If not NP?} +{~} +\begin{minipage}{\textwidth} +\begin{itemize} +\item We are not there yet! +\item There might be something not taken into account in the theory. +\item Resonances ($\PJpsi$, $\Ppsi(2S)$) tails can mimic NP effects. +\item There might be some non factorizable QCD corrections.\\ +'' However, the central value of this effect would have to be significantly larger than expected on the basis of existing estimates'' \texttt{D.Straub}, \href{http://arxiv.org/abs/1503.06199}{ {\color{blue}{arXiv::1503.06199}}} +. +\end{itemize} +\only<1>{ +\includegraphics[width=0.9\textwidth]{images/charmloop.png} +} +\only<2>{ +\begin{center} +\includegraphics[width=0.6\textwidth]{images/charmloop2.png} +\end{center} +} + +\end{minipage} +\vspace*{2.1cm} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{There is more!} +{~} +\begin{minipage}{\textwidth} + +\begin{itemize} +\item There is one other LUV decay recently measured by LHCb. +\item $R(\PDstar)=\dfrac{\mathcal{B}(\PB \to \PDstar \Ptau \Pnu)}{\mathcal{B}(\PB \to \PDstar \Pmu \Pnu)}$ +\item Clean SM prediction: $R(\PDstar)=0.252(3)$, PRD 85 094025 (2012) +\item LHCb result: $R(\PDstar)= 0.336 \pm 0.027 \pm 0.030$, HFAG average: $R(\PDstar)=0.322 \pm 0.022$ +\item $3.9~\sigma$ discrepancy wrt. SM. +\end{itemize} + +\begin{center} + +\includegraphics[width=0.52\textwidth]{images/RDstar.png} + +\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}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + + + + +\begin{frame}{Theory implications} +{~} + \begin{minipage}{\textwidth} + +\includegraphics[height=0.9\textheight]{images/table.png} + + +\end{minipage} + \vspace*{2.1cm} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}{If not NP?} +{~} +\begin{minipage}{\textwidth} +\begin{itemize} +\item How about our clean $P_i$ observables? +\item The QCD cancel as mentioned only at leading order. +\item Comparison to normal observables with the optimised ones. +\end{itemize} +\includegraphics[width=0.9\textwidth]{images/C9_S_P.png} + + +\end{minipage} +\vspace*{2.1cm} +\end{frame} + +\end{document} diff --git a/PTF2016/mchrzasz.toc b/PTF2016/mchrzasz.toc new file mode 100644 index 0000000..429917f --- /dev/null +++ b/PTF2016/mchrzasz.toc @@ -0,0 +1,5 @@ +\boolfalse {citerequest}\boolfalse {citetracker}\boolfalse {pagetracker}\boolfalse {backtracker}\relax +\defcounter {refsection}{0}\relax +\beamer@endinputifotherversion {3.24pt} +\defcounter {refsection}{0}\relax +\select@language {english} diff --git a/PTF2016/mchrzasz2.pdf b/PTF2016/mchrzasz2.pdf new file mode 100644 index 0000000..39bd888 --- /dev/null +++ b/PTF2016/mchrzasz2.pdf Binary files differ diff --git a/PTF2016/mchrzasz_v2.pdf b/PTF2016/mchrzasz_v2.pdf new file mode 100644 index 0000000..ea5f4da --- /dev/null +++ b/PTF2016/mchrzasz_v2.pdf Binary files differ diff --git a/PTF2016/tikzfeynman.sty b/PTF2016/tikzfeynman.sty new file mode 100755 index 0000000..521fc65 --- /dev/null +++ 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(textpos) Environment textblock* should not have any text (textpos) or printable material appearing before it. -(textpos) Alignment may work out wrongly. on input line 872. +(textpos) Alignment may work out wrongly. on input line 823. -Overfull \vbox (46.7159pt too high) detected at line 872 +Overfull \vbox (55.47925pt too high) detected at line 823 [] File: images/BG_lower.png Graphic file (type QTm) @@ -3248,23 +3262,26 @@ [19 ] -File: images/compare_AFBPad.pdf Graphic file (type QTm) - -File: images/compare_S7Pad.pdf Graphic file (type QTm) - -File: images/compare_S8Pad.pdf Graphic file (type QTm) +LaTeX Font Info: Try loading font information for EU1+lmtt on input line 864 +. + (/usr/share/texlive/texmf-dist/tex/latex/euenc/eu1lmtt.fd +File: eu1lmtt.fd 2009/10/30 v1.6 Font defs for Latin Modern +) +File: images/wilsonchi2.pdf Graphic file (type QTm) - -File: images/compare_S9Pad.pdf Graphic file (type QTm) - + +Overfull \hbox (4.38206pt too wide) detected at line 864 +[][][] $[]$[][][][][][][][] $[]$[][][][][][][][] $[]$[][][][][][] + [] + Package textpos Warning: environment textblock* not in vertical mode. (textpos) Environment textblock* should not have any text (textpos) or printable material appearing before it. -(textpos) Alignment may work out wrongly. on input line 872. +(textpos) Alignment may work out wrongly. on input line 864. -Overfull \vbox (46.7159pt too high) detected at line 872 +Overfull \vbox (32.68571pt too high) detected at line 864 [] File: images/BG_lower.png Graphic file (type QTm) @@ -3288,16 +3305,14 @@ [20 ] -File: images/S6cPad.pdf Graphic file (type QTm) - +File: images/ksmumu_BF.png Graphic file (type QTm) + +File: images/kmumu_BF.png Graphic file (type QTm) + +File: images/bukst_BF.png Graphic file (type QTm) -Package textpos Warning: environment textblock* not in vertical mode. -(textpos) Environment textblock* should not have any text -(textpos) or printable material appearing before it. -(textpos) Alignment may work out wrongly. on input line 872. - - -Overfull \vbox (55.47925pt too high) detected at line 872 + +Overfull \vbox (66.24098pt too high) detected at line 898 [] File: images/BG_lower.png Graphic file (type QTm) @@ -3321,26 +3336,16 @@ [21 ] -LaTeX Font Info: Try loading font information for EU1+lmtt on input line 913 -. - (/usr/share/texlive/texmf-dist/tex/latex/euenc/eu1lmtt.fd -File: eu1lmtt.fd 2009/10/30 v1.6 Font defs for Latin Modern -) -File: images/wilsonchi2.pdf Graphic file (type QTm) - - -Overfull \hbox (4.38206pt too wide) detected at line 913 -[][][] $[]$[][][][][][][][] $[]$[][][][][][][][] $[]$[][][][][][] - [] - +File: images/bs2phipi.png Graphic file (type QTm) + Package textpos Warning: environment textblock* not in vertical mode. 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(textpos) Environment textblock* should not have any text (textpos) or printable material appearing before it. -(textpos) Alignment may work out wrongly. on input line 968. +(textpos) Alignment may work out wrongly. on input line 953. -Overfull \vbox (45.42638pt too high) detected at line 968 +Overfull \vbox (22.65746pt too high) detected at line 953 [] File: images/BG_lower.png Graphic file (type QTm) @@ -3428,16 +3441,16 @@ [24 ] -File: images/Lb_BR.png Graphic file (type QTm) - +File: images/AFB_Lb.png Graphic file (type QTm) + Package textpos Warning: environment textblock* not in vertical mode. 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-Overfull \vbox (68.56355pt too high) detected at line 1270 +File: images/vub.png Graphic file (type QTm) + +Overfull \vbox (61.49702pt too high) detected at line 1268 [] File: images/BG_lower.png Graphic file (type QTm) @@ -3803,9 +3808,9 @@ [37 ] -File: images/hfagccs.png Graphic file (type QTm) - -Overfull \vbox (34.30829pt too high) detected at line 1290 +File: images/vub2.png Graphic file (type QTm) + +Overfull \vbox (39.40065pt too high) detected at line 1294 [] File: images/BG_lower.png Graphic file (type QTm) @@ -3829,9 +3834,9 @@ [38 ] -File: images/vub.png Graphic file (type QTm) - -Overfull \vbox (61.49702pt too high) detected at line 1315 +File: images/charmCP.png Graphic file (type QTm) + +Overfull \vbox (60.04861pt too high) detected at line 1319 [] File: images/BG_lower.png Graphic file (type QTm) @@ -3855,13 +3860,8 @@ [39 ] -File: images/vub2.png Graphic file (type QTm) - -Overfull \vbox (39.40065pt too high) detected at line 1341 - [] - File: images/BG_lower.png Graphic file (type QTm) - + Overfull \vbox (19.18185pt too high) has occurred while \output is active [] ................................................. @@ -3881,9 +3881,9 @@ [40 ] -File: images/charmCP.png Graphic file (type QTm) - -Overfull \vbox (60.04861pt too high) detected at line 1366 +File: images/CKMfit.png Graphic file (type QTm) + +Overfull \vbox (16.4327pt too high) detected at line 1357 [] File: images/BG_lower.png Graphic file (type QTm) @@ -3928,9 +3928,9 @@ [42 ] -File: images/CKMfit.png Graphic file (type QTm) - -Overfull \vbox (16.4327pt too high) detected at line 1404 +File: images/gelman.png Graphic file (type QTm) + +Overfull \vbox (26.3181pt too high) detected at line 1385 [] File: images/BG_lower.png Graphic file (type QTm) @@ -3954,8 +3954,18 @@ [43 ] +File: images/Z4430.png Graphic file (type QTm) + +Overfull \hbox (4.38205pt too wide) detected at line 1436 +[][][] $[]$[][][][][][][][] $[]$[][][][][][][][] $[]$[][][][][][] + [] + + +Overfull \vbox (1.70079pt too high) detected at line 1436 + [] + File: images/BG_lower.png Graphic file (type QTm) - + Overfull \vbox (19.18185pt too high) has occurred while \output is active [] ................................................. @@ -3975,9 +3985,9 @@ [44 ] -File: images/gelman.png Graphic file (type QTm) - -Overfull \vbox (26.3181pt too high) detected at line 1432 +File: images/Z44301.png Graphic file (type QTm) + +Overfull \vbox (56.78085pt too high) detected at line 1454 [] File: images/BG_lower.png Graphic file (type QTm) @@ -4001,14 +4011,9 @@ [45 ] -File: images/x3872.png Graphic file (type QTm) - -Overfull \hbox (4.38205pt too wide) detected at line 1459 -[][][] $[]$[][][][][][][][] $[]$[][][][][][][][] $[]$[][][][][][] - [] - - -Overfull \vbox (33.61595pt too high) detected at line 1459 +File: images/penta.png Graphic file (type QTm) + +Overfull \vbox (57.78618pt too high) detected at line 1476 [] File: images/BG_lower.png Graphic file (type QTm) @@ -4032,14 +4037,9 @@ [46 ] -File: images/Z4430.png Graphic file (type QTm) - -Overfull \hbox (4.38205pt too wide) detected at line 1483 -[][][] $[]$[][][][][][][][] $[]$[][][][][][][][] $[]$[][][][][][] - [] - - -Overfull \vbox (1.70079pt too high) detected at line 1483 +File: images/penta2.png Graphic file (type QTm) + +Overfull \vbox (21.59618pt too high) detected at line 1498 [] File: images/BG_lower.png Graphic file (type QTm) @@ -4063,9 +4063,9 @@ [47 ] -File: images/Z44301.png Graphic file (type QTm) - -Overfull \vbox (56.78085pt too high) detected at line 1501 +File: images/penta3.png Graphic file (type QTm) + +Overfull \vbox (50.16116pt too high) detected at line 1537 [] File: images/BG_lower.png Graphic file (type QTm) @@ -4089,84 +4089,6 @@ [48 ] -File: images/penta.png Graphic file (type QTm) - -Overfull \vbox (57.78618pt too high) detected at line 1523 - [] - -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" -. -. Font Trebuchet MS does not contain any OpenType `Script' information. -................................................. -................................................. -. fontspec info: "defining-font" -. -. Font family 'TrebuchetMS(0)' created for font 'Trebuchet MS' with options -. [Mapping=tex-text,]. -. -. This font family consists of the following shapes: -................................................. - -[49 - -] -File: images/penta2.png Graphic file (type QTm) - -Overfull \vbox (21.59618pt too high) detected at line 1545 - [] - -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" -. -. Font Trebuchet MS does not contain any OpenType `Script' information. -................................................. -................................................. -. fontspec info: "defining-font" -. -. Font family 'TrebuchetMS(0)' created for font 'Trebuchet MS' with options -. [Mapping=tex-text,]. -. -. This font family consists of the following shapes: -................................................. - -[50 - -] -File: images/penta3.png Graphic file (type QTm) - -Overfull \vbox (50.16116pt too high) detected at line 1584 - [] - -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" -. -. Font Trebuchet MS does not contain any OpenType `Script' information. -................................................. -................................................. -. fontspec info: "defining-font" -. -. Font family 'TrebuchetMS(0)' created for font 'Trebuchet MS' with options -. [Mapping=tex-text,]. -. -. This font family consists of the following shapes: -................................................. - -[51 - -] File: images/BG_lower.png Graphic file (type QTm) Overfull \vbox (19.18185pt too high) has occurred while \output is active [] @@ -4185,7 +4107,7 @@ . This font family consists of the following shapes: ................................................. -[52 +[49 ] File: images/Joke.jpg Graphic file (type QTm) @@ -4208,7 +4130,7 @@ . This font family consists of the following shapes: ................................................. -[53 +[50 ] \c@framenumberappendix=\count442 @@ -4230,12 +4152,91 @@ . 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This font family consists of the following shapes: +................................................. + +[52 + +] +File: images/C9_S_P.png Graphic file (type QTm) + +Overfull \vbox (19.02252pt too high) detected at line 1627 + [] + +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" +. +. Font Trebuchet MS does not contain any OpenType `Script' information. +................................................. +................................................. +. fontspec info: "defining-font" +. +. Font family 'TrebuchetMS(0)' created for font 'Trebuchet MS' with options +. [Mapping=tex-text,]. +. +. This font family consists of the following shapes: +................................................. + +[53 + +] +Overfull \hbox (14.91016pt too wide) in alignment at lines 1670--1670 + [][][] [] + [] + + +Overfull \vbox (61.75616pt too high) detected at line 1670 + [] + +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" +. +. Font Trebuchet MS does not contain any OpenType `Script' information. +................................................. +................................................. +. fontspec info: "defining-font" +. +. Font family 'TrebuchetMS(0)' created for font 'Trebuchet MS' with options +. [Mapping=tex-text,]. +. +. 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leptons exists in 6 ''flavors'' (u,c,t,d,s,b) and (e,$\mu$, $\tau$, $\nu_e$, $\nu_{\mu}$, $\nu_{\tau}$).\\ +\ARROW WHAT: Quarks and leptons exists in 6 ''flavours'' (u,c,t,d,s,b) and (e,$\mu$, $\tau$, $\nu_e$, $\nu_{\mu}$, $\nu_{\tau}$).\\ \ARROW WHY: \begin{itemize} \item Flavour is the heart of SM. It involves $22$ from $28$ free parameters, like masses mixing and CP violation. -\item Flavor physics loop processes (box and penguins) are sensitive to energy scales well beyond the ones of the accelerators, thanks to virtual contributions. +\item Flavour physics loop processes (box and penguins) are sensitive to energy scales well beyond the ones of the accelerators, thanks to virtual contributions. \end{itemize} \begin{center} \includegraphics[width=0.8\textwidth]{images/mglass.png} @@ -340,7 +340,7 @@ \vspace*{2.cm} \end{frame} -\begin{frame}{Introduction to flavor physics} +\begin{frame}{Introduction to flavour physics} \begin{minipage}{\textwidth} \begin{footnotesize} @@ -375,7 +375,7 @@ \mathcal{L}_{CC}=-\frac{g}{\sqrt{2}} \bar{u} \gamma^{\mu}(1-\gamma^5)V_{CKM}d+... \end{align*} \column{2in} -\includegraphics[width=0.85\textwidth]{images/in_thi9.png} +\includegraphics[width=0.95\textwidth]{images/in_thi9.png} \end{columns} @@ -397,9 +397,9 @@ \begin{align*} V_{CKM}= \begin{pmatrix} -1-\lambda^2/2 & \lambda & A\lambda^3(\rho- i \eta)\\ +1-\lambda^2/2 & \lambda & A\lambda^3({\color{red}\rho- i \eta})\\ -\lambda & 1-\lambda^2/2 & A \lambda^2 \\ -A \lambda^3 (1-\rho - i \eta) & -A \lambda^2 & 1 +A \lambda^3 ({\color{red}1-\rho - i \eta}) & -A \lambda^2 & 1 \end{pmatrix} \end{align*} \ARROW Strong hierarchy: @@ -501,11 +501,11 @@ \item $(g-2)_{\mu}$ \item CP violation: \begin{itemize} -\item $\gamma$ angle. -\item CP violation in $\PBd $ and $\PBs$. -\item CP violation in charm. -\item CP violation in kaons. -\item $V_{ub}$. +\item $\gamma$ angle +\item CP violation in $\PBd $ and $\PBs$ +\item CP violation in charm +\item CP violation in kaons +\item $V_{ub}$ \end{itemize} \item Tetra\&Pentaquarks \end{itemize} @@ -517,22 +517,6 @@ \end{frame} - - - -\begin{frame}{Heavy flavor experiments} - \begin{minipage}{\textwidth} -\begin{footnotesize} -{~}\\{~}\\ - - - - -\end{footnotesize} -\end{minipage} - \vspace*{2.cm} -\end{frame} - \begin{frame} \begin{center} \begin{Huge} @@ -562,7 +546,7 @@ \item[i=1,2] Tree \item[i=3-6,8] Gluon penguin \item[i=7] Photon penguin - \item[i=9.10] EW penguin + \item[i=9,10] EW penguin \item[i=S] Scalar penguin \item[i=P] Pseudoscalar penguin \end{description} @@ -586,7 +570,7 @@ %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% -\begin{frame}\frametitle{$\PBzero \rightarrow \Pmu^+ \Pmu^-$} +\begin{frame}\frametitle{$\PB_{d,s} \rightarrow \Pmu^+ \Pmu^-$} \begin{columns} \column{3.2in} @@ -599,6 +583,7 @@ \item Sensitive to contributions from scalar and pesudoscalar couplings. \item Probing: MSSM, higgs sector, etc. \item In MSSM: $\mathcal{B}(\PBs \to \Pmuon \APmuon) \sim \tan^6 \beta /m_A^4$ +\item Theory errors dominated by the form factors! Will go down in the future. \end{itemize} \column{1.5in} @@ -610,36 +595,6 @@ \end{frame} -%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% -\begin{frame}\frametitle{$\PBzero \rightarrow \Pmu^+ \Pmu^-$ searches} - - -\begin{columns} -\column{5in} - -\begin{itemize} -\item Background rejection power is a key feature of rare decays $\rightarrow$ use multivariate classifiers (BDT) and strong PID. -\end{itemize} -\column{0.1in}{~} - -\end{columns} -\begin{columns} -\column{2.5in} -\includegraphics[width=0.95\textwidth]{hql/BDT.png} - -\column{2.5in} - -\includegraphics[width=0.95\textwidth]{hql/mass.png} - -\end{columns} - -\begin{itemize} -\item Normalize the BF to $\PBplus \to \PJpsi(\mu\mu) \PKplus$ and $\PBzero \to \PK \Ppi$. -\end{itemize} -\textref{ PRL 111 (2013) 101805} - -\end{frame} - %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}\frametitle{$\PBzero \rightarrow \Pmu^+ \Pmu^-$ Results} @@ -752,11 +707,6 @@ \begin{align*} P_5^{\prime}=\frac{S_5}{F_L(1-F_L)} \end{align*} -\ARROW Analysis performed with 3 methods:\begin{itemize} -\item Likelihood fit. -\item Method of moments. -\item Amplitudes fit. -\end{itemize} \end{minipage} @@ -801,7 +751,7 @@ \begin{itemize} \item Tension with $3~\invfb$ gets confirmed! -\item two bins both deviate by $2.8~\sigma$ from SM prediction. +\item Two bins both deviate by $2.8~\sigma$ from SM prediction. \item Result compatible with previous results and Belle! \item SM: \href{http://arxiv.org/abs/1407.8526}{\color{blue}JHEP12(2014)125} \end{itemize} @@ -851,7 +801,8 @@ \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} +\includegraphics[angle=-90,width=0.49\textwidth]{images/compare_S9Pad.pdf}\\ +\ARROW $S_7$, $S_8$, $S_9$ are zero in the SM! } \only<3>{ \includegraphics[angle=-90,width=0.75\textwidth]{images/S6cPad.pdf}\\ @@ -978,8 +929,8 @@ \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} + \includegraphics[width=0.55\textwidth]{images/Lblow.png} +\includegraphics[width=0.55\textwidth]{images/Lbhigh.png} } @@ -1054,8 +1005,8 @@ \column{3.0in} \begin{itemize} \item Does the NP couple equally to all flavours? -\includegraphics[width=0.9\textwidth]{images/uni2.png} -\item Challenging analysis due to bremsstrahlung. +\includegraphics[width=0.99\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. @@ -1087,15 +1038,17 @@ \item There is one other LUV decay recently measured by LHCb. \item $R(\PDstar)=\dfrac{\mathcal{B}(\PB \to \PDstar \Ptau \Pnu)}{\mathcal{B}(\PB \to \PDstar \Pmu \Pnu)}$ \item Clean SM prediction: $R(\PDstar)=0.252(3)$, PRD 85 094025 (2012) -\item LHCb result: $R(\PDstar)= 0.336 \pm 0.027 \pm 0.030$, HFAG average: $R(\PDstar)=0.322 \pm 0.022$ +\item LHCb result: $R(\PDstar)= 0.336 \pm 0.027 \pm 0.030$ +\item HFAG average: $R(\PDstar)=0.322 \pm 0.022$ \item $4.0~\sigma$ discrepancy wrt. SM. \end{itemize} \begin{center} -\includegraphics[width=0.52\textwidth]{images/RDstar.png} +\includegraphics[width=0.48\textwidth]{images/RDstar.png} \end{center} +%\textref{http://www.slac.stanford.edu/xorg/hfag/index.html} \end{minipage} \vspace*{2.1cm} \end{frame} @@ -1112,7 +1065,7 @@ \includegraphics[width=0.75\textwidth]{images/quim2.png} \end{center} \ARROW The fit prefer a modification of $C_9$ Wilson coefficient with a value of $C_9^{NP}=-1$, with a significance over $4\sigma$.\\ -\ARROW Many theories link might accommodate the observed deviations. +%\ARROW Many theories link might accommodate the observed deviations. \textref{arXiv:1510.04239} \end{minipage} @@ -1169,7 +1122,7 @@ \ARROW Experiment: $a_{\mu}^{\rm E821}=(116 592 091 \pm 63) \times 10^{-11}$ [PDG 2014]\\ \ARROW Difference: $a_{\mu}^{\rm E821} -a_{\mu}^{\rm SM} =(288 \pm 80)\times 10^{-11}$ $\Leftrightarrow$ $3.6~\sigma$!\\ \ARROW Underestimated uncertainties? SUSY? NP?\\ -\ARROW Fermilabs E989 should futher reduce the experimental error to $\pm16 \times 10^{-11}$. +\ARROW Fermilabs E989 should futher reduce the experimental error\\ to $\pm16 \times 10^{-11}$. \end{minipage} \vspace*{2.1cm} @@ -1197,12 +1150,12 @@ \includegraphics[width=0.9\textwidth]{images/gamma.png} \column{2.8in} -\ARROW The LHCb combinations leads to: $\gamma = 70.9^{+7.1}_{-8.5}$.\\ -\ARROW Improved by $2^{\deg}$ compared to our previous result!\\ +\ARROW The LHCb combinations leads to: $\gamma = {70.9^{+7.1}_{-8.5} }^{\circ} $.\\ +\ARROW Improved by $2^{\circ}$ compared to our previous result!\\ \ARROW Other B-factories have 2 times larger errors: \begin{itemize} -\item BaBar: $\gamma=(70\pm 18)^{\deg}$ -\item Belle: $\gamma=(73^{+18}_{-15})^{\deg}$ +\item BaBar: $\gamma=(70\pm 18)^{\circ}$ +\item Belle: $\gamma=(73^{+18}_{-15})^{\circ}$ \end{itemize} @@ -1227,8 +1180,8 @@ \begin{center} \includegraphics[width=0.85\textwidth]{images/phis.png} \end{center} -\ARROW In the Sm $\phi_s \approx -2 \beta+s = -(0.0376^{+0.0007}_{-0.0008})~\rm rad$, where $\beta_s=\arg \left(- \frac{V_{ts}V_{tb}^{\ast}}{V_{cs} V_{cb}^{\ast}} \right)$\\ -\ARROW At the leading order the same phase is expected $\PBs \to \PDs \PDs$ and $\PB \to \PJpsi \Ppi \Ppi$.\\ +\ARROW In the SM $\phi_s \approx -2 \beta_s = -(0.0376^{+0.0007}_{-0.0008})~\rm rad$, where $\beta_s=\arg \left(- \frac{V_{ts}V_{tb}^{\ast}}{V_{cs} V_{cb}^{\ast}} \right)$\\ +\ARROW At the leading order same phase is expected $\PBs \to \PDs \PDs$ and $\PB \to \PJpsi \Ppi \Ppi$.\\ \ARROW NP can enter in the $\PBs$ mixing!\\ \ARROW Measured by simultaneous fit to $\PBs$ and $\bar{\PBs}$ decay rates: \begin{center} @@ -1306,7 +1259,7 @@ \begin{center} \includegraphics[width=0.45\textwidth]{images/vub.png} \end{center} -where $R_{FF}$ is a ratio of form factors, that can be calculated using lattice QCD [rxiv:1503.01421]. +where $R_{FF}$ is a ratio of form factors, that can be calculated using lattice QCD [arxiv:1503.01421]. \end{footnotesize} \textref{Nature Physics 11, 743-747 (2015)} @@ -1371,7 +1324,7 @@ {~} \begin{small} \ARROW 1999: Discovery of CP violation in $\PK \to \pi \pi$ (NA48, KTeV).\\ -\ARROW 2001: Combined experimental average of the two above experiments: $\Re (\epsilon^{\prime}/ \epsilon )=(16.6\pm 2.3)~\%$, compatible with SM. Experimental precision much better than the theoretical prediction.\\ +\ARROW 2001: Combined experimental average of the two above experiments: $\Re (\epsilon^{\prime}/ \epsilon )=(16.6\pm 2.3)\times 10^{-4}$, compatible with SM. Experimental precision much better than the theoretical prediction.\\ \ARROW 2015: Fantastic progresses in lattice QCD. Can now compute all relevant long-distance effects that used to dominate the theoretical uncertainty: \begin{align*} @@ -1433,7 +1386,7 @@ - +\iffalse \begin{frame}{X(3872)} {~} \begin{footnotesize} @@ -1457,7 +1410,7 @@ \vspace*{2.1cm} \end{frame} - +\fi \begin{frame}{$Z(4430)^-$} @@ -1594,7 +1547,7 @@ \ARROW Anomalies in the electroweak penguin and lepton universality combine to over $4\sigma$ significance discrepancy for NP.\\ \ARROW The dominant anomaly was recently confirmed by Belle experiment.\\ \ARROW $\gamma$ angle combination from LHCb is now two times more precise then the B-factories.\\ -\ARROW After $50$ years after the first prof. Gelman paper the pentraquark states have been observed.\\ +\ARROW After $50$ years after the first Prof. Gelman paper the pentraquark states have been observed.\\ \ARROW Stay tuned as there are plenty of more results in the pipe line! @@ -2048,6 +2001,39 @@ \vspace*{2.1cm} \end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PBzero \rightarrow \Pmu^+ \Pmu^-$ searches} + + +\begin{columns} +\column{5in} + +\begin{itemize} +\item Background rejection power is a key feature of rare decays $\rightarrow$ use multivariate classifiers (BDT) and strong PID. +\end{itemize} +\column{0.1in}{~} + +\end{columns} +\begin{columns} +\column{2.5in} +\includegraphics[width=0.95\textwidth]{hql/BDT.png} + +\column{2.5in} + +\includegraphics[width=0.95\textwidth]{hql/mass.png} + +\end{columns} + +\begin{itemize} +\item Normalize the BF to $\PBplus \to \PJpsi(\mu\mu) \PKplus$ and $\PBzero \to \PK \Ppi$. +\end{itemize} +\textref{ PRL 111 (2013) 101805} + +\end{frame} + %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % Lepton non universality %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%