Changeset 562 in svn
- Timestamp:
- Apr 8, 2010, 11:19:53 PM (15 years ago)
- Location:
- trunk/paper/CommPhysComp
- Files:
-
- 7 edited
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trunk/paper/CommPhysComp/notes.tex
r561 r562 12 12 \usepackage{fancyhdr} 13 13 \usepackage{verbatim} 14 \addtolength{\textwidth}{1cm} \addtolength{\hoffset}{-0.5cm}14 %\addtolength{\textwidth}{1cm} \addtolength{\hoffset}{-0.5cm} 15 15 \usepackage[colorlinks=true, pdfstartview=FitV, linkcolor=blue, citecolor=blue, urlcolor=blue, unicode]{hyperref} 16 16 \usepackage{ifpdf} … … 159 159 \begin{figure*}[!ht] 160 160 \begin{center} 161 %\includegraphics[scale=0.78]{FlowDELPHES}162 161 \includegraphics[scale=0.78]{fig1} 163 162 \caption{Flow chart describing the principles behind \textit{Delphes}. Event … … 239 238 \begin{figure}[!ht] 240 239 \begin{center} 241 %\includegraphics[width=\columnwidth]{Detector_DELPHES_3}242 240 \includegraphics[width=\columnwidth]{fig2} 243 241 \caption{ … … 297 295 \begin{figure}[!ht] 298 296 \begin{center} 299 %\includegraphics[width=\columnwidth]{calosegmentation}300 297 \includegraphics[width=\columnwidth]{fig3} 301 298 \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.} … … 549 546 \begin{figure}[!ht] 550 547 \begin{center} 551 %\includegraphics[width=0.6\columnwidth]{Tau} 552 \includegraphics[width=0.80\columnwidth]{fig5} 548 \includegraphics[width=0.80\columnwidth]{fig4} 553 549 \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.} 554 550 \label{h_WW_ss_cut1} … … 592 588 \begin{figure}[!ht] 593 589 \begin{center} 594 %\includegraphics[width=\columnwidth]{Tau2} 595 \includegraphics[width=\columnwidth]{fig6} 590 \includegraphics[width=\columnwidth]{fig5} 596 591 \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 $\ell = e, \mu, \tau$. 597 592 Events generated with MadGraph/MadEvent~\citep{bib:mgme}. … … 615 610 \begin{figure}[!ht] 616 611 \begin{center} 617 %\includegraphics[width=\columnwidth]{Tau1} 618 \includegraphics[width=\columnwidth]{fig7} 612 \includegraphics[width=\columnwidth]{fig6} 619 613 \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}. 620 614 Histogram entries correspond to true $\tau$-jets, matched with generator-level data.} … … 688 682 \begin{figure}[!ht] 689 683 \begin{center} 690 %\includegraphics[width=\columnwidth]{fdets} 691 \includegraphics[width=\columnwidth]{fig4} 684 \includegraphics[width=\columnwidth]{fig7} 692 685 \caption{Default location of the very forward detectors, including 693 686 \textsc{ZDC}, \textsc{RP220} and \textsc{FP420} in the \textsc{LHC} beamline. … … 899 892 \begin{figure}[!ht] 900 893 \begin{center} 901 %\includegraphics[width=\columnwidth]{resolutionJet}902 894 \includegraphics[width=\columnwidth]{fig8} 903 895 \caption{Resolution of the transverse energy of reconstructed jets … … 986 978 \begin{figure}[!ht] 987 979 \begin{center} 988 %\includegraphics[width=\columnwidth]{resolutionETmis}989 980 \includegraphics[width=\columnwidth]{fig10} 990 981 \includegraphics[width=\columnwidth]{fig10b} … … 1072 1063 \begin{figure}[!ht] 1073 1064 \begin{center} 1074 %\includegraphics[width=\columnwidth]{Detector_DELPHES_2b}1075 1065 \includegraphics[width=\columnwidth]{fig11} 1076 1066 \caption{Layout of the generic detector geometry assumed in \textit{Delphes}. … … 1106 1096 \begin{figure}[!ht] 1107 1097 \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) 1100 and transverse (right) views, with $t \rightarrow Wb$. One 1113 1101 $W$ boson decays into a $\mu \nu_\mu$ pair and the second one into a $e \nu_e$ 1114 1102 pair. The surviving proton leaves a forward hemisphere with no hadronic … … 1127 1115 \begin{figure}[!ht] 1128 1116 \begin{center} 1129 %%\includegraphics[width=\columnwidth]{Events_DELPHES_1}1130 %\includegraphics[width=\columnwidth]{Displayppgg}1131 1117 \includegraphics[width=0.6\columnwidth]{fig13} 1132 1118 \caption{Example of inclusive gluon pair production $pp \rightarrow ggX$. Many
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