FCCee_MDI_Oct10.tex

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\title[ CLIC-inspired detector for FCC-ee \hspace{13.5em}\insertframenumber/
\inserttotalframenumber]{ Tracking and single particle performance with the CLIC-inspired detector for FCC-ee }


	\author[Oleksandr Viazlo, Emilia Leogrande]{Oleksandr Viazlo, Emilia Leogrande \\ 
% 	{\small ???}
	}
	\institute{\small CERN\\} 
	
       
	\date{10 October 2017}

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%*****************************************************************************
\begin{frame}{\large \large Introduction}
 
 \begin{itemize}
  \item ???
 \end{itemize}

 
\end{frame}
%*****************************************************************************



%*****************************************************************************
\begin{frame}{\large \large FCC-ee detector model}
 
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      \begin{itemize}
	\item Update on detector model (FCCee$\_$o5$\_$v04). Implementation of carbon support structures in the VTX and Tracker.
      \end{itemize}
    \end{minipage}
};


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%     \begin{minipage}{0.5\textwidth}
% 
%     \resizebox{\columnwidth}{!}{%
%       \begin{tabular}{lccc}
% 	 & CLIC & & FCC-ee \\[0.18cm]
% 	VTX Barrel & 31-60 mm & $\Longrightarrow$ & 17-59 mm \\[0.18cm]
% 	VTX Endcap & Spirals & $\Longrightarrow$ & Disks \\[0.18cm]
% 	Tracker Radius & 1486 mm & $\Longrightarrow$ & 2100 mm \\[0.18cm]
%       \end{tabular}%
%     }
%     \end{minipage}
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%   
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%     \begin{minipage}{0.54\textwidth}
% 
%     \resizebox{\columnwidth}{!}{%
%       \begin{tabular}{lccc}
% 	 & CLIC & & FCC-ee \\[0.18cm]
% 	ECAL thickness & 202 mm & $\Longrightarrow$ & 202 mm \\[0.18cm]
% 	HCAL thickness & 44 $\times$ 7.5 $\lambda_0$ & $\Longrightarrow$ & 44 $\times$ 5.5 $\lambda_0$ \\[0.18cm]
% 	Yoke Thickness & 1989 mm & $\Longrightarrow$ & 1521 mm \\[0.18cm]
%       \end{tabular}%
%     }
%     \end{minipage}
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% 
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%*****************************************************************************
\begin{frame}{\large \large Summary and outlook}
 
 
 
 
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  \begin{minipage}{0.99\textwidth}
 \begin{itemize}
  \item Complete FCC-ee detector model is available for performance studies
  \item Tracking performance was studied with full simulation and reconstruction (truth tracking)
    \end{itemize}
  \end{minipage}
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     \item Conformal tracking performance (single $\mu$ and Z $\to$ uds events) \\[0.3cm]

     \item Effect of increased material budget in VTX \\[0.3cm]
     
     \item Calorimeter studies: 
     \begin{itemize}
      \item complex events - PID efficiency
      \item jet energy resolution
     \end{itemize}
     
     \item Overlay of beam background \\[0.3cm]

%      electron and photon PID efficiencies using the Pandora Particle Flow Algorithm, jets performance
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%*****************************************************************************

%------------------------------------------------
\begin{frame}
\frametitle{BACKUP} 
 
\end{frame}
%------------------------------------------------

%*****************************************************************************
\begin{frame}{\large \large CLIC detector}

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  \begin{itemize}
   \item Full silicon VTX and Tracker: \\ $\geqslant$12 hits per track
   \item W-Si ECAL and Fe-Scint HCAL
   \item Coil is outside of the calorimeter; \\4 Tesla magnetic field
   \item Steel return yoke with 6 RPC muon chambers
  \end{itemize}

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   \item Momentum resolution (at 500 GeV): $\sigma_{\mathrm{p_T}}/ \mathrm{p_T}^2 \simeq 2\cdot10^{-5}$ GeV$^{-1}$
   \item Lepton ID efficiency: $>$ 95$\%$
   \item Impact parameter resolution: \\
	 $\sigma_{d_0} = a \oplus \dfrac{b}{p~sin^{3/2} \theta}$ \\ $a \leqslant $5$ \mu$m, $b \leqslant $15 $\mu$m GeV
   \item Jet energy resolution: \\
	 $\sigma_E / E \simeq $ 3.5 $\%$
 \end{itemize}

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%*****************************************************************************

%*****************************************************************************
\begin{frame}{\large \large FCC-ee detector}
 
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	 & CLIC & & FCC-ee \\[0.18cm]
	VTX Barrel & 31-60 mm & $\Longrightarrow$ & 17-59 mm \\[0.18cm]
	VTX Endcap & Spirals & $\Longrightarrow$ & Disks \\[0.18cm]
	Tracker radius & 1486 mm & $\Longrightarrow$ & 2100 mm \\[0.18cm]
% 	ECAL thickness & 202 mm & $\Longrightarrow$ & 202 mm \\[0.18cm]
% 	HCAL thickness & 44 $\times$ 7.5 $\lambda_0$ & $\Longrightarrow$ & 44 $\times$ 5.5 $\lambda_0$ \\[0.18cm]
	ECAL thickness & 40 layers, 22 X$_0$ & $\Longrightarrow$ & 40 layers, 22 X$_0$ \\[0.18cm]
	HCAL thickness & 60 layers, 7.5 $\lambda_I$ & $\Longrightarrow$ & 44 layers, 5.5 $\lambda_I$ \\[0.18cm]
	Yoke thickness & 1989 mm & $\Longrightarrow$ & 1521 mm \\[0.18cm]
	MDI (forward region) &  & $\Longrightarrow$ & $<$ 150 mrad \\[0.4cm]
	Solenoid field & 4 Tesla & $\Longrightarrow$ & 2 Tesla \\
	
      \end{tabular}%
    }
    \end{minipage}
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%*****************************************************************************


%*****************************************************************************
\begin{frame}{\large \large Tracking}

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    \begin{minipage}{0.99\textwidth}

  \begin{itemize}
  \item Two tracking algorithms are available: 
  \begin{itemize}
   \item truth tracking - track fitting is done by using all hits produced by particle (by using truth information)
   \item conformal tracking - hits are found by pattern recognition algorithm in conformal space
  \end{itemize}
  \item Single-point resolution (sigma): VTX - 3$\times$3 $\mu$m; IT - 7$\times$300$\mu$m; OT - 7$\times$3000$\mu$m
 \end{itemize}

    \end{minipage}
};

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  \begin{itemize}
  \item Charged particles with p$_\mathrm{T} >$ 0.65 GeV reach calorimeter.
 \end{itemize}

    \end{minipage}
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