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\author{S.~Menke, MPP M{\"u}nchen}
\date{27-Oct-2010}
\title{HEC Group Activities 2007-2010}
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\begin{document}  
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Title                                                                         %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
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  \colormathc{blue}{\Large\baselineskip=12pt 
  HEC Group Activities 2007-2010} \centerline{\parbox{0.9\textwidth}{\tiny
      {\textcolor{white}{Visit of the Fachbeirat}}\hfill
      \href{http://www.mppmu.mpg.de/~menke}{\textcolor{pink}{Sven
          Menke}},~\href{http://www.mppmu.mpg.de/}{\textcolor{pink}{MPP
          M{\"u}nchen}} \hfill \thedate, MPP M{\"u}nchen}}

  \vspace{-0.2cm}

  \begin{center}\baselineskip=8pt
    \textcolor{white}{\tiny on behalf of the MPP Munich HEC Group:\\
      T.~Barillari, J.~Erdmann (until 12-2008), J.~Huber,
      P.~Giovannini, A.~Jantsch, A.~Kiryunin, S.~Menke, M.~Nagel,
      H.~Oberlack, G.~Pospelov, E.~Rauter (until 7-2009),
      D.~Salihagic, P.~Schacht}
  \end{center}
 
  \vspace{-0.6cm}
  
  \vbox to 0 pt{\parbox[c]{0.2\textwidth}{\p{a}}\parbox[c]{0.61\textwidth}{
      \textcolor{white}{\footnotesize
        \begin{itemize}\itemsep3pt\baselineskip11pt
        \item[\hyperlink{Intro}{\itriang}] The ATLAS Hadronic Endcap Calorimeter
        \item[\hyperlink{Commissioning}{\itriang}] Commissioning
          \textcolor{ghostwhite}{\tiny\raggedright\baselineskip=8pt
            \begin{itemize}\itemsep0pt
            \item[{\ibullet}] Cosmics
            \item[{\ibullet}] Beam Splash Events
            \item[{\ibullet}] Collisions
          \end{itemize}}
        \item[\hyperlink{LocalHadCalib}{\itriang}] Hadronic Calibration
          \textcolor{ghostwhite}{\tiny\raggedright\baselineskip=8pt
            \begin{itemize}\itemsep0pt
            \item[{\ibullet}] Local Hadron Calibration
            \item[{\ibullet}] Jet-level Corrections
            \item[{\ibullet}] Validation with Testbeam and Collisions
              Data
          \end{itemize}}
        \item[\hyperlink{Analysis}{\itriang}] Analysis
          \textcolor{ghostwhite}{\tiny\raggedright\baselineskip=8pt
            \begin{itemize}\itemsep0pt
            \item[{\ibullet}] Top-mass Measurements in the
              Semi-Leptonic and All-Hadronic Channel
          \end{itemize}}
        \item[\hyperlink{Upgrade}{\itriang}] Upgrade Activities for sLHC
          \textcolor{ghostwhite}{\tiny\raggedright\baselineskip=8pt
            \begin{itemize}\itemsep0pt
            \item[{\ibullet}] Cold Electronics
            \item[{\ibullet}] Low Voltage Power Supplies
          \end{itemize}}
  \end{itemize}}}}
  
  \vfill
  
  \hbox{ }\hfill{\small\Acrobatmenu{NextPage}{\textcolor{tomato}{%
        \replacecolor{mathcolor}{textcolor}\myRIGHT}}}
  
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
% Calorimeters                                                                  %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
\begin{slide}
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  \heading{\small The ATLAS Detector $\myRIGHT$ Calorimetry}
  
  \vspace{-0.7cm}

  \textcolor{white}{\footnotesize\raggedright\baselineskip=10pt
    \begin{itemize}\itemsep2pt
    \item[\itriang] Calorimeter coverage up to $|\eta| < 4.9$
      \item[\itriang] EM Barrel/Endcap: LAr/Pb Accordion $|\eta|<1.4$/$1.375 <|\eta|<3.2$
    \end{itemize}}
        
  \vspace{-0.5cm}

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      \item[\itriang] Had Barrel: iron/scintillating tiles $|\eta|\lesssim1.7$ 
      \item[\itriang] Had Endcap: LAr/Cu parallel plates $1.7 \lesssim |\eta| \lesssim 3.2$  
      \item[\itriang] EM(HAD) Forward: LAr/Cu(W) tubular electrodes $3.2 \lesssim |\eta| \lesssim 4.9$   
\end{itemize}}}
  \parbox[c]{0.6\textwidth}{
    \hspace{-0.5cm}\centerline{%
      \resizebox{0.7\textwidth}{!}{\includegraphics{calo2.png}}%
    }}
 
  \vspace{-0.8cm}

  \textcolor{white}{\footnotesize\raggedright\baselineskip=10pt
    \begin{itemize}\itemsep-3pt
      \item[\itriang] typical cell sizes $\Delta\eta \times \Delta\phi = 0.025\times0.025$ (EM) and $0.1\times0.1$ (HAD);\\ $3$ to $7$ samplings; at least $10\,\lambda$  
      \item[\itriang] $e/\gamma$: $\sigma_E/E \simeq 10\%/\sqrt{E}$
      \item[\itriang] jets: $\sigma_E/E \simeq 50\%/\sqrt{E} \oplus 3\%$
    \end{itemize}}

  \vspace{-0.3cm}

  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% HEC Geometry                                                                  %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
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  \pdfbookmark[1]{HEC Calorimeter}{HEC}
  \heading{\small The ATLAS Calorimeters $\itriang$ Hadronc Endcap Calorimeter (HEC)}

  \vspace{-0.1cm}

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          \begin{itemize}
          \item[\ibullet] Absorbers plates parallel to beam axis
          \item[\ibullet] $\sf 2.5\,cm$ thick Cu plates in HEC 1
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      \end{itemize}}
      \end{itemize}}}   
  \parbox[c]{0.3\textwidth}{%
    \textcolor{black}{\resizebox{0.3\textwidth}{!}{%
    \includegraphics{hec1mod}}}}
        
  \vspace{-0.5cm}

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          \begin{itemize}
          \item[\ibullet] $\delta\eta\times\delta\phi \simeq 0.1(0.2)\times 0.1(0.2)$
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          \item[\ibullet] Layer2 (HEC1 Back): $\sum 16\,{\sf gaps}$
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          \item[\ibullet] Layer3\&4 (HEC2 Front\&Back): $\sum 8\,{\sf gaps}$
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          \item[\ibullet] $5632$ readout channels
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  \footing
\end{slide}    

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% MPI Contribution                                                              %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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  \vspace{-0.1cm}

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          \item[\ibullet] GaAs based readout electronics 
            made by MPP
          \item[\ibullet] radiation hard up to $3\times10^{14}\,{\sf n}/{\sf cm}^{2}$ corresponding to $\sim 15$ times the expected fluence after $10$ years of LHC 
          \end{itemize}}
      \end{itemize}}}   
  \parbox[c]{0.3\textwidth}{%
    \textcolor{black}{\resizebox{0.3\textwidth}{!}{%
        \includegraphics{psb}}}}

  \vspace{-0.2cm}

    \textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
      \begin{itemize}
      \item[\itriang] Construction/Installation (up to 2006)
        \textcolor{ghostwhite}{\footnotesize\baselineskip=9pt
          \begin{itemize}
          \item[\ibullet] about $1/4$ of all modules assembled at MPP
          \item[\ibullet] stacking of copper plates, cabling, quality
            control including beam tests (see bottom picture for one full wheel) 
          \end{itemize}}
      \item[\itriang] Commisioning (2007-2009)
        \textcolor{ghostwhite}{\footnotesize\baselineskip=9pt
          \begin{itemize}
          \item[\ibullet] Pulse shape and noise measurements with
            Cosmic Muons and Beam Splash events
          \end{itemize}}
      \item[\itriang] Calibration (since 1999)
        \textcolor{ghostwhite}{\footnotesize\baselineskip=9pt
          \begin{itemize}
          \item[\ibullet] Cluster reconstruction and Hadronic Calibraton 
          \item[\ibullet] Validation with test beam and collisions data
          \end{itemize}}
      \end{itemize}}   

  \vspace{-0.5cm}
  
  \footing
\end{slide}    

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Commissioning                                                                 %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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  \vspace{-0.3cm}

  \parbox[c]{0.69\textwidth}{%
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          from muons traversing LAr gaps in the HEC allows to check
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        \item[\ibullet] only small deviations from predicted shape ($3-5\%$) 
          have been observed 
        \end{itemize}}
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  \parbox[c]{0.3\textwidth}{%
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  \vspace{-0.3cm}

  \parbox[c]{0.3\textwidth}{%
    \textcolor{black}{\resizebox{0.34\textwidth}{!}{%
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  \vspace{-0.3cm}

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    \begin{itemize}\itemsep1pt
    \item[\itriang] Commissioning with collisions
      \textcolor{ghostwhite}{\tiny\baselineskip=8pt
        \begin{itemize}\itemsep0pt
        \item[\ibullet] Ratio of Cluster energy in Minium Bias events at $\sqrt{s} = 900\,{\sf GeV}$ in Data over Monte Carlo simulations shows agreement already on $5\%$ level 
        \end{itemize}}
    \end{itemize}}}
  \parbox[c]{0.3\textwidth}{%
    \textcolor{black}{\resizebox{0.3\textwidth}{!}{%
        \includegraphics{fig_12}}}}

  \vspace{-0.5cm}

  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Hadronic Calibration                                                          %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{LocalHadCalib}{}
  \pdfbookmark[0]{Hadronic Calibration}{LocalHadCalib}
  \heading{\small Hadronic Calibration}
  
  \vspace{-0.5cm}

  \parbox[c]{0.49\textwidth}{
    \textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
      \begin{itemize}\itemsep1pt
      \item[\itriang] Aim is to have best possible response to hadrons and
      electrons in physics channels like ${\sf t}\bar{\sf
	t}\to{\sf Wb}\,{\sf Wb}\to{\sf l}\nu j_{\sf b}\,
      jjj_{\sf b}$
      \textcolor{ghostwhite}{
        \begin{itemize}\itemsep1pt
        \item[\ibullet] pseudo event display in $r-\phi$ and $r-z$ 
	  illustrates this 
        \item[\ibullet] use calorimeter objects calibrated to stable particle 
	  level to form jets which point back to primary partons   
      \end{itemize}}
    \end{itemize}}}
  \parbox[c]{0.49\textwidth}{
    \textcolor{black}{\resizebox{0.5\textwidth}{!}{%
        \includegraphics{ttbar5RPhi}}}}
  
  \vspace{-1.2cm}

  \centerline{\p{a}\hfill\textcolor{black}{\resizebox{0.8\textwidth}{!}{%
	\includegraphics{ttbar5RZ}}}}
  
  \vspace{-1.2cm}

  \textcolor{white}{\tiny MC{\myat}NLO\replacecolor{mathcolor}{white} ${\sf t}\bar{\sf t}$ Event (semileptonic)}

  \vspace{-1.2cm}

  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Hadron Calorimetry in ATLAS                                                   %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{Hadron Shower Components}{}
  \pdfbookmark[1]{Hadron Shower Components}{Hadron Shower Components}
  \heading{\small Hadronic Calibration \itriang\ Hadron Shower Components}
  
  \vspace{-0.2cm}
  
  \parbox[c]{0.35\textwidth}{%
    \textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
      \begin{itemize}
      \item[\itriang] A hadronic shower consists of
        \textcolor{ghostwhite}{\tiny\baselineskip=8pt
          \begin{itemize}
          \item[\ibullet] EM energy (e.g. $\pi^0\to\gamma\gamma$)
            $O(50\,\%)$
          \item[\ibullet] visible non-EM energy (e.g. ${\sf d}E/{\sf
              d}x$ from $\pi^\pm$,$\mu^\pm$, etc.) $O(25\,\%)$
          \item[\ibullet] invisible energy (e.g. breakup of nuclei and
            nuclear excitation) $O(25\,\%)$
          \item[\ibullet] escaped energy (e.g. $\nu$) $O(2\,\%)$
          \end{itemize}}
      \item[\itriang] each fraction is energy dependent and subject to
        large fluctuations
      \end{itemize}}}   
  \parbox[c]{0.64\textwidth}{%
  \textcolor{blue}{\resizebox{0.65\textwidth}{!}{%
      \includegraphics{had-shower}}}}

\vspace{-0.3cm}

\textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
  \begin{itemize}
  \item[\itriang] invisible energy is the main source of the
    non-compensating nature of hadron calorimeters
  \item[\itriang] hadronic calibration has to account for the
    invisible and escaped energy and deposits in dead material
    and ignored calorimeter parts
  \end{itemize}}  
\vspace{-0.1cm}
  
\footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Hadron Calorimetry in ATLAS II                                                %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \heading{\small Hadronic Calibration \itriang\ Hadron Shower Components}
  
  \vspace{-0.2cm}
  
  \textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
    \begin{itemize}
    \item[\itriang] From a {\em Geant4} simulation of endcap calorimeters
    \end{itemize}}
  
  \vspace{-0.4cm}

  \parbox[c]{0.64\textwidth}{%
    \textcolor{black}{\resizebox{0.65\textwidth}{!}{%
        \includegraphics{E_frac_QGSP}}}}
  \parbox[c]{0.35\textwidth}{%
    \textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
      \begin{itemize}
      \item[]
        \textcolor{ghostwhite}{\tiny\baselineskip=8pt
          \begin{itemize}
          \item[\ibullet] EM energy strongly {\em anti-correlated} with
            visible non-EM energy
          \item[\ibullet] visible non-EM energy strongly {\em
              correlated} with invisible energy 
          \end{itemize}}
      \item[\itriang] need to separate EM part of the shower from the
        non-EM part
      \item[\itriang] apply a weight to the non-EM part to compensate
        invisible energy
      \end{itemize}}}   
  
  \vspace{-0.3cm}

  \textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
    \begin{itemize}
    \item[\itriang] How to separate EM fraction from non-EM
      fraction?  
      \textcolor{ghostwhite}{\tiny\baselineskip=6pt\itemsep-1pt
        \begin{itemize}
        \item[\ibullet] $X_0 \ll \lambda \simeq 20\,{\sf cm}$ 
        \item[\ibullet] {\em high} energy density in a cell denotes
          high EM activity
        \item[\ibullet] {\em low} energy density in a cell
          corresponds to hadronic activity
        \item[\ibullet] apply weights as function of energy density
        \end{itemize}}
    \end{itemize}} 
  
  \vspace{-0.1cm}
  
  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Hadron Calorimetry in ATLAS II                                                %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{LocalHad}{}
  \pdfbookmark[1]{Local Hadron Calibration}{LocalHad}
  \heading{\small Hadronic Calibration \itriang\ Local Hadron Calibration}
  
  \vspace{-0.6cm}
  
  \textcolor{white}{\footnotesize\raggedright\baselineskip=8pt\itemsep1pt
    \begin{itemize}
    \item[\itriang] Local Hadron Calibration is a modular approach
      with 5 steps developed at MPP for hadronic calibration
      \textcolor{ghostwhite}{%\tiny%\baselineskip=6pt\itemsep-1pt
        \begin{description}
        \item[Classification] clusters are classified as
          electromagnetic or hadronic based on shower shape variables
          (cluster moments)
        \item[Weighting] cells in hadronic clusters are corrected as
          function of energy density ($e/h$ compensation)
        \item[Out-Of-Cluster] energy deposits outside clusters but
          inside the calorimeter are corrected on cluster level
        \item[Dead-Material] energy deposits outside the calorimeter
          are corrected on cluster level
        \item[Jet-Correction] final jet-level corrections compensate
          particles without any calorimeter signal
        \end{description}}
    \item[\itriang] continous refinement of calibration constants to
      keep up with changes in the simulation (G.~Pospelov, S.~Menke)
    \item[\itriang] jet level corrections derived as part of PhD
      thesis (A.~Jantsch)
    \item[\itriang] validation on test beam (J.~Erdmann, A.~Kiryunin,
      G.~Pospelov) and collisions data (P.~Giovannini) and application
      to MET and top-quark pairs (T.~Barillari)
    \end{itemize}}
  
  \vspace{-0.4cm}

  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
% Cluster Moments                                                               %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{Moments}{}
  \pdfbookmark[1]{Cluster Moments}{Moments}
  \heading{\small Hadronic Calibration \itriang\ Cluster Moments}
  
  \vspace{-0.3cm}

  \parbox[c]{0.54\textwidth}{
  \textcolor{white}{\footnotesize\raggedright\baselineskip=10pt
    \begin{itemize}\itemsep2pt
    \item[\itriang] shape variables calculated from the positive cells in a cluster
    \item[\itriang] first a principal value analysis is run on the cluster cells
        \textcolor{ghostwhite}{\tiny\baselineskip=8pt
          \begin{itemize}\itemsep0pt
          \item[\ibullet] provides centroid and 3 major axes of the shower
            \end{itemize}}
    \item[\itriang] angles of the major axis w.r.t.~IP-shower-center direction
      are calculated
    \item[\itriang] other shape quantities defined by moments of the form\\
      $\Dy\langle x^n\rangle=\frac{1}{E_{\textsf{norm}}}\times\!\!\!\sum\limits_{\{i|E_i>0\}}{\!\!\!\!\!E_i\,x_i^n}$, with\\
      $\Dy E_{\textsf{norm}} = \!\!\!\sum\limits_{\{i|E_i>0\}}{\!\!\!\!\!E_i}$.
    \end{itemize}}}
  \parbox[c]{0.45\textwidth}{
    \resizebox{0.45\textwidth}{!}{%
      \includegraphics{ClusterMoments}}}

  \vspace{-0.6cm}

  \textcolor{white}{\footnotesize\raggedright\baselineskip=10pt
    \begin{itemize}\itemsep2pt
    \item[\itriang] typical choices for $x$: energy density
      $\rho=E/V$, radial distance from shower axis $r$, longitudinal
      distance along major shower axis $\lambda$
    \item[\itriang] plot shows cell energy distribution for charged
      pion showers in $r-\lambda$ space and some shape variables
      superimposed
    \end{itemize}}

  \vspace{-0.3cm}

  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Performance of single pions                                                   %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{Perf}{}
  \pdfbookmark[1]{Performance of Single Pions and Jets}{Perf}
  \heading{\small Hadronic Calibration $\myRIGHT$ Performance}

  \vspace{-0.6cm}
  
  \textcolor{white}{\footnotesize\raggedright\baselineskip=10pt
    \begin{itemize}\itemsep2pt
    \item[\itriang] Linearity (left) and Resolution (right) after each
      calibration step as function of pion energy
    \end{itemize}}
  
  \centerline{
    \replacecolor{textcolor}{white}%
    \replacecolor{presentcolor}{white}%
    \present{\textcolor{black}{\resizebox{0.4\textwidth}{!}{%
          \includegraphics{../LocalHadCalib/LCSinglePionsPerf/pictures/LCSinglePionsPerf_piplus_r796_tid081901_15.5.1ndim.vv05.piprob.sum/pict_page12_LCSinglePionsPerf_piplus_Linearity_vs_ebeam_etabin1.pdf}}}}
    \present{\textcolor{black}{\resizebox{0.4\textwidth}{!}{%
          \includegraphics{../LocalHadCalib/LCSinglePionsPerf/pictures/LCSinglePionsPerf_piplus_r796_tid081901_15.5.1ndim.vv05.piprob.sum/pict_page10_LCSinglePionsPerf_piplus_Resolution_vs_ebeam_etabin1.pdf}}}}}
  
  \vspace{-0.1cm}
  
  \parbox[c]{0.54\textwidth}{
    \textcolor{white}{\footnotesize\raggedright\baselineskip=10pt
      \begin{itemize}\itemsep2pt
      \item[\itriang] linearity and resolution improve in every step
      \item[\itriang] linearity on jet level after each calibration step 
        shown on the right
      \item[\itriang] especially at low jet energies final jet-level
        corrections are needed due to lost particles 
      \end{itemize}}}
  \parbox[c]{0.45\textwidth}{
    \resizebox{0.45\textwidth}{!}{%
      \includegraphics{ResponseJetLevelCorrectColors}}}
  
  \vspace{-0.5cm}
  
  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 
% Jet Level Corrections                                                         %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{JLC}{}
  \pdfbookmark[1]{Jet Level Corrections}{JLC}
  \heading{\small Hadronic Calibration $\myRIGHT$ Jet Level Corrections}

  \vspace{-0.4cm}

  \textcolor{white}{\footnotesize\raggedright\baselineskip=10pt
    \begin{itemize}\itemsep2pt
    \item[\itriang] energy fraction caried by low energetic clusters
      inside jet is correlated with lost energy
    \item[\itriang] compute correction weights based on this quantity
    \item[\itriang] left plot shows the weights as function of
      the low energy fraction and the jet energy 
    \item[\itriang] right plot shows linearity for jets before any calibration (black), after cluster calibration (red) and after final jet calibration (blue)
    \end{itemize}}

  \centerline{
    \replacecolor{textcolor}{white}%
    \replacecolor{presentcolor}{white}%
    \present{\textcolor{black}{\resizebox{0.33\textwidth}{!}{%
          \includegraphics{jantsch_jlc_ieta_inv_1}}}}
    \present{\textcolor{black}{\resizebox{0.47\textwidth}{!}{%
          \includegraphics{jantsch_lin_0}}}}}
  
  \vspace{-0.4cm}
  
  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Analysis                                                                 %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{Analysis}{}
  \pdfbookmark[0]{Analysis}{Top Quark Analyses}
  \heading{\small Top Quark Analyses}
  
  \vspace{-0.5cm}

  \textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
    \begin{itemize}\itemsep1pt
    \item[\itriang] ${\sf t}\bar{\sf t}$ Analysis in the semileptonic channel (A.~Jantsch)
      \textcolor{ghostwhite}{\tiny\baselineskip=8pt
        \begin{itemize}\itemsep0pt
        \item[\ibullet] based on simulations at $\sqrt{s} = 10\,{\sf TeV}$
        \item[\ibullet] Signal produced with \code{MC{\myat}NLO}
        \item[\ibullet] QCD background with \code{Alpgen}
        \item[\ibullet] Jets from the \code{AntiKt} jet algorithm 
          with local hadron calibrated clusters and jet-level-corrections as input
        \item[\ibullet] Exactly one good electron or muon with $p_\perp > 10\,{\sf GeV}$ and $|\eta| < 2.5$
        \item[\ibullet] At least $4$ good jets with $E_\perp > 20\,{\sf GeV}$  and $|\eta| < 2.5$
        \item[\ibullet] $E_\perp^\textsf{miss} > 10\,{\sf GeV}$
        \item[\ibullet] combine $3$ jets to hadronic top quark candidate
          by either maximizing $p_\perp$ of the tripplet (left) or by minimizing $\Delta R$ of the tripplet (right) 
        \item[\ibullet] fit Gaussian with exponential left side tail 
          plus polynomial to obtain top quark mass
        \end{itemize}}
    \end{itemize}}

  \centerline{
    \replacecolor{textcolor}{white}%
    \replacecolor{presentcolor}{white}%
    \present{\textcolor{black}{\resizebox{0.45\textwidth}{!}{%
          \includegraphics{top_had_m_fit_1}}}}
    \present{\textcolor{black}{\resizebox{0.45\textwidth}{!}{%
          \includegraphics{top_had_m_fit_2}}}}}
  

  \vspace{-0.5cm}

  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Analysis                                                                 %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \heading{\small Top Quark Analyses}
  
  \vspace{-0.5cm}

  \textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
    \begin{itemize}\itemsep1pt
    \item[\itriang] ${\sf t}\bar{\sf t}$ Analysis in the all-hadronic channel (P.~Giovannini)
      \textcolor{ghostwhite}{\tiny\baselineskip=8pt
        \begin{itemize}\itemsep0pt
        \item[\ibullet] same $\sqrt{s} = 10\,{\sf TeV}$ simulation as semi-leptonic analysis
        \item[\ibullet] No good electron or muon with $p_\perp > 10\,{\sf GeV}$ and $|\eta| < 2.5$
        \item[\ibullet] At least $6$ good jets with $E_\perp > 20\,{\sf GeV}$  and $|\eta| < 2.5$
        \item[\ibullet] $E_\perp^\textsf{miss}/0.5\sqrt{\sum{E_\perp}} < 6.5$ (no significant missing transverse energy)
        \item[\ibullet] $2$ jets tagged as ${\sf b}$-jets
        \item[\ibullet] Event shape cuts on centrality $\sum{E_\perp}/m_\textsf{jets} > 0.6$ and $\sum{E_\perp} - E_\perp^\textsf{max} - E_\perp^\textsf{2nd}> 170\,{\sf GeV}$ help reduce QCD bckgd.
        \item[\ibullet] sub-leading jet cuts: $p_\perp^\textsf{4th} > 40\,{\sf GeV}$;  $p_\perp^\textsf{5th} > 30\,{\sf GeV}$  
        \item[\ibullet] $\Delta R({\sf b}\textsf{-jets})> 1.5$ $\myRIGHT$ $S/B$ improves from $1/10000$ before to $1/3.6$ after all cuts 
        \end{itemize}}
    \end{itemize}}

  \centerline{
    \replacecolor{textcolor}{white}%
    \replacecolor{presentcolor}{white}%
    \present{\textcolor{black}{\resizebox{0.35\textwidth}{!}{%
          \includegraphics{FinalTop}}}}
    \present{\textcolor{black}{\resizebox{0.35\textwidth}{!}{%
          \includegraphics{FitFinalTop}}}}}
  

  \vspace{-0.5cm}

  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Upgrade                                                                       %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{Upgrade}{}
  \pdfbookmark[0]{Upgrade Activities for sLHC}{Upgrade}
  \heading{\small Upgrade Activities for sLHC}
  
  \vspace{-0.5cm}

  \parbox[c]{0.6\textwidth}{
  \textcolor{white}{\footnotesize\raggedright\baselineskip=9pt
    \begin{itemize}\itemsep1pt
    \item[\itriang] MPP contributed two hardware components to the exisiting HEC 
      \textcolor{ghostwhite}{\tiny\baselineskip=8pt
        \begin{itemize}\itemsep0pt
        \item[\ibullet] Cold readout electronics based on GaAs pre-amplifiers
        \item[\ibullet] Low Voltage Power Supplies sitting just outside the 
          cryostats 
        \end{itemize}}
    \item[\itriang] The current cold electronics withstand $1.5$ times
      the expected radiation dose of $10\,$years running with LHC
      including safety factors
    \item[\itriang] Thus a factor $10$ increase as anticipated by the
      sLHC upgrade scenarios (see plot) brings the electronics at its limits and
      eliminates any safety factor.
    \end{itemize}}}
  \parbox[c]{0.39\textwidth}{
        \replacecolor{textcolor}{white}%
        \replacecolor{presentcolor}{white}%
        \present{\textcolor{black}{\resizebox{0.39\textwidth}{!}{%
              \includegraphics{Cal_TID_Atlas}}}}}

  \vspace{-0.5cm}

  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Upgrade                                                                       %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{Electronics}{}
  \pdfbookmark[1]{Electronics}{Electronics}
  \heading{\small Upgrade Activities for sLHC $\myRIGHT$ Electronics}
  
  \vspace{-0.2cm}

  \parbox[c]{0.6\textwidth}{
    \textcolor{white}{\tiny\raggedright\baselineskip=8pt
      \begin{itemize}\itemsep1pt
      \item[\itriang] The LV PS would not withstand the radiation conditions at 
        sLHC and provide not enough redundancy\\
        $\myRIGHT$ the need to be exchanged at sLHC even if the cold electronics 
        stays the same
      \item[\itriang] Exact radiation levels for LHC have to be
        established until
        end of 2011\\
        $\myRIGHT$ only then we know for certain if the cold
        electronics have to
        be exchanged\\
        $\myRIGHT$ current numbers including safety factor of $10$ for
        $10\,$years running: LHC = $2\times10^{14}\,{\sf n}/{\sf
          cm}^2$; sLHC $2\times10^{15}\,{\sf n}/{\sf cm}^2$
      \item[\itriang] The R\&D for a possible upgrade has started
        already (2012 would be too late)
      \item[\itriang] Amplitude loss after irradiation for the
        exisiting cold electronics and $4$ bipolar transistors tested
        for sLHC (bottom)
      \item[\itriang] SiGe bipolar, GaAs FET and Si COMOS FET
        transistors are currently tested. So far all technologies
        tested would tolerate the sLHC radiation levels
      \item[\itriang] for cost reasons the Si based CMOS option is
        currently prefered
      \item[\itriang] a modified transistor design for further tests
        in the cold and under irradiation (in Rez/Prague) is in
        progress
    \end{itemize}}}
  \parbox[c]{0.39\textwidth}{
    \centerline{
      \replacecolor{textcolor}{white}%
      \replacecolor{presentcolor}{white}%
      \present{\textcolor{black}{\resizebox{0.35\textwidth}{!}{%
            \includegraphics{radt}}}}
    }
    \centerline{
      \replacecolor{textcolor}{white}%
      \replacecolor{presentcolor}{white}%
      \present{\textcolor{black}{\resizebox{0.35\textwidth}{!}{%
          \includegraphics{IHP34}}}}}}

  \vspace{-0.5cm}

  \footing
\end{slide}

%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Upgrade                                                                       %
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\begin{slide}
  \backgroundstyle
  [%
  startcolor=midnightblue,endcolor=royalblue,firstgradprogression=3,
  toppanelheight=0.6cm,toppanelcolor=royalblue,
  bottompanelheight=0.4cm,bottompanelcolor=navy%
  ]{vgradient}%
  \hypertarget{HILUM}{}
  \pdfbookmark[1]{High Lumi Experiment}{HILUM}
  \heading{\small Upgrade Activities for sLHC $\myRIGHT$ High Lumi Experiment}
  
  \vspace{-0.2cm}

  \parbox[c]{0.6\textwidth}{
    \textcolor{white}{\tiny\raggedright\baselineskip=8pt
      \begin{itemize}\itemsep1pt
      \item[\itriang] The operation of the endcap calorimeters under
        high radiation levels is tested at the IHEP $70\,{\sf GeV}$
        synchrotron in Protvino, Russia
      \item[\itriang] Small test modules corresponding to the
        electromagnetic (EMEC), hadronic (HEC) endcap and forward
        (FCal) calorimeters are exposed to beams of $10^{13}$ protons
        per spill
      \item[\itriang] Main objective is if the ion-buildup in the LAr
        expected at sLHC can still be tolerated
      \item[\itriang] A degradation of the pulse shape is expected in
        the EMEC and HEC (upper plot shows pulse shape in the EMEC at
        low radiation rates; lower plot at high rates)
      \item[\itriang] Tests so far indicate that the EMEC and HEC can be operated
        with possibly modified electronics 
      \item[\itriang] The FCal needs to be either replaced by a device
        with smaller LAr gaps or a new detector has to be placed in
        front of the existing FCal to withstand the sLHC radiation
        levels
      \end{itemize}}}
  \parbox[c]{0.39\textwidth}{
    \centerline{
      \replacecolor{textcolor}{white}%
      \replacecolor{presentcolor}{white}%
      \present{\textcolor{black}{\resizebox{0.35\textwidth}{!}{%
            \rotatebox{270}{\includegraphics{pulse_low}}}}}
    }
    \centerline{
      \replacecolor{textcolor}{white}%
      \replacecolor{presentcolor}{white}%
      \present{\textcolor{black}{\resizebox{0.35\textwidth}{!}{%
          \rotatebox{270}{\includegraphics{pulse_high}}}}}}}

  \vspace{-0.5cm}

  \footinglast

\end{slide}

\end{document}

