\documentclass{beamer}
\usepackage{pgf}
\usepackage{times}
\usepackage[T1]{fontenc}
%\usepackage[mathscr]{eucal}
%\usepackage{mathptmx}
%\usepackage{mathrsfs}
\usepackage{hyperref}
% \usepackage{pgfpagfes}
% \setbeameroption{show notes on second screen}
%\pgfpagesuselayout{4 on 1}[a4paper,border shrink=5mm,landscape]
\usepackage{xcolor}
%\usepackage[dvipsnames]{xcolor}
%\usepackage{amsfonts}
%\usepackage{amsmath}
% \usepackage[amssymb]{SIunits}
%\usepackage{natbib}
%\usepackage{amssymb}
\usepackage{hepparticles}
\usepackage{hepnicenames}
\usepackage{hepunits}
\usepackage{tikz}
\usepackage[polish]{babel}
%\usepackage{lmodern}
\usepackage{feynmp}
% suppress navigation bar
\beamertemplatenavigationsymbolsempty
\usepackage[mathscr]{eucal}
\usepackage{mathrsfs}
\mode<presentation>
{
  \usetheme{bunsen}
  \setbeamercovered{transparent}
  \setbeamertemplate{items}[circle]
}

% set fonts
\usepackage{amsfonts}
\usepackage{amsmath}
\usepackage{verbatim}

\usetikzlibrary{arrows}
\usetikzlibrary{shapes}

%\usepackage{gfsartemisia-euler}
%\usepackage[T1]{fontenc}
\setbeamerfont{frametitle}{size=\LARGE,series=\bfseries}
\tikzstyle{decision} = [diamond, draw, fill=gray!20, 
    text width=4.5em, text badly centered, node distance=3cm, inner sep=0pt]
\tikzstyle{block} = [rectangle, draw, fill=blue!10, 
    text width=5em, text centered, rounded corners, minimum height=2em]
\tikzstyle{line} = [draw, -latex']
\tikzstyle{cloud} = [draw, ellipse,fill=red!10, node distance=3cm,
    minimum height=2em]

\tikzstyle{every picture}+=[remember picture]


\renewcommand{\PKs}{{\HepParticle{K}{S}{}\xspace}}
% color definitions
\usepackage{color}
\definecolor{uipoppy}{RGB}{225, 64, 5}
\definecolor{uipaleblue}{RGB}{96,123,139}
\definecolor{uiblack}{RGB}{0, 0, 0}

% caption styling
%\DeclareCaptionFont{uiblack}{\color{uiblack}}
%\DeclareCaptionFont{uipoppy}{\color{uipoppy}}
%\captionsetup{labelfont={uipoppy},textfont=uiblack}

% see the macros.tex file for definitions
\include{macros}

% title slide definition
\title{The SuperB factory}  
\subtitle{physics prospects and project status}
\author{Marcin Chrz\k{a}szcz}
\institute[Institute of Nuclear Physics]
{
Institute of Nuclear Physics,
\newline Polish Academy of Science,
\newline on behave of SuperB collaboration
}


\date{$21^{st}$ September $2012$} 

 

\begin{document}


\setbeamertemplate{background}
{\includegraphics[width=\paperwidth,height=\paperheight]{frontpage_bg_mine}}
\setbeamertemplate{footline}[default]

\begin{frame}
\vspace{1.5cm}
\begin{columns}
\column{2.75in}
  \titlepage
  \vspace{0.8cm}
  \begin{center}
    \includegraphics[height=1.0cm,keepaspectratio ]{pic/ifj.png}
   \hspace{1cm}
  \includegraphics[height=1.0cm]{pic/SuperB_logo.png}
   \end{center}
  \vspace{10cm}
\column{2.0in}
\end{columns}
\end{frame}



%tutaj mamy pierwsza strone


\section[Outline]{}
\begin{frame}
\tableofcontents
\end{frame}
\setbeamertemplate{background}
 {\includegraphics[width=\paperwidth,height=\paperheight]{slide_bg}}
\setbeamertemplate{footline}[bunsentheme]

%normal slides
\section{Introduction}


\begin{frame}\frametitle{B factories}

B factories achived a great success over the dozen years. A natural continuation of this project are Super Flavor Factories.
\begin{exampleblock}{Super Flavor Factories} \begin{enumerate}
\item Data $75 ab^{-1}$.
\item Luminosity $10^{36} cm^{-2} s^{-1} $.
\item Flexibility to run on charm threshold with luminosity $10^{35} cm^{-2} s^{-1} $. 
\item Logitudanal polarization of electron beam $80 \% $.
\item Upgradet Babar detector.
\item Start of data taking: 2018.
\item $10ab^{-1}$ peer year.

\end{enumerate}we have in 200 metres 3 shops selling tissot

\end{exampleblock}

\end{frame}

\section{SuperB Infrasctructure}


\subsection{Accelerator}
\begin{frame}\frametitle{TorVegata Site}

\vspace{0.8cm}
\includegraphics[scale=0.35]{pic/tor_veggata_site.png}



\end{frame}


%\subsection{Accelerator}
\begin{frame}\frametitle{TorVegata Site}

\vspace{0.7cm}
\includegraphics[scale=0.35]{pic/acc.png}



\end{frame}

\subsection{Luminosity}
\begin{frame}\frametitle{Quest for Luminosity}

\begin{columns}[c]

	\column{3.0in}
	\includegraphics[scale=0.4]{pic/crab_off.png}

	\column{1.5in}
	
	$L \propto \dfrac{1}{\sqrt{\beta}_{y}}$, $  \Phi \approx \dfrac{\sigma_{z}}{\sigma_{x}} \dfrac{\theta}{2}$ 	
	
	
	\end{columns}
		
	
	

\end{frame}
\begin{frame}\frametitle{Quest for Luminosity}
\vspace{1cm}
\begin{columns}[c]

	\column{3.0in}
	\includegraphics[scale=0.4]{pic/crab_on.png}

	\column{1.5in}
	
	$L \propto \dfrac{1}{\sqrt{\beta}_{y}}$, $  \Phi \approx \dfrac{\sigma_{z}}{\sigma_{x}} \dfrac{\theta}{2}$ 	
	
	\end{columns}
		
	
	

\end{frame}

\section{Detector}
\begin{frame}\frametitle{Recycling, Babar}

\vspace{0.5cm}
\includegraphics[scale=7]{pic/det.jpg}


\end{frame}


\subsection{SVT}

\begin{frame}\frametitle{Silicon Vertex Tracker}

\vspace{0.5cm}
	\includegraphics[scale=0.15]{pic/svt2.png}

\begin{columns}[c]
	\column{3in}

	\begin{itemize}
	\item Five layers(1-5) of double-sided silicon strip detectors.
	\item Radial span $3-15~{\rm cm}$.
	\item Upgrade the electronics for faster readout.
	\item Additional Layer 0:
	\begin{enumerate}
\footnotesize	\item Radius $\approx 1.5 cm$ .
\footnotesize   \item Low material budget: $X_{0}=0.5\%$.
\footnotesize	\item Two possible technologies: Hybrid Pixels, Double Sided Strip detectors(Striplets).
	\end{enumerate}
		\end{itemize}	

		
	%first column	
	\column{2in}
	\newline \includegraphics[scale=0.23]{pic/svtb.png}
		
	%second column	
\end{columns}


\end{frame}







\subsection{DCH}
\begin{frame}\frametitle{Drift Chamber}

\vspace{0.5cm}
\begin{columns}[c]
	\column{3in}
	\includegraphics[scale=0.15]{pic/dich.png}

	\begin{itemize}
	\item 40 layers of $\approx 1 cm$ cells parralel to beam line.
	\item Provide momentum and $\dfrac{dE}{dx}$ for low momentum particles($p<700 MeV$).
	\item $\approx 10000$ channels
	\item Ocuupancy($3.5 \% - 5\%$).

		\end{itemize}	

		
	%first column	
	\column{2in}
	R\&D:
	\begin{itemize}
	\item Geometry
	\item Gas mixture
	\item aaaa
	\end{itemize}
		
	%second column	
\end{columns}


\end{frame}


\subsection{DIRC}
\begin{frame}\frametitle{ {\Large Detector of Internally Reflected Cherenkov light}}


\begin{columns}[c]
	\column{2in}
	\includegraphics[scale=0.23]{pic/DIRC.png}
\newline	\includegraphics[scale=0.23]{pic/dirc2.png}

		
	%first column	
	\column{3in}
	
	\begin{itemize}
	\item Momentum range $ 0.7 - 4 GeV$
	\item Radiator: synthetic fused silica.
	\item Photon detectors outside field region.
	\item Radiatoin hard.
		
	\end{itemize}		
		
	%second column	
\end{columns}


\end{frame}


\subsection{EMC and IFR}
\begin{frame}\frametitle{{ \Large Electromagnetic and hadronic calorimeter}}


\begin{columns}[c]
	\column{3in}
	\includegraphics[scale=0.23]{pic/ifr.png}


		
	%first column	
	\column{2in}
	Electronamgnetic Calorimeter:
	\begin{itemize}
	\item Coverage $94\% of 4 \Pi$
	\item CsI or LYSO cristals
	\item Crystal lenght $16-17.5 X_{0}$ 
	\item Radiatoin hard.
	\end{itemize}		
	Instrumented Flux Return:
	\begin{itemize}
	\item Upgrade form TDC to BIRO
	\item Scintilators
	\item Iron reused from Babar
	\item SiPM
	\end{itemize}		
	%second column	
\end{columns}


\end{frame}


%%%%%%%%%%% uFFFFFFFFFFFFFFFFFfff detector  finished


\section{Physics}

\subsection{Rare B Physics}
\begin{frame}\frametitle{$B \rightarrow \tau \nu$}
\vspace{0.5cm}
\hspace{0.7cm}
\begin{columns}[c]
\column{3.8in}
\hspace{0.7cm}{
%\hspace{0.3cm}}
Precise SM prediction:
\small \newline $Br(B \rightarrow l \nu) = \dfrac{G^{2}_{F} m_{B}}{8\pi} m_{l}^{2} (1-\dfrac{m_{l}^{2}}{m_{B}^{2}})f_{B}^{2}\vert V_{ub}\vert^{2} \tau_{B}$
\newline In SUSY:
\small \newline $Br(B \rightarrow l \nu) = \dfrac{G^{2}_{F} m_{B}}{8\pi} m_{l}^{2} (1-\dfrac{m_{l}^{2}}{m_{B}^{2}})f_{B}^{2}\vert V_{ub}\vert^{2} \tau_{B}(1-\dfrac{tan^{2}\beta}{1+\overline{\epsilon} tan \beta}\dfrac{m_{B}^{2}}{m_{H}^{2}})$
}
\center \includegraphics[scale=0.16]{pic/excl.png}


\column{1.5in}
\includegraphics[scale=0.2]{pic/b2taunu.png}
\newline \includegraphics[scale=0.2]{pic/higggs.png}
\end{columns}


\end{frame}

\subsection{TDCP}
\begin{frame}\frametitle{Time Depended CP}

Time Depended CP can be signs of new physics. One has to study set of modes:
\newline $b \rightarrow s\overline{s}c$, $b \rightarrow s$

Curent experimental results(SM -observed):
\newline $\Delta sin(2\beta)=2.7\sigma$, penguin 
\newline $\Delta sin(2\beta)=2.1\sigma$, tree

Golden modes in SuperB:
$B \rightarrow J/\psi K^{0}$, $B \rightarrow \eta ' K^{0}$, $B \rightarrow f_{0}K_{s}^{0}$
\begin{columns}[c]
\column{3.0in}
\includegraphics[scale=0.17]{pic/table.png}
\column{2.0in}
\includegraphics[scale=0.12]{pic/jpsi.png}
\newline
\newline \includegraphics[scale=0.12]{pic/jpsi2.png}
\end{columns}
\end{frame}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\subsection{$B \rightarrow X_{s} \gamma$}
\begin{frame}\frametitle{$B \rightarrow X_{s} \gamma$}
\vspace{0.5cm}
Very important probe of new physics! Current experimental result averaged out:
$Br(B \rightarrow X_{s} \gamma ) = (3.52\pm0.23\pm0.09) 10^{-4} $

Theoretical calculations on NNLO:

$Br(B \rightarrow X_{s} \gamma ) = (3.15 \pm 0.23) 10^{-4}$

Experimently chalenging to measure the inclusive decays. THere are two ways of studing this decay:
\begin{enumerate}
\item Exlusive:
\begin{itemize}

 \item The earliest results were done suing a large number of exclusive decays, which are fully reconstructed. 
\item Erros rising from unseen modes. 
\item Obsolete for SuperB.

\end{itemize}
\item Inclusive:
\begin{itemize}
\item Use tagging to tag the other B. 
\item No requirements on $X_{s}$.
\item Disadvantage: Cut on photon energy.
\item Effort to keep the cut as small as possible

\end{itemize}
\end{enumerate}


\end{frame}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\subsection{LFV}
\begin{frame}\frametitle{LFV}
\begin{itemize}
\item LFV can occure in SM due to masses of the neutrinos.
\item Any observation is evidence of new physics.
\item Most promising channels: $\tau \rightarrow l \gamma $, $\tau \rightarrow l l l$.
\newline
\includegraphics[scale=0.33]{pic/tau3mu_SUSY_r_violating-eps-converted-to.pdf}
\includegraphics[scale=0.33]{pic/tau3mu_littlest_higgs-eps-converted-to.pdf}
\includegraphics[scale=0.33]{pic/tau3mu_SUSY_seesaw-eps-converted-to.pdf}
\newline \includegraphics[scale=0.33]{pic/tau3mu_SUSY_seesaw-eps-converted-to.pdf}
\includegraphics[scale=0.33]{pic/tau3mu_SM2-eps-converted-to.pdf}
\includegraphics[scale=0.33]{pic/tau3mu_SM-eps-converted-to.pdf}

\end{itemize}
\end{frame}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%

\begin{frame}\frametitle{$\tau \rightarrow l \gamma$ sensitivity}


\begin{columns}[c]
\column{2.5in}

\begin{itemize}
\item Better tracking resolution, increase $\Delta m - \Delta E $ box, by $65\%$.
\item Higher photon efficiency.
\item Increase of geometry acceprance.
\item Thicker signal peak.
\item Smaller boost improves performance of the fit.
\end{itemize}
\column{2.5in}

\includegraphics[scale=0.2]{pic/dm_de.png}

\end{columns}

\end{frame}





\begin{frame}\frametitle{Polarization}
\vspace{0.5cm} 
\begin{columns}[c]
\column{2.6in}


{~}

\begin{enumerate}
       \item SuperB will have polarized electron beam($80\%$). \\
       \item One can use this infromation in serching for NP. \\
	   \item Preliminary results:
	\end{enumerate}    
\begin{itemize}
\item Upper limit at $90\%$: $2.44\times10^{-9}$
\item $3 \sigma$ observation:  $5.50\times 10^{-9}$
\end{itemize}
\column{2.4in}

\includegraphics[scale=0.23]{pic/polar.png}

\end{columns}

\end{frame}


\begin{frame}\frametitle{$\tau \rightarrow 3\mu$}
\begin{columns}[c]
\column{2.0in}
Current analysis:
\begin{itemize}
\item Calculate the trust axis.
\item Semi tag the second $ \tau $. 
\item Limit obtained($90\%$ Br($\tau \rightarrow 3\mu$) = $8.1 \times 10^{-10}$
\end{itemize}
\column{3.0in}
\includegraphics[scale=0.23]{pic/dm_de23mu.png}
\end{columns}
\end{frame}



\begin{frame}\frametitle{LFV Summary}
%!!!!!!!!!!!!!!!!!!!!!!
\includegraphics[scale=0.4]{pic/lfv_superb.png}

\end{frame}




\subsection{CP violation}
\begin{frame}\frametitle{CP violation}
\begin{itemize}
\item CP violation was never observed in $\tau$ sector. 
\item SM prediction is neglible small $O(10^{-12})l$ in $\tau^{\pm} \rightarrow K^{pm} \pi^{0} \nu$. 
\item Any obserwation is clear identification of NP.
\item Very fiew NP models can explain this:
\begin{enumerate}
\item RPV SUSY
\item Multi Higgs models
\end{enumerate}
\item SuperB can improve sensitivety 75 times compared to CLEO.
\end{itemize}

\end{frame}


\subsection{EDM}
\begin{frame}\frametitle{EDM}


EDM can be measured with single angle differential cross section $e^{+}e^{-} \rightarrow \tau^{+} \tau^{-}$.
\begin{itemize}
\item Improvement using polarized beam.
\item Achivable sensitivety: $10^{-19} ecm$

\end{itemize}


\end{frame}










\end{document}
