\documentclass[11 pt,xcolor={dvipsnames,svgnames,x11names,table}]{beamer} \usepackage[english]{babel} \usepackage{polski} \usetheme[ bullet=circle, % Other option: square bigpagenumber, % circled page number on lower right topline=true, % colored bar at the top of the frame shadow=false, % Shading for beamer blocks watermark=BG_lower, % png file for the watermark ]{Flip} %\logo{\kern+1.em\includegraphics[height=1cm]{SHiP-3_LightCharcoal}} \usepackage[lf]{berenis} \usepackage[LY1]{fontenc} \usepackage[utf8]{inputenc} \usefonttheme{professionalfonts} \usepackage[no-math]{fontspec} \defaultfontfeatures{Mapping=tex-text} % This seems to be important for mapping glyphs properly \setmainfont{Times} % Beamer ignores "main font" in favor of sans font \setsansfont{Times} % This is the font that beamer will use by default % \setmainfont{Gill Sans Light} % Prettier, but harder to read \setbeamerfont{title}{family=\fontspec{Times}} \input t1augie.fd %\newcommand{\handwriting}{\fontspec{augie}} % From Emerald City, free font %\newcommand{\handwriting}{\usefont{T1}{fau}{m}{n}} % From Emerald City, free font % \newcommand{\handwriting}{} % If you prefer no special handwriting font or don't have augie %% Gill Sans doesn't look very nice when boldfaced %% This is a hack to use Helvetica instead %% Usage: \textbf{\forbold some stuff} %\newcommand{\forbold}{\fontspec{Arial}} \usepackage{graphicx} \usepackage[export]{adjustbox} \usepackage{amsmath} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{colortbl} \usepackage{mathrsfs} % For Weinberg-esque letters \usepackage{cancel} % For "SUSY-breaking" symbol \usepackage{slashed} % for slashed characters in math mode \usepackage{bbm} % for \mathbbm{1} (unit matrix) \usepackage{amsthm} % For theorem environment \usepackage{multirow} % For multi row cells in table \usepackage{arydshln} % For dashed lines in arrays and tables \usepackage{siunitx} \usepackage{xhfill} \usepackage{grffile} \usepackage{textpos} \usepackage{subfigure} \usepackage{tikz} %\usepackage{hepparticles} \usepackage[italic]{hepparticles} \usepackage{hepnicenames} % Drawing a line \tikzstyle{lw} = [line width=20pt] \newcommand{\topline}{% \tikz[remember picture,overlay] {% \draw[crimsonred] ([yshift=-23.5pt]current page.north west) -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % \usepackage{tikzfeynman} % For Feynman diagrams \usetikzlibrary{arrows,shapes} \usetikzlibrary{trees} \usetikzlibrary{matrix,arrows} % For commutative diagram % http://www.felixl.de/commu.pdf \usetikzlibrary{positioning} % For "above of=" commands \usetikzlibrary{calc,through} % For coordinates \usetikzlibrary{decorations.pathreplacing} % For curly braces % http://www.math.ucla.edu/~getreuer/tikz.html \usepackage{pgffor} % For repeating patterns \usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams \usetikzlibrary{decorations.markings} \tikzset{ % >=stealth', %% Uncomment for more conventional arrows vector/.style={decorate, decoration={snake}, draw}, provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, fermion/.style={draw=gray, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, fermionbar/.style={draw=gray, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, fermionnoarrow/.style={draw=gray}, gluon/.style={decorate, draw=black, decoration={coil,amplitude=4pt, segment length=5pt}}, scalar/.style={dashed,draw=black, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, scalarbar/.style={dashed,draw=black, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, scalarnoarrow/.style={dashed,draw=black}, electron/.style={draw=black, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, } % TIKZ - for block diagrams, % from http://www.texample.net/tikz/examples/control-system-principles/ % \usetikzlibrary{shapes,arrows} \tikzstyle{block} = [draw, rectangle, minimum height=3em, minimum width=6em] \usetikzlibrary{backgrounds} \usetikzlibrary{mindmap,trees} % For mind map \newcommand{\degree}{\ensuremath{^\circ}} \newcommand{\E}{\mathrm{E}} \newcommand{\Var}{\mathrm{Var}} \newcommand{\Cov}{\mathrm{Cov}} \newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut \newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut \graphicspath{{images/}} % Put all images in this directory. Avoids clutter. % SOME COMMANDS THAT I FIND HANDY % \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec \newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild \newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold \newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold \newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert \newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert %% "\alert" is already a beamer pre-defined \newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% \def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} \usepackage{gmp} \usepackage[final]{feynmp-auto} \usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} \bibliography{bib} \setbeamertemplate{bibliography item}[text] \makeatletter\let\frametextheight\beamer@frametextheight\makeatother % suppress frame numbering for backup slides % you always need the appendix for this! \newcommand{\backupbegin}{ \newcounter{framenumberappendix} \setcounter{framenumberappendix}{\value{framenumber}} } \newcommand{\backupend}{ \addtocounter{framenumberappendix}{-\value{framenumber}} \addtocounter{framenumber}{\value{framenumberappendix}} } \definecolor{links}{HTML}{2A1B81} %\hypersetup{colorlinks,linkcolor=,urlcolor=links} % For shapo's formulas: \def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} \def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} \newcommand{\lsim}{\mathop{\lsi}} \newcommand{\gsim}{\mathop{\gsi}} \newcommand{\wt}{\widetilde} %\newcommand{\ol}{\overline} \newcommand{\Tr}{\rm{Tr}} \newcommand{\tr}{\rm{tr}} \newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} \newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} \newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} \newcommand{\eV}{\rm{eV}} \newcommand{\keV}{\rm{keV}} \newcommand{\GeV}{\rm{GeV}} \newcommand{\im}{\rm{Im}} \newcommand{\disp}{\displaystyle} \def\be{\begin{equation}} \def\ee{\end{equation}} \def\ba{\begin{eqnarray}} \def\ea{\end{eqnarray}} \def\d{\partial} \def\l{\left(} \def\r{\right)} \def\la{\langle} \def\ra{\rangle} \def\e{{\rm e}} \def\Br{{\rm Br}} \def\LcTopmumu{\Lambda_c^{+} \to p \mu^+ \mu^-} \def\Lc{\Lambda_c^{+}} \def\mumu{\mu\mu} \newcommand{\BRof}[1]{\ensuremath{{\cal B}(#1)}\xspace} \def\LcTopphi{\Lc \to p \Pphi (\mumu)} \def\Lcpomegano{\Lc \to p \omega} \def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} \def\ARROWR{{\color{WildStrawberry}{$\Rrightarrow$}}\xspace} \def\pt{p_T} \def\mevc{MeV/c} \def\mevcc{MeV/c^2} \def\gevc{GeV/c} \def\gevcc{GeV/c^2} \author{ {Marcin Chrzaszcz} (CERN)} \institute{UZH} \title[Review of $B \to K_s \pi^+ \pi^-$ ]{Review of $B \to K_s \pi^+ \pi^-$ } \date{25 September 2014} \begin{document} \tikzstyle{every picture}+=[remember picture] { \setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} \begin{frame}[c]%{\phantom{title page}} \begin{center} \begin{center} \begin{columns} \begin{column}{0.75\textwidth} \flushright \bfseries \Large {Anatomy of the decay $\PBzero \to \PKshort \Ppi^+ \Ppi^- $ and first observation of the $CP$ asymmetry in the transition $\APBzero \to \PKstar^- \Ppi^+$} \end{column} \begin{column}{0.02\textwidth} {~} \end{column} \begin{column}{0.23\textwidth} % \hspace*{-1.cm} \vspace*{-3mm} \includegraphics[width=0.6\textwidth]{lhcb-logo} \end{column} \end{columns} \end{center} \quad \vspace{3em} \begin{columns} \begin{column}{0.44\textwidth} \flushright \vspace{-2.8em} { \fontspec{Zapfino} Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} %\flushright \vspace{-2.8em} { Marcin Chrzaszcz\\\vspace{-0.1em}\small \href{mailto:mchrzasz@cern.ch}{mchrzasz@cern.ch}} \end{column} \begin{column}{0.53\textwidth} \hspace{2.0cm} \includegraphics[height=1.6cm]{cern} \end{column} \end{columns} \vspace{1em} \textcolor{normal text.fg!50!Comment}{LBT meeting, CERN\\October 6, 2017} \end{center} \end{frame} } \begin{frame}{Yellow pages} \vspace{1.5em} \begin{minipage}{\textwidth} \ARROW Proponents: M. Baalouch, E. Ben-Haim, E. Cogneras, T. Gershon, M. Grabalosa, L. Henry, T. Latham, J.M. Maratas, J. McCarthy, D. Milanes, S. Monteil, R. Silva Coutinho, N. Watson\\ \ARROW Reviewers: Stephanie Hansmann-Menzemer (chair), Stefano Gallorini\\ \ARROW EB: Mitesh Patel\\ \ARROW EB readers: Patrick Koppenburg, Simon Eidelman\\ \ARROW Twiki: \href{https://twiki.cern.ch/twiki/bin/viewauth/LHCbPhysics/Dalitz_KSPiPi}{\url{https://twiki.cern.ch/twiki/bin/viewauth/LHCbPhysics/Dalitz_KSPiPi}}\\ \ARROW Jurnal: PRL.\\ \vspace{1cm} \ARROW Deadline for comments: $13^{\rm th}$ October.\\ \ARROW Please send me comments before: $12^{\rm th}$ October.\\ \end{minipage} \vspace*{2.cm} \end{frame} \begin{frame}{Physics in the paper} \vspace{1.5em} \begin{minipage}{\textwidth} \begin{columns} \column{0.5\textwidth} \ARROW Looking for new source of CP violation outside the CKM matrix.\\ \ARROW Looking at the transition $b \to s q\bar{q}$, where $q=u,d,s$.\\ \ARROW Rule of thumb: CP violation should be similar to the ones in $b \to s c\bar{c}$.\\ \ARROW The decay $\PBzero \to \PKshort \Ppi^+ \Ppi^- $ has reach resonant structure!!\\ \ARROWR Dalitz analysis. \column{0.5\textwidth} \includegraphics[width=0.9\textwidth]{images/Fig1.png} \end{columns} \ARROW Because of available statistics, the analysis is untagged and time integrated (isobar model): \begin{align*} P(s_+, s_- )= \frac{ \vert A(s_+, s_-) \vert^2 \vert \bar{A}(s_+, s_-) \vert^2 }{\int\int_{\Omega} ( \vert A(s_+, s_-) \vert^2 \vert \bar{A}(s_+, s_-) \vert^2 ) d s_+ ds_-} \end{align*} \end{minipage} \vspace*{2.cm} \end{frame} \begin{frame}{Physics in the paper} \vspace{1.5em} \begin{minipage}{\textwidth} \ARROW The amplitudes are defined: \begin{align*} A = \sum_{j=1}^N c_j F_j(s_+, s_-),~~\bar{A} = \sum_{j=1}^N \bar{c}_j \bar{F}_j(s_+, s_-) \end{align*} \begin{columns} \column{0.65\textwidth} \includegraphics[width=0.9\textwidth]{images/Tab1.png} \column{0.35\textwidth} \begin{align*} A_{CP}= \frac{ \vert \bar{c}_j \vert^2 - \vert c_j \vert^2 }{ \vert \bar{c}_j \vert^2 + \vert c_j \vert^2} \end{align*} \end{columns} \end{minipage} \vspace*{2.cm} \end{frame} \begin{frame}{Experimental elements} \vspace{1.5em} \begin{minipage}{\textwidth} \ARROW Run1 data set! ($3~{\rm fb}^{-1}$).\\ \ARROW Interesting trigger solution: \begin{itemize} \item $\PKshort \to \pi \pi$ can decay outside the VELO. \item Only for the second part of 2012 ($1.4~{\rm fb}^{-1}$) there was an HLT2 line implemented which considered downstream $\PKshort$. \end{itemize} \ARROW BDT for selection.\\ \ARROW Correcting efficiency in Dalitz plane. \end{minipage} \vspace*{2.cm} \end{frame} \begin{frame}{Results} \vspace{1.5em} \begin{minipage}{\textwidth} \ARROW Paper reports:\\ \only<1>{ \begin{align*} \mathcal{F}_j = \frac{\int \int_{\Omega} \vert c_j F_j(s_+, s_-) \vert^2 d s_+ ds_- }{\int \int_{\Omega} \vert \sum_j c_j F_j (s_+, s_-) \vert^2 d s_+ ds_- } \end{align*} \begin{align*} A_{CP}= \frac{ \vert \bar{c}_j \vert^2 - \vert c_j \vert^2 }{ \vert \bar{c}_j \vert^2 + \vert c_j \vert^2} \end{align*} } \only<2>{ \begin{center} \includegraphics[width=0.8\textwidth]{images/Fig2.png} \end{center} } \only<3>{ \begin{center} \includegraphics[width=0.8\textwidth]{images/Fig3.png} \end{center} \ARROW The result is $6.8(6.0)~\sigma$ away from being zero. (including systematics).\\ \ARROW Reasonable agreement with world average: \begin{align*} A_{CP} (\PKstar^{\pm} \pi^{\mp})-0.23 \pm 0.06 \end{align*} } \only<4>{ \begin{center} \includegraphics[width=0.65\textwidth]{images/Fig4.png} \end{center} } \end{minipage} \vspace*{2.cm} \end{frame} \begin{frame}{Systematics} \vspace{1.5em} \begin{minipage}{\textwidth} \ARROW There are two cathegories of systematics: \begin{itemize} \item Experimental. \item Model related. \end{itemize} \ARROW The experimental one were obtained with pseudo experiments.\\ \ARROW Dominant systematics is the efficiency determination!\\ \ARROWR Model related systematics are also evaluated: \begin{itemize} \item Varying each of the parameters of the mean and the width. \item related to marginal $f_2(1270)$ and $f_0(500)$ resonance components. \end{itemize} \end{minipage} \vspace*{2.cm} \end{frame} \begin{frame}{First comments} \vspace{1.5em} \begin{minipage}{\textwidth} \ARROW Overall the analysis seems solid!!\\ \ARROW Some things might be better described in the paper.\\ \ARROW Some physics comments: \begin{itemize} \item Non-resonant modelling. \item Over estimation of model systematic. \item \end{itemize} \ARROW Paper is to long: $3803$ words (PRL : $3750$).\\ \end{minipage} \vspace*{2.cm} \end{frame} \backupbegin \begin{frame}\frametitle{Backup} \topline \end{frame} \backupend \end{document}