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Presentations / Kstmumu / Answers_to_questions_v3 / group_meeting.tex
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% see the macros.tex file for definitions
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% title slide definition
\title{Answers to questions raised by conveners on EW penguin, Vol3.}
%\subtitle{a bias report}
\author{ Marcin Chrz\k{a}szcz$^{1,2}$ ,  Nicola Serra$^{1}$ }
\institute[UTH, IFJ]
{
 %\begin{tiny}
$ ^1$ University of Zurich , $ ^2$ Institute of Nuclear Physics, Krakow,  
 %\end{tiny}smallsmall
}
  

\date{ \begin{small} \today \end{small}}

%--------------------------------------------------------------------
%                           Introduction
%--------------------------------------------------------------------

\begin{document}




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%--------------------------------------------------------------------
%                          OUTLINE
%--------------------------------------------------------------------




%\section[Outline]{}
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%-------------------------------------------------------------------
%                          Introduction
%-------------------------------------------------------------------
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\title{Update on analysis}


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\begin{frame}\frametitle{Lets make calculations really slowly}
\only<1>{
Let's take just the stripping line(this is incomplete because of the the offline cuts)($\PJpsi$ veto is applied everywhere):
\begin{itemize}
\item total: 10835
\item dimuon\footnote{mu1ID==13 and mu2ID==13}: 9085
\item efficiency: 83\%
\end{itemize}


}
\only<2>
{
Immediately after stripping we have the following cuts: piminusisMuon=0 KplusisMuon=0  KplusPIDK>-5 piminusPIDK<25
\begin{itemize}
\item total: 4708
\item dimuon\footnote{mu1ID=13 and mu2ID=13}: 4333
\item efficiency: 92\%
\end{itemize}
}

\only<3>
{
then we discovered that muID==0 are still muons: MU1ID=0 or Mu2ID=0(reminder we have Jpsi veto!):\\
  \includegraphics[scale=0.2 ]{ghost.png}
}
\only<4>
{
So we require that muons have some real truth matched ID different form zero:
\begin{itemize}
\item total: 4547
\item dimuon\footnote{mu1ID=13 and mu2ID=13}: 4333
\item efficiency: 95.3\%
\end{itemize}
Cross check: 161(ghots events, see plot) +  4547 = 4708(no ghost cut). All consistent!




}
\only<5>
{
Then we play with PID cuts. Putting a cut grater then 5(3). With this cuts:
\begin{itemize}
\item total: 1956
\item dimuon\footnote{mu1ID=13 and mu2ID=13}: 1939
\item efficiency: 99\% (97,4\%)
\end{itemize}
}
\only<6>
{
Why do ghosts change so much and why are they harmless:
\begin{itemize}
\item As Mitesh wanted I am VETOing $\PJpsi$. 
\item Of coz we have a lot of those. 
\item Is turns out that the ghost ratio is $0.5\%$.
\item Even $0.5\%$ from 13879 $\PJpsi$ makes a difference cuz they are treated as non-muon bck.
\end{itemize}
Please note that $161/4547$ is not the ghost rate. 

}



	\textref {M.Chrz\k{a}szcz, N.Serra 2013}

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\begin{Huge}
SPARES
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	\textref {M.Chrz\k{a}szcz, N.Serra 2013}

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After the pure stripping we are applying:
\begin{enumerate}
\item Kismuon=0 and piismuon=0
\item KpidK>5 and piPIDK<25
\end{enumerate}
Starting from 10835 applying following number of events remain:
\begin{enumerate}
\item 8833
\item 5662
\end{enumerate}


	\textref {M.Chrz\k{a}szcz, N.Serra 2013}

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