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Changeset 562 in svn


Ignore:
Timestamp:
Apr 8, 2010, 11:19:53 PM (14 years ago)
Author:
Xavier Rouby
Message:

arXiv v3

Location:
trunk/paper/CommPhysComp
Files:
7 edited

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  • trunk/paper/CommPhysComp/notes.tex

    r561 r562  
    1212\usepackage{fancyhdr}
    1313\usepackage{verbatim}
    14 \addtolength{\textwidth}{1cm} \addtolength{\hoffset}{-0.5cm}
     14%\addtolength{\textwidth}{1cm} \addtolength{\hoffset}{-0.5cm}
    1515\usepackage[colorlinks=true, pdfstartview=FitV, linkcolor=blue, citecolor=blue, urlcolor=blue, unicode]{hyperref}
    1616\usepackage{ifpdf}
     
    159159\begin{figure*}[!ht]
    160160\begin{center}
    161 %\includegraphics[scale=0.78]{FlowDELPHES}
    162161\includegraphics[scale=0.78]{fig1}
    163162\caption{Flow chart describing the principles behind \textit{Delphes}. Event
     
    239238\begin{figure}[!ht]
    240239\begin{center}
    241 %\includegraphics[width=\columnwidth]{Detector_DELPHES_3}
    242240\includegraphics[width=\columnwidth]{fig2}
    243241\caption{
     
    297295\begin{figure}[!ht]
    298296\begin{center}
    299 %\includegraphics[width=\columnwidth]{calosegmentation}
    300297\includegraphics[width=\columnwidth]{fig3}
    301298\caption{Default segmentation of the calorimeters in the $(\eta,\phi)$ plane. Only the central detectors (\textsc{ECAL}, \textsc{HCAL}) and \textsc{FCAL} are considered. $\phi$ angles are expressed in radians.}
     
    549546\begin{figure}[!ht]
    550547\begin{center}
    551 %\includegraphics[width=0.6\columnwidth]{Tau}
    552 \includegraphics[width=0.80\columnwidth]{fig5}
     548\includegraphics[width=0.80\columnwidth]{fig4}
    553549\caption{Illustration of the identification of $\tau$-jets ($1-$prong). The jet cone is narrow and contains only one track. The small cone serves to apply the \textit{electromagnetic collimation}, while the broader cone is used to reconstruct the jet originating from the $\tau$-decay.}
    554550\label{h_WW_ss_cut1}
     
    592588\begin{figure}[!ht]
    593589\begin{center}
    594 %\includegraphics[width=\columnwidth]{Tau2}
    595 \includegraphics[width=\columnwidth]{fig6}
     590\includegraphics[width=\columnwidth]{fig5}
    596591\caption{Distribution of the electromagnetic collimation $C_\tau$ variable for true $\tau$-jets, normalised to unity. This distribution is shown for associated $WH$ photoproduction~\citep{bib:whphotoproduction}, where the Higgs boson decays into a $W^+ W^-$ pair. Each $W$ boson decays into a $\ell \nu_\ell$ pair, where $\ell = e, \mu, \tau$.
    597592Events generated with MadGraph/MadEvent~\citep{bib:mgme}.
     
    615610\begin{figure}[!ht]
    616611\begin{center}
    617 %\includegraphics[width=\columnwidth]{Tau1}
    618 \includegraphics[width=\columnwidth]{fig7}
     612\includegraphics[width=\columnwidth]{fig6}
    619613\caption{Distribution of the number of tracks $N^\textrm{tracks}$ within a small jet cone for true $\tau$-jets, normalised to unity. Photoproduced $WH$ events, where $W$ bosons decay leptonically ($e,\mu,\tau$), as in Fig.~\ref{fig:tau2}.
    620614Histogram entries correspond to true $\tau$-jets, matched with generator-level data.}
     
    688682\begin{figure}[!ht]
    689683\begin{center}
    690 %\includegraphics[width=\columnwidth]{fdets}
    691 \includegraphics[width=\columnwidth]{fig4}
     684\includegraphics[width=\columnwidth]{fig7}
    692685\caption{Default location of the very forward detectors, including
    693686\textsc{ZDC}, \textsc{RP220} and \textsc{FP420} in the \textsc{LHC} beamline.
     
    899892\begin{figure}[!ht]
    900893\begin{center}
    901 %\includegraphics[width=\columnwidth]{resolutionJet}
    902894\includegraphics[width=\columnwidth]{fig8}
    903895\caption{Resolution of the transverse energy of reconstructed jets
     
    986978\begin{figure}[!ht]
    987979\begin{center}
    988 %\includegraphics[width=\columnwidth]{resolutionETmis}
    989980\includegraphics[width=\columnwidth]{fig10}
    990981\includegraphics[width=\columnwidth]{fig10b}
     
    10721063\begin{figure}[!ht]
    10731064\begin{center}
    1074 %\includegraphics[width=\columnwidth]{Detector_DELPHES_2b}
    10751065\includegraphics[width=\columnwidth]{fig11}
    10761066\caption{Layout of the generic detector geometry assumed in \textit{Delphes}.
     
    11061096\begin{figure}[!ht]
    11071097\begin{center}
    1108 %%\includegraphics[width=\columnwidth]{Events_DELPHES_1}
    1109 %\includegraphics[width=\columnwidth]{DisplayWt}
    1110 \includegraphics[width=0.6\columnwidth]{fig12}
    1111 \caption{Example of $pp(\gamma p \rightarrow Wt)pY$ event display in
    1112 transverse view, with $t \rightarrow Wb$. One
     1098\includegraphics[width=0.9\columnwidth]{fig12}
     1099\caption{Example of $pp(\gamma p \rightarrow Wt)pY$ event display in side (left)
     1100and transverse (right) views, with $t \rightarrow Wb$. One
    11131101$W$ boson decays into a $\mu \nu_\mu$ pair and the second one into a $e \nu_e$
    11141102pair. The surviving proton leaves a forward hemisphere with no hadronic
     
    11271115\begin{figure}[!ht]
    11281116\begin{center}
    1129 %%\includegraphics[width=\columnwidth]{Events_DELPHES_1}
    1130 %\includegraphics[width=\columnwidth]{Displayppgg}
    11311117\includegraphics[width=0.6\columnwidth]{fig13}
    11321118\caption{Example of inclusive gluon pair production $pp \rightarrow ggX$. Many
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