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$\PKstar \to \PK^+ \Ppi^-$ helps in vertex reconstruction. \item High $\mathcal{B}(\chi \to \Pmuon \APmuon)$. \end{itemize} @@ -434,7 +435,7 @@ %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}\frametitle{$\PB \to \PKstar \chi(\mu\mu)$ motivation} -Possible models: +Discussed models: \begin{enumerate} \item \textbf{Inflaton:} \href{http://arxiv.org/abs/1403.4638}{{\color{blue}{Phys.Lett. B736 (2014) 494}}} \begin{itemize} @@ -479,12 +480,12 @@ \end{itemize} \column{2.5in} -\textbf{Long lifetime} ($\leq0.2~{\rm{ps}}$) +\textbf{Short lifetime} ($\leq0.2~{\rm{ps}}$) \begin{itemize} \item Dark matter mediator \href{http://arxiv.org/abs/1310.6752}{{\color{blue}{ Phys. Lett. B727 }}} \item Axion \href{http://arxiv.org/abs/0911.5355}{{\color{blue}{Phys.Rev.D81}}} \item Prompt decay. -\item Contaminated via Sm decay. +\item Contaminated via SM decay. \end{itemize} \end{columns} @@ -507,7 +508,7 @@ \begin{frame}\frametitle{Selection} \begin{itemize} \item Trigger on muons. -\item Multivariate selection: ${\rm{\mu BDT}}$ \href{JINST 8(2013)}{http://arxiv.org/abs/1305.7248} +\item Multivariate selection: ${\rm{\mu BDT}}$ \href{http://arxiv.org/abs/1305.7248}{JINST 8(2013)} \begin{itemize} \item ${\rm{\mu BDT}}$ ensures flat efficiency in lifetime of $\chi$. \end{itemize} @@ -543,10 +544,9 @@ \item Scan $m_{{\rm test}}$ in steps of $0.5~\sigma_m$. \begin{itemize} \item {\color{orange}{Wide resonances}} can't affect the search. -\item {\color{green}{Narrows resonances}} one we veto. +\item {\color{turtlegreen}{Narrows resonances}} we veto. \end{itemize} \item Calculations performed in each $m_{test}$ window. -\item A global p-value is assigned form minimum local p-value observed. \end{itemize} \column{1.6in} \includegraphics[width=0.9\textwidth]{susy/williams.png} @@ -565,7 +565,7 @@ $\Rrightarrow$ Largest deviation seen in $m_{\chi}=253~\MeV$.\\ $\rightarrowtail$ Not statistically significant: local p-value $=0.2$.\\ -$\Rrightarrow$ LHCb-PAPER-2015-036 in preparation. +$\Rrightarrow$ \href{http://arxiv.org/abs/1508.04094}{\color{blue}{LHCb-PAPER-2015-036}} submited to PRL. \end{frame} @@ -588,14 +588,14 @@ -$\Rrightarrow$ Interpretation of the results in to specific models:\\{~}\\ +$\Rrightarrow$ Interpretation of the results in two specific models:\\{~}\\ \includegraphics[width=1.05\textwidth]{susy/benchmarks.png} \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 -\begin{frame}\frametitle{Long living charged particles} +\begin{frame}\frametitle{Long living charged particles like $\PStau$} $\Rrightarrow$ Long living particles can also be produced in the PV. \\ \begin{itemize} @@ -604,8 +604,6 @@ $\Rrightarrow$ LHCb performed a search for long living $\PStau$ particles.\\ $\Rrightarrow$ $\PStau^+ \PStau^-$ produced by Drell-Yan process. \\ - - \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 @@ -615,7 +613,7 @@ \includegraphics[width=1.05\textwidth]{susy/stau.png} -$\Rrightarrow$ After the preselection an Neural Network is trained based on Cherenkov detectors to calculate to further suppress the remaining background. +$\Rrightarrow$ After the preselection an Neural Net is trained based on Cherenkov detectors to calculate to further suppress the remaining background. \end{frame} @@ -623,22 +621,84 @@ \begin{frame}\frametitle{$\PStau$ results} \begin{itemize} \item No significant signal yield has been observed. -\item Upper limit has been set. +\item $95~\%$ upper limit has been set. \end{itemize} \includegraphics[width=0.8\textwidth]{susy/sps7.png} \end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Hidden valley searches} +\begin{itemize} +\item A possible extensions of the SM are models where the new particles have a small couplings to the SM particles. +\item Such models are: +\begin{itemize} +\item Lightest SUSY +\item B/LNV +\item Gravity mediated SUSY +\item Hidden Valleys +\end{itemize} +\item LHCb have performed a search for $\pi_{\nu}$ particles that are pair produced from Higgs like SM particle. +\item They have a long lifetime and decay to pair of jets. +\end{itemize} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Analysis strategy} +\begin{itemize} +\item Efficient trigger for long living particles. +\item Reconstruction of two jets. +\item MVA used for vertex search. +%\item Remove interactions with material. + +\item Search performed in different regions of displaced vertexes ($R_{xy}$). +\begin{itemize} +\item $0.4< R_{xy}<4\rm ~mm$, removes heavy flavour and material interaction backgrounds. +\end{itemize} +\end{itemize} +\begin{columns} + + + +\column{0.5\textwidth} +\includegraphics[angle=-90,width=1.\textwidth]{images/Fig1a.pdf} + +\column{0.5\textwidth} +\includegraphics[angle=-90,width=1.\textwidth]{images/Fig1b.pdf} + +\end{columns} + + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Di-jet distribution} + +\includegraphics[width=0.8\textwidth]{dijet.png} + +\begin{itemize} +\item {\color{turtlegreen}{Signal component fit result}}, {\color{cyan}{Background component}} +\end{itemize} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Results} +\includegraphics[width=0.85\textwidth]{images/Fig4.pdf} + + +\end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 \begin{frame}\frametitle{Conclusion} \begin{itemize} \item A search for a dark boson in the decay channel\\ $\PBzero \to \PKstar \Pmuon \APmuon$ has been presented. \begin{itemize} -\item No deviations form SM observed. +\item No deviations from SM observed. \end{itemize} \item Results are the most constraining exclusion limit on the process. -\item LHCb is suited for search for long living particles. +\item LHCb is suited for search for long lived particles. \item Stay tuned, more searches like this are on they way. \end{itemize} diff --git a/SUSY_2015/LongLive_light/BKG.png b/SUSY_2015/LongLive_light/BKG.png new file mode 100644 index 0000000..8434cf0 --- /dev/null +++ b/SUSY_2015/LongLive_light/BKG.png Binary files differ diff --git a/SUSY_2015/LongLive_light/CKM_logo.jpg b/SUSY_2015/LongLive_light/CKM_logo.jpg new file mode 100644 index 0000000..86f351a --- /dev/null +++ b/SUSY_2015/LongLive_light/CKM_logo.jpg Binary files differ diff --git a/SUSY_2015/LongLive_light/CLS2.png b/SUSY_2015/LongLive_light/CLS2.png new file mode 100644 index 0000000..fb2d789 --- /dev/null +++ b/SUSY_2015/LongLive_light/CLS2.png Binary files differ diff --git a/SUSY_2015/LongLive_light/ClsB.png b/SUSY_2015/LongLive_light/ClsB.png new file mode 100644 index 0000000..f5db462 --- /dev/null +++ b/SUSY_2015/LongLive_light/ClsB.png Binary files differ diff --git a/SUSY_2015/LongLive_light/Double_beta_decay_feynman.png 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mchrzasz.tex +# xelatex mchrzasz.tex +clean: + rm *.aux *.bbl *.blg *.log *.out mchrzasz.pdf *.sh *.xml *.snm *.toc *.nav diff --git a/SUSY_2015/LongLive_light/Makefile~ b/SUSY_2015/LongLive_light/Makefile~ new file mode 100644 index 0000000..e4cf8e8 --- /dev/null +++ b/SUSY_2015/LongLive_light/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/SUSY_2015/LongLive_light/OS_banan_un.png b/SUSY_2015/LongLive_light/OS_banan_un.png new file mode 100644 index 0000000..e2c078c --- /dev/null +++ b/SUSY_2015/LongLive_light/OS_banan_un.png Binary files differ diff --git a/SUSY_2015/LongLive_light/SS_banan_un.png b/SUSY_2015/LongLive_light/SS_banan_un.png new file mode 100644 index 0000000..d606523 --- /dev/null +++ b/SUSY_2015/LongLive_light/SS_banan_un.png Binary files differ diff --git a/SUSY_2015/LongLive_light/babar.jpg b/SUSY_2015/LongLive_light/babar.jpg new file mode 100644 index 0000000..5a6a665 --- /dev/null +++ b/SUSY_2015/LongLive_light/babar.jpg Binary files differ diff --git a/SUSY_2015/LongLive_light/bananas.png b/SUSY_2015/LongLive_light/bananas.png new file mode 100644 index 0000000..76fe1ae --- /dev/null +++ b/SUSY_2015/LongLive_light/bananas.png Binary files differ diff --git a/SUSY_2015/LongLive_light/beamercolorthemeFlip.sty b/SUSY_2015/LongLive_light/beamercolorthemeFlip.sty new file mode 100755 index 0000000..d6b9c50 --- /dev/null +++ b/SUSY_2015/LongLive_light/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/SUSY_2015/LongLive_light/beamerinnerthemeFlip.sty b/SUSY_2015/LongLive_light/beamerinnerthemeFlip.sty new file mode 100755 index 0000000..9910f4d --- /dev/null +++ b/SUSY_2015/LongLive_light/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/SUSY_2015/LongLive_light/beamerouterthemeFlip.sty b/SUSY_2015/LongLive_light/beamerouterthemeFlip.sty new file mode 100755 index 0000000..d12f6d6 --- /dev/null +++ b/SUSY_2015/LongLive_light/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/SUSY_2015/LongLive_light/beamerouterthemedecolines.sty b/SUSY_2015/LongLive_light/beamerouterthemedecolines.sty new file mode 100755 index 0000000..669e493 --- /dev/null +++ b/SUSY_2015/LongLive_light/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/SUSY_2015/LongLive_light/beamerthemeFlip.sty b/SUSY_2015/LongLive_light/beamerthemeFlip.sty new file mode 100755 index 0000000..a615ff5 --- /dev/null +++ b/SUSY_2015/LongLive_light/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/SUSY_2015/LongLive_light/belle2-logo.png b/SUSY_2015/LongLive_light/belle2-logo.png new file mode 100644 index 0000000..9434105 --- /dev/null +++ b/SUSY_2015/LongLive_light/belle2-logo.png Binary files differ diff --git a/SUSY_2015/LongLive_light/blind.png b/SUSY_2015/LongLive_light/blind.png new file mode 100644 index 0000000..851aab2 --- /dev/null +++ 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It will be recreated as +required. + +@Control{biblatex-control, + options = {2.3:0:0:1:0:0:1:1:0:0:0:0:1:1:3:1:79:+}, +} diff --git a/SUSY_2015/LongLive_light/mchrzasz.tex b/SUSY_2015/LongLive_light/mchrzasz.tex new file mode 100644 index 0000000..af8bfaf --- /dev/null +++ b/SUSY_2015/LongLive_light/mchrzasz.tex @@ -0,0 +1,893 @@ +\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} + +\usepackage[english]{babel} +\usepackage{polski} + + +\usetheme[ + bullet=circle, % Other option: square + bigpagenumber, % circled page number on lower right + topline=true, % colored bar at the top of the frame + shadow=false, % Shading for beamer blocks + watermark=BG_lower, % png file for the watermark + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +\usepackage{emerald} +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% +\newcommand{\thetal}{\theta_l} +\newcommand{\thetak}{\theta_k} + +\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{\TeV}{\rm{TeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} + + + +\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich)} +\institute{UZH} +\title[Searches for long-lived light particles at LHCb]{Searches for long-lived light particles at LHCb} +\date{25 September 2015} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright\fontspec{Trebuchet MS}\bfseries \LARGE {Searches for long-lived light particles at LHCb} + \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} +\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + \textcolor{normal text.fg!50!Comment}{SUSY 2015, Tahoe City, 23-29 August, 2015} + + +\end{center} +\end{frame} +} + + +%------------------------------------------------------------------- +% Introduction +%------------------------------------------------------------------- +% +% Set the background for the rest of the slides. +% Insert infoline +%\setbeamertemplate{background} +% {\includegraphics[width=\paperwidth,height=\paperheight]{slide_bg}} +%\setbeamertemplate{footline}[bunsentheme] + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +%\setbeamertemplate{background} +% {\includegraphics[width=\paperwidth,height=\paperheight]{slide_bg}} +%\setbeamertemplate{footline}[bunsentheme] +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%\section{LHCb detector} + +%\begin{frame}\frametitle{LHCb detector} +%\begin{columns} +%\column{3.in} +%\begin{center} +%\includegraphics[width=0.98\textwidth]{det.jpg} +%\end{center} + +%\column{2.0in} +%\begin{footnotesize} + + + % LHCb is a forward spectrometer: + % \begin{itemize} + % \item Excellent vertex resolution. + % \item Efficient trigger. + % \item High acceptance for $\Ptau$ and $\PB$. + % \item Great Particle ID + % \end{itemize} + + + +%\end{footnotesize} +%\end{columns} + +%\end{frame} + +\section{Introduction} + +\begin{frame}\frametitle{Why long-lived particles?} +\begin{columns} +\column{3in} +\begin{itemize} +\item We all know here that the SM is incomplete. +\item Unfortunately we do no know what is the scale of NP. +\item NP still can come from the Higgs sector $\Rightarrow$ not all properties are yet constrained. +\item There is a long list of theoretical models that predict the existence +of new particles that couple to the SM sector by mixing with the +Higgs. +\end{itemize} + +\column{2in} +\includegraphics[width=0.9\textwidth]{susy/NP_couplings.png} + + +\end{columns} +\begin{itemize} + +\item Inflaton, axion-like, dark matter mediator models also predict the +new boson to be light. +\item SUSY models also can have stable long living particles like $\Psquark$, $\Pslepton$. +\end{itemize} + + +\end{frame} + +\begin{frame} +\only<1>{\frametitle{LHCb detector - tracking} +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{susy/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{susy/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]{susy/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{susy/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}\frametitle{Data taken by LHCb} +\includegraphics[width=0.9\textwidth]{susy/data.png} + +\begin{itemize} +\item In 2011 and 2012 LHCb has gathered $3~{\rm{fb^{-1}}}$ of $pp$ collisions. +\end{itemize} + +\end{frame} + + + +\section{Lepton Flavour Violation} +\begin{frame}\frametitle{Lepton Flavour/Number Violation} +\begin{small} + Lepton Flavour Violation(LFV): +\end{small} + + +\begin{footnotesize} + +After $\Pmuon$ was discovered it was natural to think of it as an excited $\Pelectron$. +\begin{columns} +\column{3in} +\begin{itemize} +\item Expected: $B(\mu\to\Pe\gamma) \approx 10^{-4}$ +\item Unless another $\Pnu$, in intermediate vector boson loop, cancels. +\end{itemize} + +\column{2in} +{~}\includegraphics[width=0.98\textwidth]{rabi.png} + +\end{columns} +\begin{columns} +\column{0.5in} +{~} +\column{3in} +\begin{block}{I.I.Rabi:} +"Who ordered that?" +\end{block} +\column{0.3in}{~} +\column{2in} +{~}\includegraphics[scale=0.08]{II_Rabi.jpg} + +\end{columns} + + +\begin{itemize} +\item Up to this day charged LFV is being searched for in various decay modes. +\item LFV was already found in neutrino sector (oscillations). +\end{itemize} +\end{footnotesize} + + +\begin{footnotesize} + +\begin{columns} +\column{3.5in} +\begin{small} + Lepton Number Violation (LNV) +\end{small} + +\begin{itemize} +\item Even with LFV, lepton number can be a conserved quantity. +\item Many NP models predict it violation(Majorana neutrinos) +\item Searched in so called Neutrinoless double $\beta$ decays. +\end{itemize} + +\column{1.5in} +\includegraphics[width=0.8\textwidth]{Double_beta_decay_feynman.png} + +\end{columns} + +\end{footnotesize} +%Double_beta_decay_feynman.png + + % \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + + +% \section{Lepton Number Violation} +\section{ $\PB$ decays} +\subsection{$\PBminus\to h^{+}\Plepton^{-}\Plepton^{-}$} +\begin{frame}%[t] +\frametitle{LNV in bottom decays}%$\PBminus\to h^{+}\ell^{-}\ell^{-}$} + +\only<1>{ +\begin{columns}\begin{column}{.5\textwidth} +on-shell neutrino + +\includegraphics[width=\textwidth]{pic/B-Majorana2.pdf} +\end{column} +{\begin{column}{.45\textwidth} +virtual neutrino + +\includegraphics[width=\textwidth]{pic/B-Majorana1.pdf} +\end{column} +} +\end{columns} +\begin{columns} +\begin{column}{.5\textwidth} +\begin{itemize} +\item resonant production in accessible mass range +\item rates depend on Majorana neutrino--lepton coupling $|V_{\mu 4}|$ +\newline {\footnotesize{(e.g.\ \href{http://arxiv.org/abs/0901.3589}{arXiv:0901.3589)}}} +\item $m_4 = m_{\Plepton^{-},\Ppiplus}$ +\item $m_{\mu} + m_{\pi} < m_4 < m_{\PB} - m_{\mu}$ +\end{itemize} +\end{column} +{ +\begin{column}{.5\textwidth} +\begin{exampleblock}{~} +%\begin{itemize} +Diagram without mass restriction + Cabbibo favoured for $\PB\to\PD$ + Analogous to double $\beta$ decay. +%\end{itemize} +\end{exampleblock} +\end{column} +} +\end{columns} +} + % \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}[t] +\frametitle{Virtual Majorana neutrinos} + + +\begin{columns} +\only<1>{ +\begin{column}{.78\textwidth} +\begin{block}{} +%\begin{itemize} + $\PBminus\to\PDplus\Pmuon\Pmuon\quad\quad\quad\quad\quad\quad\PBminus\to\PD^{*+}\Pmuon\Pmuon$ +%\end{itemize} +\includegraphics[width=\textwidth]{pic/MassFitDp_.pdf} +\end{block} +\end{column} +} + + +\end{columns} +\only<1>{{ +{~} + +\begin{columns} +\column{2.5in} +$\quad\mathcal{B}(\PBminus\to\PDplus\Pmuon\Pmuon)<6.9\times 10^{-7}$ +\column{2.5in} + +$\mathcal{B}(\PBminus\to\PD^{*+}\Pmuon\Pmuon)<2.4\times 10^{-6}$ + +\end{columns} +}} + + + {@ 95\,\% CL}\hspace{.35\textwidth} + {@ 95\,\% CL} +\\ Based on $0.41~\rm fb^{-1}${~}$7~\TeV$ data. + +{~} + +\begin{columns} +\begin{column}{6.5cm} +\end{column} +\begin{column}{1.5cm} +%\includegraphics[width=\textwidth]{pic/LHCb_logo.jpg} +\end{column} +\begin{column}{4cm} +\hspace{.4cm} + + {\footnotesize{\href{http://prd.aps.org/abstract/PRD/v85/i11/e112004}{\texttt{Phys. Rev.D85 (2012) 112004 }}}} + +\end{column} +\end{columns} + +%LHCb, arXiv:1201.5600 +%\includegraphics[width=.5\textwidth]{UpperAll} + % \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}[t] +\frametitle{On-shell Majorana neutrinos} +\begin{itemize} +\item $\PBminus \to \Ppiplus \Pmuon \Pmuon$ searched with full data set${~}3~\rm fb^{-1}$. +\item Cut based analysis. +\item Normalization channel $\PBplus \to \PJpsi(\mu\mu)\PKplus$. +\item Searches performed for two scenarios: +\begin{itemize} +\item Short life-time neutrinos: $\tau_4 <1ps$ +\item Long life-time neutrinos: $\tau_4 \in (1,1000) ps$ +\end{itemize} +\end{itemize} +\begin{columns} + +\only<1>{ +\includegraphics[width=\textwidth]{Figure2.png} +} + +\end{columns} + + +\begin{columns} +\begin{column}{8.5cm} + +\includegraphics[width=\textwidth]{Figure3.png} + +\end{column} +\begin{column}{.5cm} +%\includegraphics[width=\textwidth]{pic/LHCb_logo.jpg} +\end{column} + +\begin{column}{4cm} +\hspace{.4cm} + + + {\footnotesize{\href{http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.112.131802}{\texttt{Phys. Rev. Lett. 112, 131802 }}}} + +\end{column} +\end{columns} + + +% \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}[t] +\frametitle{On-shell Majorana neutrinos} +{~}\\ +\begin{columns} +\column{2.5in} +\includegraphics[width=\textwidth]{Figure5.png}\\ +\includegraphics[width=\textwidth]{Figure6.png}\\ + + +\column{2.5in} +\begin{small} +\begin{itemize} +\item In absence of signal UL. were set. +\item $Br(\PBminus \to \Ppiplus \Pmuon \Pmuon)$ in range $10^{-9}$. +\item Limits also set for the coupling $| V_{\mu 4} |^2$ +\end{itemize} +{~}{~}$Br(\PBminus \to \Ppiplus \Pmuon \Pmuon) = \dfrac{G_f^4 f_B^2f_{\pi}^2}{128\pi\hbar } \tau_B m_B^5 |V_{ub}V_{ud}|^2|V_{\mu4}|^4(1- \dfrac{m_4^2}{m_B^2})\dfrac{m_4}{\Gamma_{N_4}}$ +\end{small} +\end{columns} +% \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% johan %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame} +\frametitle{Summary on LNV in $\color{white} \textbf{B}$ decays} +\vspace{0.5cm} +\begin{columns} +\begin{column}{.65\textwidth} +\begin{footnotesize} +\begin{tabular}{lclr} +channel & limit & & \\\hline + $\mathcal{B}(\PBminus\to\Ppi^{+}\Pelectron\Pelectron) $ & $<2.3\times 10^{-8}$ & @$90\,\%$ CL &\includegraphics[height=.25cm]{babar}\footnote{BaBar,\href{http://link.aps.org/doi/10.1103/PhysRevD.85.071103}{Phys.\ Rev.\ D \textbf{85}, 071103} (2012)\label{babarB}}\\ + $\mathcal{B}(\PBminus\to\PK^{+}\Pelectron\Pelectron) $ & $<3.0\times 10^{-8}$ & @$90\,\%$ CL &\includegraphics[height=.25cm]{babar}\footnotesize{$^{\text{\ref{babarB}}}$}\\ + $\mathcal{B}(\PBminus\to\PK^{*+}\Pelectron\Pelectron) $ & $<2.8\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{cleo}\footnote{CLEO, \href{http://link.aps.org/doi/10.1103/PhysRevD.65.111102}{Phys.\ Rev.\ D \textbf{65}, 111102} (2002)\label{cleolnv}}\\ + $\mathcal{B}(\PBminus\to\Prho^{+}\Pelectron\Pelectron) $ & $<2.6\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{cleo}\footnotesize{$^{\text{\ref{cleolnv}}}$}\\ + $\mathcal{B}(\PBminus\to\PD^{+}\Pelectron\Pelectron) $ & $<2.6\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{belle2-logo}\footnote{Belle, \href{http://link.aps.org/doi/10.1103/PhysRevD.84.071106}{Phys.\ Rev.\ D \textbf{84}, 071106(R)}, (2011)\label{bellelnv}}\\ + $\mathcal{B}(\PBminus\to\PD^{+}\Pelectron\Pmuon) $ & $<1.8\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{belle2-logo}\footnotesize{$^{\text{\ref{bellelnv}}}$}\\ +%$\mathcal{B}(\PBminus\to\Ppi^{+}\Pmuon\Pmuon)$ & $<1.3\times 10^{-8}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnote{LHCb, CERN-PH-EP-2012-006, \href{http://arxiv.org/abs/1201.5600}{\texttt{arXiv:1201.5600}} (2012)\label{xxxxx}} \\ + + $\mathcal{B}(\PBminus\to\PK^{+}\Pmuon\Pmuon) $ & $<5.4\times 10^{-7}$ & @$95\,\%$ CL &\includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnote{LHCb, \href{http://link.aps.org/doi/10.1103/PhysRevLett.108.101601}{Phys.\ Rev.\ Lett.\ 108 101601} (2012)} \\ + %$\mathcal{B}(\PBminus\to\PK^{*+}\Pmuon\Pmuon) $ & $<4.4\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{cleo}\footnotesize{$^{\text{\ref{cleolnv}}}$}\\ + %$\mathcal{B}(\PBminus\to\Prho^{+}\Pmuon\Pmuon) $ & $<5.0\times 10^{-6}$ & @$90\,\%$ CL & \footnotesize{$^{\text{\ref{cleolnv}}}$}\\ + $\mathcal{B}(\PBminus\to\PD^{+}\Pmuon\Pmuon) $ & $<6.9\times 10^{-7}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnote{LHCb,Phys. Rev. Lett. (112) 131802 (2014)\label{xxxxx}} \\ + $\mathcal{B}(\PBminus\to\PD^{*+}\Pmuon\Pmuon)$ & $<2.4\times 10^{-6}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnotesize{$^{\text{\ref{xxxxx}}}$}\\ + $\mathcal{B}(\PBminus\to\PDs^{+}\Pmuon\Pmuon)$ & $<5.8\times 10^{-7}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnotesize{$^{\text{\ref{xxxxx}}}$}\\ + $\mathcal{B}(\PBminus\to\PDzero\Ppiminus\Pmuon\Pmuon)$ & $<1.5\times 10^{-6}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnotesize{$^{\text{\ref{xxxxx}}}$}\\ +\hline +\end{tabular} %pic/LHCb_logo.jpg +\end{footnotesize} +\end{column} +\end{columns} +%\textref{M.Chrz\k{a}szcz 2014} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PB \to \PKstar \chi(\mu\mu)$ search} +\begin{itemize} +\item Search for displaced di-muon vertex coming form $\PB$ meson. +\end{itemize} +\begin{columns} +\column{2.5in} +\begin{Large} +$\PBzero \to \PKstar \chi( \Pmuon \APmuon)$ +\end{Large} +\column{2.5in} +\includegraphics[width=0.9\textwidth]{susy/inflaton.png} +\end{columns} +\begin{itemize} +\item If $\chi$ mixes with the Higgs and it is light: +\begin{itemize} +\item $\Gamma(\PK \to \Ppi \chi) \propto m_t^4 \lambda^5$ +\item $\Gamma(\PD \to \Ppi \chi) \propto m_b^4 \lambda^5$ +\item $\Gamma(\PB \to \PK \chi) \propto m_t^4 \lambda^2$ +\end{itemize} +\item In addition; $\PKstar \to \PK^+ \Ppi^-$ helps in vertex reconstruction. +\item High $\mathcal{B}(\chi \to \Pmuon \APmuon)$. +\end{itemize} + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PB \to \PKstar \chi(\mu\mu)$ motivation} +Discussed models: +\begin{enumerate} +\item \textbf{Inflaton:} \href{http://arxiv.org/abs/1403.4638}{{\color{blue}{Phys.Lett. B736 (2014) 494}}} +\begin{itemize} +\item $\tau_{\chi} = 10^{-8} - 10^{-10}~s$ +\item $m_{\chi} ~\mathcal{O}(1~\GeV)$ +\item $\mathcal{B}(\PB \to \PK \chi)~\sim 10^{-6}$ +\item effective couplings to SM particles: +\begin{itemize} +\item $g_Y\frac{m_f}{v_{EW}},~g_Y=\sin \theta$ +\end{itemize} +\end{itemize} +\item \textbf{Axion portal:} \href{http://arxiv.org/abs/0911.5355}{{\color{blue}{Phys.Rev.D81:034001,2010}}} +\begin{itemize} +\item Prompt decay. +\item Large allowed masses. +\item Axion decay constant: $f_{\chi} \sim 1-3~\TeV$ +\begin{itemize} +\item Coupling $\propto \frac{m_f}{f_{\chi}}$. +\end{itemize} +\end{itemize} +\end{enumerate} + +All those particles have width much smaller than resolution of LHCb detector. + + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Signal properties} +$\Rrightarrow$ Depending on the coupling of the hidden sector we can identify two lifetime regimes:\\{~} + +\begin{columns} +\column{0.1in} +{~} +\column{2.5in} +\textbf{Long lifetime} ($>0.2~{\rm{ps}}$) +\begin{itemize} +\item Inflaton \href{http://arxiv.org/abs/0912.0390v2}{{\color{blue}{JHEP 1005:010}}} +\item Displaced vertex. +\item Almost background free. +\item Lower reconstruction efficiency. +\end{itemize} + +\column{2.5in} +\textbf{Short lifetime} ($\leq0.2~{\rm{ps}}$) +\begin{itemize} +\item Dark matter mediator \href{http://arxiv.org/abs/1310.6752}{{\color{blue}{ Phys. Lett. B727 }}} +\item Axion \href{http://arxiv.org/abs/0911.5355}{{\color{blue}{Phys.Rev.D81}}} +\item Prompt decay. +\item Contaminated via SM decay. +\end{itemize} + +\end{columns} +\begin{columns} +\column{0.1in} +{~} + +\column{2.5in} +\includegraphics[width=0.95\textwidth]{susy/displaced.png} + +\column{2.5in} +\includegraphics[width=0.95\textwidth]{susy/prompt.png} + +\end{columns} + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Selection} +\begin{itemize} +\item Trigger on muons. +\item Multivariate selection: ${\rm{\mu BDT}}$ \href{http://arxiv.org/abs/1305.7248}{JINST 8(2013)} +\begin{itemize} +\item ${\rm{\mu BDT}}$ ensures flat efficiency in lifetime of $\chi$. +\end{itemize} +\item Optimized on Punzi figure-of-merit: +\begin{align*} +P_a = \dfrac{S}{\frac{5}{2}+\sqrt{B}}, +\end{align*} +with $S$ and $B$ are signal and background yields. +\item Factorize lifetime into two components: $\mathcal{L}=\mathcal{L}^{{\rm{prompt}}} \bigotimes \mathcal{L}^{{\rm{displaced}}}$ +\begin{itemize} +\item Prompt: $\tau < 3\sigma_{\tau}$\\ +$\mapsto$ SM background of $\PBzero \to \PKstar \Pmuon \APmuon$ +\item Displeased: $\tau > 3\sigma_{\tau}$\\ +$\mapsto$ Almost background free. +\end{itemize} +\end{itemize} + + + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Search strategy} +\begin{columns} + +\column{0.05in} +{~} +\column{3.4in} +\begin{itemize} +\item $\PBzero$ mass constrained. +\item Di-muon mass resolution $\sigma_m =1 -7~\MeV$. +\item Scan $m_{{\rm test}}$ in steps of $0.5~\sigma_m$. +\begin{itemize} +\item {\color{orange}{Wide resonances}} can't affect the search. +\item {\color{turtlegreen}{Narrows resonances}} we veto. +\end{itemize} +\item Calculations performed in each $m_{test}$ window. +\end{itemize} +\column{1.6in} +\includegraphics[width=0.9\textwidth]{susy/williams.png} +\end{columns} + + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Results} + +\includegraphics[width=0.95\textwidth]{susy/results.png} + +$\Rrightarrow$ Grey regions correspond to vetoed regions where narrow resonances are expected.\\ +$\Rrightarrow$ Largest deviation seen in $m_{\chi}=253~\MeV$.\\ +$\rightarrowtail$ Not statistically significant: local p-value $=0.2$.\\ + +$\Rrightarrow$ \href{http://arxiv.org/abs/1508.04094}{\color{blue}{LHCb-PAPER-2015-036}} submited to PRL. + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Branching fraction exclusion limit} + +\includegraphics[width=0.95\textwidth]{susy/limit.png} + +$\Rrightarrow$ No deviations from background only hypothesis is observed. +\begin{itemize} +\item We set a $95\%$ CL upper limit as function of mass and lifetime of the new particle (in the LHCb accessible range). +\item Lower lifetimes have better limit due to higher reconstruction efficiency. +\end{itemize} + + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Benchmark models} + + + +$\Rrightarrow$ Interpretation of the results in two specific models:\\{~}\\ + +\includegraphics[width=1.05\textwidth]{susy/benchmarks.png} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Conclusion} +\begin{itemize} +\item A search for a dark boson in the decay channel\\ $\PBzero \to \PKstar \Pmuon \APmuon$ has been presented. +\begin{itemize} +\item No deviations from SM observed. + +\end{itemize} +\item Results are the most constraining exclusion limit on the process. +\item LHCb is suited for search for long lived particles. +\item Stay tuned, more searches like this are on they way. + +\end{itemize} + + + +\end{frame} + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/SUSY_2015/LongLive_light/mchrzasz.tex~ b/SUSY_2015/LongLive_light/mchrzasz.tex~ new file mode 100644 index 0000000..5572ca0 --- /dev/null +++ b/SUSY_2015/LongLive_light/mchrzasz.tex~ @@ -0,0 +1,893 @@ +\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} + +\usepackage[english]{babel} +\usepackage{polski} + + +\usetheme[ + bullet=circle, % Other option: square + bigpagenumber, % circled page number on lower right + topline=true, % colored bar at the top of the frame + shadow=false, % Shading for beamer blocks + watermark=BG_lower, % png file for the watermark + ]{Flip} + +%\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} + + +\usepackage[lf]{berenis} +\usepackage[LY1]{fontenc} +\usepackage[utf8]{inputenc} + +\usepackage{emerald} +\usefonttheme{professionalfonts} +\usepackage[no-math]{fontspec} +\defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly + +\setmainfont{Gillius ADF} % Beamer ignores "main font" in favor of sans font +\setsansfont{Gillius ADF} % This is the font that beamer will use by default +% \setmainfont{Gill Sans Light} % Prettier, but harder to read + +\setbeamerfont{title}{family=\fontspec{Gillius ADF}} + +\input t1augie.fd + +%\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font +%\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font +% \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie + +%% Gill Sans doesn't look very nice when boldfaced +%% This is a hack to use Helvetica instead +%% Usage: \textbf{\forbold some stuff} +%\newcommand{\forbold}{\fontspec{Arial}} + +\usepackage{graphicx} +\usepackage[export]{adjustbox} + +\usepackage{amsmath} +\usepackage{amsfonts} +\usepackage{amssymb} +\usepackage{bm} +\usepackage{colortbl} +\usepackage{mathrsfs} % For Weinberg-esque letters +\usepackage{cancel} % For "SUSY-breaking" symbol +\usepackage{slashed} % for slashed characters in math mode +\usepackage{bbm} % for \mathbbm{1} (unit matrix) +\usepackage{amsthm} % For theorem environment +\usepackage{multirow} % For multi row cells in table +\usepackage{arydshln} % For dashed lines in arrays and tables +\usepackage{siunitx} +\usepackage{xhfill} +\usepackage{grffile} +\usepackage{textpos} +\usepackage{subfigure} +\usepackage{tikz} + +%\usepackage{hepparticles} +\usepackage[italic]{hepparticles} + +\usepackage{hepnicenames} + +% Drawing a line +\tikzstyle{lw} = [line width=20pt] +\newcommand{\topline}{% + \tikz[remember picture,overlay] {% + \draw[crimsonred] ([yshift=-23.5pt]current page.north west) + -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} + + + +% % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % +\usepackage{tikzfeynman} % For Feynman diagrams +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram +% http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +% http://www.math.ucla.edu/~getreuer/tikz.html +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Uncomment for more conventional arrows + vector/.style={decorate, decoration={snake}, draw}, + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, + fermion/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, + fermionbar/.style={draw=gray, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, + fermionnoarrow/.style={draw=gray}, + gluon/.style={decorate, draw=black, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + scalarbar/.style={dashed,draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, + scalarnoarrow/.style={dashed,draw=black}, + electron/.style={draw=black, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, + bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, +} + +% TIKZ - for block diagrams, +% from http://www.texample.net/tikz/examples/control-system-principles/ +% \usetikzlibrary{shapes,arrows} +\tikzstyle{block} = [draw, rectangle, +minimum height=3em, minimum width=6em] + + + + +\usetikzlibrary{backgrounds} +\usetikzlibrary{mindmap,trees} % For mind map +\newcommand{\degree}{\ensuremath{^\circ}} +\newcommand{\E}{\mathrm{E}} +\newcommand{\Var}{\mathrm{Var}} +\newcommand{\Cov}{\mathrm{Cov}} +\newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut +\newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut + +\graphicspath{{images/}} % Put all images in this directory. Avoids clutter. + +% SOME COMMANDS THAT I FIND HANDY +% \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec +\newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild +\newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold +\newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold +\newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert +\newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert +%% "\alert" is already a beamer pre-defined +\newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% +\newcommand{\thetal}{\theta_l} +\newcommand{\thetak}{\theta_k} + +\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{\TeV}{\rm{TeV}} +\newcommand{\im}{\rm{Im}} +\newcommand{\disp}{\displaystyle} +\def\be{\begin{equation}} +\def\ee{\end{equation}} +\def\ba{\begin{eqnarray}} +\def\ea{\end{eqnarray}} +\def\d{\partial} +\def\l{\left(} +\def\r{\right)} +\def\la{\langle} +\def\ra{\rangle} +\def\e{{\rm e}} +\def\Br{{\rm Br}} + + + +\author{ {\fontspec{Trebuchet MS}Marcin Chrz\k{a}szcz} (Universit\"{a}t Z\"{u}rich)} +\institute{UZH} +\title[Searches for long-lived light particles at LHCb]{Searches for long-lived light particles at LHCb} +\date{25 September 2015} + + +\begin{document} +\tikzstyle{every picture}+=[remember picture] + +{ +\setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} +\begin{frame}[c]%{\phantom{title page}} +\begin{center} +\begin{center} + \begin{columns} + \begin{column}{0.75\textwidth} + \flushright\fontspec{Trebuchet MS}\bfseries \LARGE {Searches for long-lived light particles at LHCb} + \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} +\end{column} +\end{columns} + +\vspace{1em} +% \footnotesize\textcolor{gray}{With N. Serra, B. Storaci\\Thanks to the theory support from M. Shaposhnikov, D. Gorbunov}\normalsize\\ +\vspace{0.5em} + \textcolor{normal text.fg!50!Comment}{SUSY 2015, Tahoe City, 23-29 August, 2015} + + +\end{center} +\end{frame} +} + + +%------------------------------------------------------------------- +% Introduction +%------------------------------------------------------------------- +% +% Set the background for the rest of the slides. +% Insert infoline +%\setbeamertemplate{background} +% {\includegraphics[width=\paperwidth,height=\paperheight]{slide_bg}} +%\setbeamertemplate{footline}[bunsentheme] + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +%\setbeamertemplate{background} +% {\includegraphics[width=\paperwidth,height=\paperheight]{slide_bg}} +%\setbeamertemplate{footline}[bunsentheme] +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +%\section{LHCb detector} + +%\begin{frame}\frametitle{LHCb detector} +%\begin{columns} +%\column{3.in} +%\begin{center} +%\includegraphics[width=0.98\textwidth]{det.jpg} +%\end{center} + +%\column{2.0in} +%\begin{footnotesize} + + + % LHCb is a forward spectrometer: + % \begin{itemize} + % \item Excellent vertex resolution. + % \item Efficient trigger. + % \item High acceptance for $\Ptau$ and $\PB$. + % \item Great Particle ID + % \end{itemize} + + + +%\end{footnotesize} +%\end{columns} + +%\end{frame} + +\section{Introduction} + +\begin{frame}\frametitle{Why long-lived particles?} +\begin{columns} +\column{3in} +\begin{itemize} +\item We all know here that the SM is incomplete. +\item Unfortunately we do no know what is the scale of NP. +\item NP still can come from the Higgs sector $\Rightarrow$ not all properties are yet constrained. +\item There is a long list of theoretical models that predict the existence +of new particles that couple to the SM sector by mixing with the +Higgs. +\end{itemize} + +\column{2in} +\includegraphics[width=0.9\textwidth]{susy/NP_couplings.png} + + +\end{columns} +\begin{itemize} + +\item Inflaton, axion-like, dark matter mediator models also predict the +new boson to be light. +\item SUSY models also can have stable long living particles like $\Psquark$, $\Pslepton$. +\end{itemize} + + +\end{frame} + +\begin{frame} +\only<1>{\frametitle{LHCb detector - tracking} +\begin{columns} +\column{3in} +\includegraphics[width=0.9\textwidth]{susy/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{susy/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]{susy/1050px-Lhcbview.jpg} + +\column{2in} +\includegraphics[width=0.95\textwidth]{susy/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}\frametitle{Data taken by LHCb} +\includegraphics[width=0.9\textwidth]{susy/data.png} + +\begin{itemize} +\item In 2011 and 2012 LHCb has gathered $3~{\rm{fb^{-1}}}$ of $pp$ collisions. +\end{itemize} + +\end{frame} + + + +\section{Lepton Flavour Violation} +\begin{frame}\frametitle{Lepton Flavour/Number Violation} +\begin{small} + Lepton Flavour Violation(LFV): +\end{small} + + +\begin{footnotesize} + +After $\Pmuon$ was discovered it was natural to think of it as an excited $\Pelectron$. +\begin{columns} +\column{3in} +\begin{itemize} +\item Expected: $B(\mu\to\Pe\gamma) \approx 10^{-4}$ +\item Unless another $\Pnu$, in intermediate vector boson loop, cancels. +\end{itemize} + +\column{2in} +{~}\includegraphics[width=0.98\textwidth]{rabi.png} + +\end{columns} +\begin{columns} +\column{0.5in} +{~} +\column{3in} +\begin{block}{I.I.Rabi:} +"Who ordered that?" +\end{block} +\column{0.3in}{~} +\column{2in} +{~}\includegraphics[scale=0.08]{II_Rabi.jpg} + +\end{columns} + + +\begin{itemize} +\item Up to this day charged LFV is being searched for in various decay modes. +\item LFV was already found in neutrino sector (oscillations). +\end{itemize} +\end{footnotesize} + + +\begin{footnotesize} + +\begin{columns} +\column{3.5in} +\begin{small} + Lepton Number Violation (LNV) +\end{small} + +\begin{itemize} +\item Even with LFV, lepton number can be a conserved quantity. +\item Many NP models predict it violation(Majorana neutrinos) +\item Searched in so called Neutrinoless double $\beta$ decays. +\end{itemize} + +\column{1.5in} +\includegraphics[width=0.8\textwidth]{Double_beta_decay_feynman.png} + +\end{columns} + +\end{footnotesize} +%Double_beta_decay_feynman.png + + % \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + + +% \section{Lepton Number Violation} +\section{ $\PB$ decays} +\subsection{$\PBminus\to h^{+}\Plepton^{-}\Plepton^{-}$} +\begin{frame}%[t] +\frametitle{LNV in bottom decays}%$\PBminus\to h^{+}\ell^{-}\ell^{-}$} + +\only<1>{ +\begin{columns}\begin{column}{.5\textwidth} +on-shell neutrino + +\includegraphics[width=\textwidth]{pic/B-Majorana2.pdf} +\end{column} +{\begin{column}{.45\textwidth} +virtual neutrino + +\includegraphics[width=\textwidth]{pic/B-Majorana1.pdf} +\end{column} +} +\end{columns} +\begin{columns} +\begin{column}{.5\textwidth} +\begin{itemize} +\item resonant production in accessible mass range +\item rates depend on Majorana neutrino--lepton coupling $|V_{\mu 4}|$ +\newline {\footnotesize{(e.g.\ \href{http://arxiv.org/abs/0901.3589}{arXiv:0901.3589)}}} +\item $m_4 = m_{\Plepton^{-},\Ppiplus}$ +\item $m_{\mu} + m_{\pi} < m_4 < m_{\PB} - m_{\mu}$ +\end{itemize} +\end{column} +{ +\begin{column}{.5\textwidth} +\begin{exampleblock}{~} +%\begin{itemize} +Diagram without mass restriction + Cabbibo favoured for $\PB\to\PD$ + Analogous to double $\beta$ decay. +%\end{itemize} +\end{exampleblock} +\end{column} +} +\end{columns} +} + % \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}[t] +\frametitle{Virtual Majorana neutrinos} + + +\begin{columns} +\only<1>{ +\begin{column}{.78\textwidth} +\begin{block}{} +%\begin{itemize} + $\PBminus\to\PDplus\Pmuon\Pmuon\quad\quad\quad\quad\quad\quad\PBminus\to\PD^{*+}\Pmuon\Pmuon$ +%\end{itemize} +\includegraphics[width=\textwidth]{pic/MassFitDp_.pdf} +\end{block} +\end{column} +} + + +\end{columns} +\only<1>{{ +{~} + +\begin{columns} +\column{2.5in} +$\quad\mathcal{B}(\PBminus\to\PDplus\Pmuon\Pmuon)<6.9\times 10^{-7}$ +\column{2.5in} + +$\mathcal{B}(\PBminus\to\PD^{*+}\Pmuon\Pmuon)<2.4\times 10^{-6}$ + +\end{columns} +}} + + + {@ 95\,\% CL}\hspace{.35\textwidth} + {@ 95\,\% CL} +\\ Based on $0.41~\rm fb^{-1}${~}$7~\TeV$ data. + +{~} + +\begin{columns} +\begin{column}{6.5cm} +\end{column} +\begin{column}{1.5cm} +%\includegraphics[width=\textwidth]{pic/LHCb_logo.jpg} +\end{column} +\begin{column}{4cm} +\hspace{.4cm} + + {\footnotesize{\href{http://prd.aps.org/abstract/PRD/v85/i11/e112004}{\texttt{Phys. Rev.D85 (2012) 112004 }}}} + +\end{column} +\end{columns} + +%LHCb, arXiv:1201.5600 +%\includegraphics[width=.5\textwidth]{UpperAll} + % \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}[t] +\frametitle{On-shell Majorana neutrinos} +\begin{itemize} +\item $\PBminus \to \Ppiplus \Pmuon \Pmuon$ searched with full data set${~}3~\rm fb^{-1}$. +\item Cut based analysis. +\item Normalization channel $\PBplus \to \PJpsi(\mu\mu)\PKplus$. +\item Searches performed for two scenarios: +\begin{itemize} +\item Short life-time neutrinos: $\tau_4 <1ps$ +\item Long life-time neutrinos: $\tau_4 \in (1,1000) ps$ +\end{itemize} +\end{itemize} +\begin{columns} + +\only<1>{ +\includegraphics[width=\textwidth]{Figure2.png} +} + +\end{columns} + + +\begin{columns} +\begin{column}{8.5cm} + +\includegraphics[width=\textwidth]{Figure3.png} + +\end{column} +\begin{column}{.5cm} +%\includegraphics[width=\textwidth]{pic/LHCb_logo.jpg} +\end{column} + +\begin{column}{4cm} +\hspace{.4cm} + + + {\footnotesize{\href{http://journals.aps.org/prl/abstract/10.1103/PhysRevLett.112.131802}{\texttt{Phys. Rev. Lett. 112, 131802 }}}} + +\end{column} +\end{columns} + + +% \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame}[t] +\frametitle{On-shell Majorana neutrinos} +{~}\\ +\begin{columns} +\column{2.5in} +\includegraphics[width=\textwidth]{Figure5.png}\\ +\includegraphics[width=\textwidth]{Figure6.png}\\ + + +\column{2.5in} +\begin{small} +\begin{itemize} +\item In absence of signal UL. were set. +\item $Br(\PBminus \to \Ppiplus \Pmuon \Pmuon)$ in range $10^{-9}$. +\item Limits also set for the coupling $| V_{\mu 4} |^2$ +\end{itemize} +{~}{~}$Br(\PBminus \to \Ppiplus \Pmuon \Pmuon) = \dfrac{G_f^4 f_B^2f_{\pi}^2}{128\pi\hbar } \tau_B m_B^5 |V_{ub}V_{ud}|^2|V_{\mu4}|^4(1- \dfrac{m_4^2}{m_B^2})\dfrac{m_4}{\Gamma_{N_4}}$ +\end{small} +\end{columns} +% \textref{M.Chrz\k{a}szcz 2014} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% johan %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\begin{frame} +\frametitle{Summary on LNV in $\color{white} \textbf{B}$ decays} +\vspace{0.5cm} +\begin{columns} +\begin{column}{.65\textwidth} +\begin{footnotesize} +\begin{tabular}{lclr} +channel & limit & & \\\hline + $\mathcal{B}(\PBminus\to\Ppi^{+}\Pelectron\Pelectron) $ & $<2.3\times 10^{-8}$ & @$90\,\%$ CL &\includegraphics[height=.25cm]{babar}\footnote{BaBar,\href{http://link.aps.org/doi/10.1103/PhysRevD.85.071103}{Phys.\ Rev.\ D \textbf{85}, 071103} (2012)\label{babarB}}\\ + $\mathcal{B}(\PBminus\to\PK^{+}\Pelectron\Pelectron) $ & $<3.0\times 10^{-8}$ & @$90\,\%$ CL &\includegraphics[height=.25cm]{babar}\footnotesize{$^{\text{\ref{babarB}}}$}\\ + $\mathcal{B}(\PBminus\to\PK^{*+}\Pelectron\Pelectron) $ & $<2.8\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{cleo}\footnote{CLEO, \href{http://link.aps.org/doi/10.1103/PhysRevD.65.111102}{Phys.\ Rev.\ D \textbf{65}, 111102} (2002)\label{cleolnv}}\\ + $\mathcal{B}(\PBminus\to\Prho^{+}\Pelectron\Pelectron) $ & $<2.6\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{cleo}\footnotesize{$^{\text{\ref{cleolnv}}}$}\\ + $\mathcal{B}(\PBminus\to\PD^{+}\Pelectron\Pelectron) $ & $<2.6\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{belle2-logo}\footnote{Belle, \href{http://link.aps.org/doi/10.1103/PhysRevD.84.071106}{Phys.\ Rev.\ D \textbf{84}, 071106(R)}, (2011)\label{bellelnv}}\\ + $\mathcal{B}(\PBminus\to\PD^{+}\Pelectron\Pmuon) $ & $<1.8\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{belle2-logo}\footnotesize{$^{\text{\ref{bellelnv}}}$}\\ +%$\mathcal{B}(\PBminus\to\Ppi^{+}\Pmuon\Pmuon)$ & $<1.3\times 10^{-8}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnote{LHCb, CERN-PH-EP-2012-006, \href{http://arxiv.org/abs/1201.5600}{\texttt{arXiv:1201.5600}} (2012)\label{xxxxx}} \\ + + $\mathcal{B}(\PBminus\to\PK^{+}\Pmuon\Pmuon) $ & $<5.4\times 10^{-7}$ & @$95\,\%$ CL &\includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnote{LHCb, \href{http://link.aps.org/doi/10.1103/PhysRevLett.108.101601}{Phys.\ Rev.\ Lett.\ 108 101601} (2012)} \\ + %$\mathcal{B}(\PBminus\to\PK^{*+}\Pmuon\Pmuon) $ & $<4.4\times 10^{-6}$ & @$90\,\%$ CL & \includegraphics[height=.25cm]{cleo}\footnotesize{$^{\text{\ref{cleolnv}}}$}\\ + %$\mathcal{B}(\PBminus\to\Prho^{+}\Pmuon\Pmuon) $ & $<5.0\times 10^{-6}$ & @$90\,\%$ CL & \footnotesize{$^{\text{\ref{cleolnv}}}$}\\ + $\mathcal{B}(\PBminus\to\PD^{+}\Pmuon\Pmuon) $ & $<6.9\times 10^{-7}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnote{LHCb,Phys. Rev. Lett. (112) 131802 (2014)\label{xxxxx}} \\ + $\mathcal{B}(\PBminus\to\PD^{*+}\Pmuon\Pmuon)$ & $<2.4\times 10^{-6}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnotesize{$^{\text{\ref{xxxxx}}}$}\\ + $\mathcal{B}(\PBminus\to\PDs^{+}\Pmuon\Pmuon)$ & $<5.8\times 10^{-7}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnotesize{$^{\text{\ref{xxxxx}}}$}\\ + $\mathcal{B}(\PBminus\to\PDzero\Ppiminus\Pmuon\Pmuon)$ & $<1.5\times 10^{-6}$ & @$95\,\%$ CL & \includegraphics[height=.25cm]{pic/LHCb_logo.jpg}\footnotesize{$^{\text{\ref{xxxxx}}}$}\\ +\hline +\end{tabular} %pic/LHCb_logo.jpg +\end{footnotesize} +\end{column} +\end{columns} +%\textref{M.Chrz\k{a}szcz 2014} +\end{frame} + + + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PB \to \PKstar \chi(\mu\mu)$ search} +\begin{itemize} +\item Search for displaced di-muon vertex coming form $\PB$ meson. +\end{itemize} +\begin{columns} +\column{2.5in} +\begin{Large} +$\PBzero \to \PKstar \chi( \Pmuon \APmuon)$ +\end{Large} +\column{2.5in} +\includegraphics[width=0.9\textwidth]{susy/inflaton.png} +\end{columns} +\begin{itemize} +\item If $\chi$ mixes with the Higgs and it is light: +\begin{itemize} +\item $\Gamma(\PK \to \Ppi \chi) \propto m_t^4 \lambda^5$ +\item $\Gamma(\PD \to \Ppi \chi) \propto m_b^4 \lambda^5$ +\item $\Gamma(\PB \to \PK \chi) \propto m_t^4 \lambda^2$ +\end{itemize} +\item In addition; $\PKstar \to \PK^+ \Ppi^-$ helps in vertex reconstruction. +\item High $\mathcal{B}(\chi \to \Pmuon \APmuon)$. +\end{itemize} + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% +\begin{frame}\frametitle{$\PB \to \PKstar \chi(\mu\mu)$ motivation} +Discussed models: +\begin{enumerate} +\item \textbf{Inflaton:} \href{http://arxiv.org/abs/1403.4638}{{\color{blue}{Phys.Lett. B736 (2014) 494}}} +\begin{itemize} +\item $\tau_{\chi} = 10^{-8} - 10^{-10}~s$ +\item $m_{\chi} ~\mathcal{O}(1~\GeV)$ +\item $\mathcal{B}(\PB \to \PK \chi)~\sim 10^{-6}$ +\item effective couplings to SM particles: +\begin{itemize} +\item $g_Y\frac{m_f}{v_{EW}},~g_Y=\sin \theta$ +\end{itemize} +\end{itemize} +\item \textbf{Axion portal:} \href{http://arxiv.org/abs/0911.5355}{{\color{blue}{Phys.Rev.D81:034001,2010}}} +\begin{itemize} +\item Prompt decay. +\item Large allowed masses. +\item Axion decay constant: $f_{\chi} \sim 1-3~\TeV$ +\begin{itemize} +\item Coupling $\propto \frac{m_f}{f_{\chi}}$. +\end{itemize} +\end{itemize} +\end{enumerate} + +All those particles have width much smaller than resolution of LHCb detector. + + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Signal properties} +$\Rrightarrow$ Depending on the coupling of the hidden sector we can identify two lifetime regimes:\\{~} + +\begin{columns} +\column{0.1in} +{~} +\column{2.5in} +\textbf{Long lifetime} ($>0.2~{\rm{ps}}$) +\begin{itemize} +\item Inflaton \href{http://arxiv.org/abs/0912.0390v2}{{\color{blue}{JHEP 1005:010}}} +\item Displaced vertex. +\item Almost background free. +\item Lower reconstruction efficiency. +\end{itemize} + +\column{2.5in} +\textbf{Short lifetime} ($\leq0.2~{\rm{ps}}$) +\begin{itemize} +\item Dark matter mediator \href{http://arxiv.org/abs/1310.6752}{{\color{blue}{ Phys. Lett. B727 }}} +\item Axion \href{http://arxiv.org/abs/0911.5355}{{\color{blue}{Phys.Rev.D81}}} +\item Prompt decay. +\item Contaminated via SM decay. +\end{itemize} + +\end{columns} +\begin{columns} +\column{0.1in} +{~} + +\column{2.5in} +\includegraphics[width=0.95\textwidth]{susy/displaced.png} + +\column{2.5in} +\includegraphics[width=0.95\textwidth]{susy/prompt.png} + +\end{columns} + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Selection} +\begin{itemize} +\item Trigger on muons. +\item Multivariate selection: ${\rm{\mu BDT}}$ \href{http://arxiv.org/abs/1305.7248}{JINST 8(2013)} +\begin{itemize} +\item ${\rm{\mu BDT}}$ ensures flat efficiency in lifetime of $\chi$. +\end{itemize} +\item Optimized on Punzi figure-of-merit: +\begin{align*} +P_a = \dfrac{S}{\frac{5}{2}+\sqrt{B}}, +\end{align*} +with $S$ and $B$ are signal and background yields. +\item Factorize lifetime into two components: $\mathcal{L}=\mathcal{L}^{{\rm{prompt}}} \bigotimes \mathcal{L}^{{\rm{displaced}}}$ +\begin{itemize} +\item Prompt: $\tau < 3\sigma_{\tau}$\\ +$\mapsto$ SM background of $\PBzero \to \PKstar \Pmuon \APmuon$ +\item Displeased: $\tau > 3\sigma_{\tau}$\\ +$\mapsto$ Almost background free. +\end{itemize} +\end{itemize} + + + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Search strategy} +\begin{columns} + +\column{0.05in} +{~} +\column{3.4in} +\begin{itemize} +\item $\PBzero$ mass constrained. +\item Di-muon mass resolution $\sigma_m =1 -7~\MeV$. +\item Scan $m_{{\rm test}}$ in steps of $0.5~\sigma_m$. +\begin{itemize} +\item {\color{orange}{Wide resonances}} can't affect the search. +\item {\color{turtlegreen}{Narrows resonances}} we veto. +\end{itemize} +\item Calculations performed in each $m_{test}$ window. +\end{itemize} +\column{1.6in} +\includegraphics[width=0.9\textwidth]{susy/williams.png} +\end{columns} + + +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Results} + +\includegraphics[width=0.95\textwidth]{susy/results.png} + +$\Rrightarrow$ Grey regions correspond to vetoed regions where narrow resonances are expected.\\ +$\Rrightarrow$ Largest deviation seen in $m_{\chi}=253~\MeV$.\\ +$\rightarrowtail$ Not statistically significant: local p-value $=0.2$.\\ + +$\Rrightarrow$ \href{http://arxiv.org/abs/1508.04094}{color{blue}{LHCb-PAPER-2015-036}} submited to PRL. + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Branching fraction exclusion limit} + +\includegraphics[width=0.95\textwidth]{susy/limit.png} + +$\Rrightarrow$ No deviations from background only hypothesis is observed. +\begin{itemize} +\item We set a $95\%$ CL upper limit as function of mass and lifetime of the new particle (in the LHCb accessible range). +\item Lower lifetimes have better limit due to higher reconstruction efficiency. +\end{itemize} + + +\end{frame} + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Benchmark models} + + + +$\Rrightarrow$ Interpretation of the results in two specific models:\\{~}\\ + +\includegraphics[width=1.05\textwidth]{susy/benchmarks.png} +\end{frame} + + +%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 +\begin{frame}\frametitle{Conclusion} +\begin{itemize} +\item A search for a dark boson in the decay channel\\ $\PBzero \to \PKstar \Pmuon \APmuon$ has been presented. +\begin{itemize} +\item No deviations from SM observed. + +\end{itemize} +\item Results are the most constraining exclusion limit on the process. +\item LHCb is suited for search for long lived particles. +\item Stay tuned, more searches like this are on they way. + +\end{itemize} + + + +\end{frame} + + +\backupbegin + +\begin{frame}\frametitle{Backup} +\topline + +\end{frame} + +\backupend + +\end{document} diff --git a/SUSY_2015/LongLive_light/pic/2d-data2.pdf b/SUSY_2015/LongLive_light/pic/2d-data2.pdf new file mode 100644 index 0000000..c1b70e3 --- /dev/null +++ b/SUSY_2015/LongLive_light/pic/2d-data2.pdf Binary files differ diff 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+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% + +\usepackage{tikz} +\usetikzlibrary{arrows,shapes} +\usetikzlibrary{trees} +\usetikzlibrary{matrix,arrows} % For commutative diagram + % http://www.felixl.de/commu.pdf +\usetikzlibrary{positioning} % For "above of=" commands +\usetikzlibrary{calc,through} % For coordinates +\usetikzlibrary{decorations.pathreplacing} % For curly braces +\usepackage[tikz]{bclogo} % For cute logo boxes +\usepackage{pgffor} % For repeating patterns + +\usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams +\usetikzlibrary{decorations.markings} +\tikzset{ + % >=stealth', %% Different kind of arrows + vector/.style={decorate, decoration={snake}, draw}, + fermion/.style={postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + fermionbar/.style={draw, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + fermionnoarrow/.style={}, + gluon/.style={decorate, + decoration={coil,amplitude=4pt, segment length=5pt}}, + scalar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{>}}}}, + scalarbar/.style={dashed, postaction={decorate}, + decoration={markings,mark=at position .55 with {\arrow{<}}}}, + scalarnoarrow/.style={dashed,draw}, +% +%% Special vectors (when you need to fine-tune wiggles) + provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, + antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, +} + diff --git a/SUSY_2015/LongLive_light/topob2.png b/SUSY_2015/LongLive_light/topob2.png new file mode 100644 index 0000000..4b5d5cd --- /dev/null +++ b/SUSY_2015/LongLive_light/topob2.png Binary files differ diff --git a/SUSY_2015/LongLive_light/uzh.jpg b/SUSY_2015/LongLive_light/uzh.jpg new file mode 100644 index 0000000..ba6a5bc --- /dev/null +++ b/SUSY_2015/LongLive_light/uzh.jpg Binary files differ