\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[absolute,overlay]{textpos} \usepackage{amsmath} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{bm} \usepackage{colortbl} \usepackage{mathrsfs} % For Weinberg-esque letters \usepackage{cancel} % For "SUSY-breaking" symbol \usepackage{slashed} % for slashed characters in math mode \usepackage{bbm} % for \mathbbm{1} (unit matrix) \usepackage{amsthm} % For theorem environment \usepackage{multirow} % For multi row cells in table \usepackage{arydshln} % For dashed lines in arrays and tables \usepackage{siunitx} \usepackage{xhfill} \usepackage{grffile} \usepackage{textpos} \usepackage{subfigure} \usepackage{tikz} %\usepackage{hepparticles} \usepackage[italic]{hepparticles} \usepackage{hepnicenames} % Drawing a line \tikzstyle{lw} = [line width=20pt] \newcommand{\topline}{% \tikz[remember picture,overlay] {% \draw[crimsonred] ([yshift=-23.5pt]current page.north west) -- ([yshift=-23.5pt,xshift=\paperwidth]current page.north west);}} % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % % \usepackage{tikzfeynman} % For Feynman diagrams \usetikzlibrary{arrows,shapes} \usetikzlibrary{trees} \usetikzlibrary{matrix,arrows} % For commutative diagram % http://www.felixl.de/commu.pdf \usetikzlibrary{positioning} % For "above of=" commands \usetikzlibrary{calc,through} % For coordinates \usetikzlibrary{decorations.pathreplacing} % For curly braces % http://www.math.ucla.edu/~getreuer/tikz.html \usepackage{pgffor} % For repeating patterns \usetikzlibrary{decorations.pathmorphing} % For Feynman Diagrams \usetikzlibrary{decorations.markings} \tikzset{ % >=stealth', %% Uncomment for more conventional arrows vector/.style={decorate, decoration={snake}, draw}, provector/.style={decorate, decoration={snake,amplitude=2.5pt}, draw}, antivector/.style={decorate, decoration={snake,amplitude=-2.5pt}, draw}, fermion/.style={draw=gray, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=gray]{>}}}}, fermionbar/.style={draw=gray, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=gray]{<}}}}, fermionnoarrow/.style={draw=gray}, gluon/.style={decorate, draw=black, decoration={coil,amplitude=4pt, segment length=5pt}}, scalar/.style={dashed,draw=black, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, scalarbar/.style={dashed,draw=black, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=black]{<}}}}, scalarnoarrow/.style={dashed,draw=black}, electron/.style={draw=black, postaction={decorate}, decoration={markings,mark=at position .55 with {\arrow[draw=black]{>}}}}, bigvector/.style={decorate, decoration={snake,amplitude=4pt}, draw}, } % TIKZ - for block diagrams, % from http://www.texample.net/tikz/examples/control-system-principles/ % \usetikzlibrary{shapes,arrows} \tikzstyle{block} = [draw, rectangle, minimum height=3em, minimum width=6em] \usetikzlibrary{backgrounds} \usetikzlibrary{mindmap,trees} % For mind map \newcommand{\degree}{\ensuremath{^\circ}} \newcommand{\E}{\mathrm{E}} \newcommand{\Var}{\mathrm{Var}} \newcommand{\Cov}{\mathrm{Cov}} \newcommand\Ts{\rule{0pt}{2.6ex}} % Top strut \newcommand\Bs{\rule[-1.2ex]{0pt}{0pt}} % Bottom strut \graphicspath{{images/}} % Put all images in this directory. Avoids clutter. % SOME COMMANDS THAT I FIND HANDY % \renewcommand{\tilde}{\widetilde} % dinky tildes look silly, dosn't work with fontspec \newcommand{\comment}[1]{\textcolor{comment}{\footnotesize{#1}\normalsize}} % comment mild \newcommand{\Comment}[1]{\textcolor{Comment}{\footnotesize{#1}\normalsize}} % comment bold \newcommand{\COMMENT}[1]{\textcolor{COMMENT}{\footnotesize{#1}\normalsize}} % comment crazy bold \newcommand{\Alert}[1]{\textcolor{Alert}{#1}} % louder alert \newcommand{\ALERT}[1]{\textcolor{ALERT}{#1}} % loudest alert %% "\alert" is already a beamer pre-defined \newcommand*{\Scale}[2][4]{\scalebox{#1}{$#2$}}% \def\Put(#1,#2)#3{\leavevmode\makebox(0,0){\put(#1,#2){#3}}} \usepackage{gmp} \usepackage[final]{feynmp-auto} \usepackage[backend=bibtex,style=numeric-comp,firstinits=true]{biblatex} \bibliography{bib} \setbeamertemplate{bibliography item}[text] \makeatletter\let\frametextheight\beamer@frametextheight\makeatother % suppress frame numbering for backup slides % you always need the appendix for this! \newcommand{\backupbegin}{ \newcounter{framenumberappendix} \setcounter{framenumberappendix}{\value{framenumber}} } \newcommand{\backupend}{ \addtocounter{framenumberappendix}{-\value{framenumber}} \addtocounter{framenumber}{\value{framenumberappendix}} } \definecolor{links}{HTML}{2A1B81} %\hypersetup{colorlinks,linkcolor=,urlcolor=links} % For shapo's formulas: \def\lsi{\raise0.3ex\hbox{$<$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} \def\gsi{\raise0.3ex\hbox{$>$\kern-0.75em\raise-1.1ex\hbox{$\sim$}}} \newcommand{\lsim}{\mathop{\lsi}} \newcommand{\gsim}{\mathop{\gsi}} \newcommand{\wt}{\widetilde} %\newcommand{\ol}{\overline} \newcommand{\Tr}{\rm{Tr}} \newcommand{\tr}{\rm{tr}} \newcommand{\eqn}[1]{&\hspace{-0.7em}#1\hspace{-0.7em}&} \newcommand{\vev}[1]{\rm{$\langle #1 \rangle$}} \newcommand{\abs}[1]{\rm{$\left| #1 \right|$}} \newcommand{\eV}{\rm{eV}} \newcommand{\keV}{\rm{keV}} \newcommand{\GeV}{\rm{GeV}} \newcommand{\MeV}{\rm{MeV}} \newcommand{\im}{\rm{Im}} \newcommand{\re}{{\rm Re}} \newcommand{\invfb}{\rm{fb^{-1}}} \newcommand{\fixme}{\rm{{\color{red}{FIXME!}}}} \newcommand{\thetal}{\theta_l} \newcommand{\thetak}{\theta_k} \newcommand{\nn}{\nonumber} \newcommand{\eq}[1]{\begin{equation} #1 \end{equation}} %\newcommand{\eqn}[1]{\begin{displaymath} #1 \end{displaymath}} \newcommand{\eqa}[1]{\begin{eqnarray} #1 \end{eqnarray}} \newcommand{\apeL}{{A_\perp^L}} \newcommand{\apeR}{{A_\perp^R}} \newcommand{\apeLR}{{A_\perp^{L,R}}} \newcommand{\apaL}{{A_\|^L}} \newcommand{\apaR}{{A_\|^R}} \newcommand{\apaLR}{{A_\|^{L,R}}} \newcommand{\azeL}{{A_0^L}} \newcommand{\azeR}{{A_0^R}} \newcommand{\azeLR}{{A_0^{L,R}}} \newcommand{\Real}{\ensuremath{\mathcal{R}e}\xspace} \newcommand{\Imag}{\ensuremath{\mathcal{I}m}\xspace} \renewcommand{\C}[1]{{\cal C}_{#1}} \newcommand{\Ceff}[1]{{\cal C}^{\rm eff}_{#1}} \newcommand{\Cpeff}[1]{{\cal C}^{\rm eff\prime}_{#1}} \newcommand{\Cp}[1]{{\cal C}^{\prime}_{#1}} \def\FL {\ensuremath{F_{\mathrm{L}}}\xspace} \def\ATDPH {\ensuremath{A_{\mathrm{T,PR}}^{(2)}}\xspace} \def\ATImPH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Im}}}\xspace} \def\ATRePH {\ensuremath{A_{\mathrm{T,PR}}^{\mathrm{Re}}}\xspace} \def\FLPH {\ensuremath{F_{\mathrm{L,PR}}}\xspace} \def\ATDKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{(2)}}\xspace} \def\ATImKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Im}}}\xspace} \def\ATReKG {\ensuremath{A_{\mathrm{T,\Kstarz \gamma}}^{\mathrm{Re}}}\xspace} \def\FLKG {\ensuremath{F_{\mathrm{L,\Kstarz \gamma}}}\xspace} \def\ATD {\ensuremath{A_{\mathrm{T}}^{(2)}}\xspace} \def\ATIm {\ensuremath{A_{\mathrm{T}}^{\mathrm{Im}}}\xspace} \def\ATRe {\ensuremath{A_{\mathrm{T}}^{\mathrm{Re}}}\xspace} \def\cgreen{\color{green}} \definecolor{green}{rgb}{0.2,0.6,0.2} \newcommand{\disp}{\displaystyle} \def\be{\begin{equation}} \def\ee{\end{equation}} \def\ba{\begin{eqnarray}} \def\ea{\end{eqnarray}} \def\d{\partial} \def\l{\left(} \def\r{\right)} \def\la{\langle} \def\ra{\rangle} \def\e{{\rm e}} \def\Br{{\rm Br}} \def\ARROW{{\color{JungleGreen}{$\Rrightarrow$}}\xspace} \newcommand\textref[1]{% \begin{textblock*}{\paperwidth}(0pt,0.025\textheight) \raggedleft \small{{\color{RoyalBlue} \emph{#1}}}\hspace{1.5em} \end{textblock*}} \newcommand\textahref[2]{% \begin{textblock*}{\paperwidth}(0pt,0.025\textheight) \raggedleft \small{\emph{\href{#1}{#2} }}\hspace{1.5em} \end{textblock*}} \author{ {M.Chrzaszcz} (CERN)} \institute{UZH} \title[Rare decays in the beauty, charm and strange sector]{Rare decays in the beauty, charm and strange sector} \date{28 March 2018} \begin{document} \tikzstyle{every picture}+=[remember picture] { \setbeamertemplate{sidebar right}{\llap{\includegraphics[width=\paperwidth,height=\paperheight]{bubble2}}} \begin{frame}[c]%{\phantom{title page}} \begin{center} \begin{center} \begin{columns} \begin{column}{0.75\textwidth} \flushright\bfseries \Huge {Rare decays in the beauty, charm and strange sector} \end{column} \begin{column}{0.02\textwidth} {~} \end{column} \begin{column}{0.23\textwidth} % \hspace*{-1.cm} \vspace*{-3mm} \includegraphics[width=0.6\textwidth]{lhcb-logo} \end{column} \end{columns} \end{center} \quad \vspace{3em} \begin{columns} \begin{column}{0.44\textwidth} \flushright \vspace{-1.8em} { \Large Marcin Chrzaszcz\\\vspace{-0.1em} \vspace{-0.1em} } \end{column} \begin{column}{0.53\textwidth} \includegraphics[height=1.3cm]{cern} \end{column} \end{columns} \vspace{0.2em} \vspace{1em} \vspace{0.5em} \textcolor{normal text.fg!50!Comment}{FPCP, Hyderabad\\14-18 July 2018 } \end{center} \end{frame} } \begin{frame}{Outline} FIXME \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}\frametitle{Why rare decays?} \begin{columns} \column{4in} \begin{itemize} \item In the SM allows only the charged interactions to change flavour. \begin{itemize} \item Other interactions are flavour conserving. \end{itemize} \item One can escape this constrain and produce $\Pbottom \to \Pstrange$ and $\Pbottom \to \Pdown$ at loop level. \begin{itemize} \item This kind of processes are suppressed in the SM $\to$~Rare decays. \item New Physics can enter in the loops. \end{itemize} \end{itemize} \begin{center} \includegraphics[scale=0.3]{images/lupa.png} \includegraphics[scale=0.3]{images/example.png} \end{center} \column{1.5in} \includegraphics[width=0.61\textwidth]{images/couplings.png} \end{columns} \end{frame} \begin{frame} \only<1>{\frametitle{LHCb detector - tracking} \begin{columns} \column{3in} \includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} \column{2in} \includegraphics[width=0.95\textwidth]{images/sketch.png} \end{columns} \begin{itemize} \item Excellent Impact Parameter (IP) resolution ($20~\rm \mu m$).\\ $\Rightarrow$ Identify secondary vertices from heavy flavour decays \item Proper time resolution $\sim~40-50~\rm fs$.\\ $\Rightarrow$ Good separation of primary and secondary vertices. \item Excellent momentum ($\delta p/p \sim 0.5 - 1.0\%$) and inv. mass resolution.\\ $\Rightarrow$ Low combinatorial background. \end{itemize} } \only<2>{\frametitle{LHCb detector - PID} \begin{columns} \column{3in} \includegraphics[width=0.9\textwidth]{images/1050px-Lhcbview.jpg} \column{2in} \includegraphics[width=0.95\textwidth]{images/cher.png} \end{columns} \begin{itemize} \item Excellent Muon identification $\epsilon_{\mu \to \mu} \sim 97\%$, $\epsilon_{\pi \to \mu} \sim 1-3\%$ \item Good $\PK-\Ppi$ separation via RICH detectors, $\epsilon_{\PK \to \PK} \sim 95\%$, $\epsilon_{\Ppi \to \PK} \sim 5\%$.\\ $\Rightarrow$ Reject peaking backgrounds. \item High trigger efficiencies, low momentum thresholds.\\ %Muons: $p_T > 1.76 \GeV/c$ at L0, $p_T > 1.0 \GeV/c$ at HLT1,\\ $B \to \PJpsi X $: Trigger $\sim 90\%$. \end{itemize} } \textref{Int. J. Mod. Phys. A30 (2015) 1530022} \vspace*{2.1cm} \end{frame} \begin{frame}{Rare beauty decays} \begin{columns} \column{0.5\textwidth} \begin{exampleblock}{$\Pbeauty \to \Pstrange \ell \ell$ family} \begin{itemize} \item $\PB \to \PKstar \mu \mu$ \item $\PBs \to \Pphi \mu \mu$ \item $\Lambda_b \to \Pproton \PK \mu \mu$ \item LUV: $R_K$, $R_{\PKstar}$ \end{itemize} \end{exampleblock} {~}\\ \ARROW To many results to be covered in one talk! Please see A.~Campos talk for more! \column{0.5\textwidth} \begin{alertblock}{$\Pbeauty \to \Pstrange \gamma$ family} \begin{itemize} \item $\PB \to \PJpsi \gamma$ \item $\PB \to \PK \Ppi \Ppi \gamma$ \end{itemize} \end{alertblock} \begin{block}{$\Pbeauty \to \Pdown \ell \ell$ family} \begin{itemize} \item $\PB \to \pi \pi \mu \mu$ \item $\APBs \to \PKstar \mu \mu$ \item $\Lambda_b \to \Pproton \pi \mu \mu$ \end{itemize} \end{block} \begin{exampleblock}{Purelly leptonic familly} \begin{itemize} \item $\PB \to \ell \ell$ \item LFV: $\PB \to \ell \ell^{\prime}$ \item LFV in $\tau$ \end{itemize} \end{exampleblock} \end{columns} \end{frame} { \usebackgroundtemplate{\includegraphics[width=\paperwidth,height=\paperheight]{images/familie.jpg}} \begin{frame}[plain] \end{frame} } %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%5 \begin{frame}{$\Lambda_b \to \Lambda \mu \mu$} \begin{columns} \column{0.01\textwidth} {~} \column{0.4\textwidth} \ARROW $\Pbeauty \to \Pstrange \mu \mu$ in baryon sector. \\ \ARROW Because of spin $1/2$ nature of the baryon there the system has to be described by 5 angles:~\href{https://arxiv.org/pdf/1710.00746.pdf}{{\color{blue}1710.00746}}\\ \ARROW Impossible to perform a likelihood fit. Need to use moments: \begin{align*} M_i = \frac{3}{32\pi^2} \int \sum_{i=1}^{34} K_i(q^2) f(\overrightarrow{\Omega}) d\overrightarrow{\Omega} \end{align*} \column{0.6\textwidth} \includegraphics[width=0.99\textwidth]{{images/angular_basis.pdf}} ~~\ARROW In total we have 34 observables! \end{columns} \textref{LHCb-PAPER-2018-029} \end{frame} \begin{frame}{$\Lambda_b \to \Lambda \mu \mu$} \begin{columns} \column{0.01\textwidth} {~} \column{0.6\textwidth} \ARROW Update with $5~\invfb$.\\ \ARROW 610 events observed in the high $q^2$.\\ \ARROW Angular efficiency modelled in 6D.\\{~}\\ \includegraphics[width=0.99\textwidth]{{images/angles.pdf}} \column{0.4\textwidth} \includegraphics[width=0.99\textwidth]{{images/figure51.pdf}}\\ \ARROW The results:\\{~}\\ \includegraphics[width=0.99\textwidth]{{images/Ki.pdf}}\\ \end{columns} \textref{LHCb-PAPER-2018-029} \end{frame} \begin{frame}{$\APBs \to \PKstar \mu \mu$} \begin{columns} \column{0.01\textwidth} {~} \column{0.6\textwidth} wq \column{0.4\textwidth} qwe \end{columns} \end{frame} \begin{frame}{$\APBs \to \PKstar \mu \mu$} \begin{columns} \column{0.01\textwidth} {~} \column{0.6\textwidth} weq \column{0.4\textwidth} qwe \end{columns} \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}\frametitle{$\PB \to e \mu$} qewqeq \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}\frametitle{$\PB \to e \mu$} qewqeq \end{frame} { \usebackgroundtemplate{\includegraphics[width=\paperwidth,height=\paperheight]{images/charmingpenguing.jpg}} \begin{frame}[plain] \end{frame} } \begin{frame}\frametitle{$\Lambda_c \to \Pproton \mu \mu$} qewqeq \end{frame} \begin{frame}\frametitle{$\Lambda_c \to \Pproton \mu \mu$} qewqeq \end{frame} \begin{frame}\frametitle{$\PD \to h h \mu \mu$} qewqeq \end{frame} \begin{frame}\frametitle{$\PD \to h h \mu \mu$} qewqeq \end{frame} { \usebackgroundtemplate{\includegraphics[width=\paperwidth,height=\paperheight]{images/strange.jpg}} \begin{frame}[plain] \end{frame} } \begin{frame}\frametitle{$\PKshort \to \mu \mu$} qewqeq \end{frame} \begin{frame}\frametitle{$\PKshort \to \mu \mu$} qewqeq \end{frame} \begin{frame}\frametitle{$\Sigma \to \Pproton \mu \mu$} qewqeq \end{frame} \begin{frame}\frametitle{$\Sigma \to \Pproton \mu \mu$} qewqeq \end{frame} \backupbegin \begin{frame}\frametitle{Backup} \topline \end{frame} \backupend \end{document}