Changeset 460 in svn for trunk/paper/CommPhysComp
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- Jul 10, 2009, 10:49:17 AM (15 years ago)
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- trunk/paper/CommPhysComp
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trunk/paper/CommPhysComp/notes.tex
r441 r460 57 57 \textit{Preprint:} \texttt{CP3-09-01}, \texttt{arXiv:0903.2225 [hep-ph]}\\ \\ 58 58 %\includegraphics[scale=0.8]{DelphesLogoSml}\\ 59 \includegraphics[scale=0.8]{fig 1}\\59 \includegraphics[scale=0.8]{fig0}\\ 60 60 {\bf PROGRAM SUMMARY}\\ 61 61 \begin{small} … … 133 133 \begin{center} 134 134 %\includegraphics[scale=0.78]{FlowDelphes} 135 \includegraphics[scale=0.78]{fig 2}135 \includegraphics[scale=0.78]{fig1} 136 136 \caption{Flow chart describing the principles behind \textsc{Delphes}. Event files coming from external Monte Carlo generators are read by a converter stage (top). 137 137 The kinematics variables of the final-state particles are then smeared according to the tunable subdetector resolutions. … … 185 185 \begin{center} 186 186 %\includegraphics[width=\columnwidth]{Detector_Delphes_3} 187 \includegraphics[width=\columnwidth]{fig 3}187 \includegraphics[width=\columnwidth]{fig2} 188 188 \caption{ 189 189 Profile of layout of the generic detector geometry assumed in \textsc{Delphes}. The innermost layer, close to the interaction point, is a central tracking system (pink). … … 273 273 \begin{center} 274 274 %\includegraphics[width=\columnwidth]{calosegmentation} 275 \includegraphics[width=\columnwidth]{fig 4}276 \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 expresse d in radians.}275 \includegraphics[width=\columnwidth]{fig3} 276 \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 expressend in radians.} 277 277 \label{fig:calosegmentation} 278 278 \end{center} … … 290 290 \begin{center} 291 291 %\includegraphics[width=\columnwidth]{fdets} 292 \includegraphics[width=\columnwidth]{fig 5}292 \includegraphics[width=\columnwidth]{fig4} 293 293 \caption{Default location of the very forward detectors, including \textsc{zdc}, \textsc{rp220} and \textsc{fp420} in the \textsc{lhc} beamline. 294 294 Incoming (red) and outgoing (black) beams on one side of the interaction point ($s=0~\textrm{m}$). … … 489 489 \begin{center} 490 490 %\includegraphics[width=0.6\columnwidth]{Tau} 491 \includegraphics[width=0.6\columnwidth]{fig 6}491 \includegraphics[width=0.6\columnwidth]{fig5} 492 492 \caption{Illustration of the identification of $\tau$-jets ($1-$prong). The jet cone is narrow and contains only one track. The small cone shown as the red one is used for the \textit{electromagnetic collimation}, while the green cone is the cone radius used to reconstruct the jet originating from the $\tau$-decay.} 493 493 \label{h_WW_ss_cut1} … … 528 528 \begin{center} 529 529 %\includegraphics[width=\columnwidth]{Tau2} 530 \includegraphics[width=\columnwidth]{fig 7}530 \includegraphics[width=\columnwidth]{fig6} 531 531 \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 $\ell = e, \mu, \tau$. 532 532 Events generated with \textsc{MadGraph/MadEvent}~\citep{bib:mgme}. … … 547 547 \begin{center} 548 548 %\includegraphics[width=\columnwidth]{Tau1} 549 \includegraphics[width=\columnwidth]{fig 8}549 \includegraphics[width=\columnwidth]{fig7} 550 550 \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}. 551 551 Histogram entries correspond to true $\tau$-jets, matched with generator-level data.} … … 636 636 \begin{center} 637 637 %\includegraphics[width=\columnwidth]{resolutionJet} 638 \includegraphics[width=\columnwidth]{fig 9}638 \includegraphics[width=\columnwidth]{fig8} 639 639 \caption{Resolution of the transverse energy of reconstructed jets $E_T^\textrm{rec}$ as a function of the transverse energy of the closest jet of generator-level particles $E_T^\textrm{MC}$. The maximum separation between the reconstructed and \textsc{mc} jets is $\Delta R= 0.25$. Pink line is the fit result for comparison to the \textsc{cms} resolution~\citep{bib:cmsjetresolution}, in blue.} 640 640 \label{fig:jetresol} … … 668 668 \begin{center} 669 669 %\includegraphics[width=\columnwidth]{resolutionETmis} 670 \includegraphics[width=\columnwidth]{fig 10}670 \includegraphics[width=\columnwidth]{fig9} 671 671 \caption{$\sigma(E^\textrm{miss}_{x})$ as a function on the scalar sum of all towers ($\Sigma E_T$) for $pp \rightarrow gg$ events.} 672 672 \label{fig:resolETmis} … … 732 732 \begin{center} 733 733 %\includegraphics[width=\columnwidth]{Detector_Delphes_2b} 734 \includegraphics[width=\columnwidth]{fig1 1}734 \includegraphics[width=\columnwidth]{fig10} 735 735 \caption{Layout of the generic detector geometry assumed in \textsc{Delphes}. Open 3D-view of the detector with solid volumes. Same colour codes as for Fig.~\ref{fig:GenDet3} are applied. Additional forward detectors are not depicted.} 736 736 \label{fig:GenDet2} … … 754 754 %%\includegraphics[width=\columnwidth]{Events_Delphes_1} 755 755 %\includegraphics[width=\columnwidth]{DisplayWt} 756 \includegraphics[width=\columnwidth]{fig1 2}756 \includegraphics[width=\columnwidth]{fig11} 757 757 \caption{Example of $pp(\gamma p \rightarrow Wt)pY$ event display in different orientations, with $t \rightarrow Wb$. 758 758 One $W$ boson decays into a $\mu \nu_\mu$ pair and the second one into a $e \nu_e$ pair. … … 771 771 %%\includegraphics[width=\columnwidth]{Events_Delphes_1} 772 772 %\includegraphics[width=\columnwidth]{Displayppgg} 773 \includegraphics[width=\columnwidth]{fig1 3}773 \includegraphics[width=\columnwidth]{fig12} 774 774 \caption{Example of inclusive gluon pair production $pp \rightarrow ggX$. Many jets are visible in the event, in particular along the beam axis. Two muons (in blue) are produced and the missing transverse energy is significant in this event (grey vector).} 775 775 \label{fig:gg} … … 819 819 \bibitem{bib:Delphes} \textsc{Delphes}, \href{http://www.fynu.ucl.ac.be/delphes.html}{www.fynu.ucl.ac.be/delphes.html} 820 820 %hepforge: 821 \bibitem{bib:stdhep} L.A. Garren, M. Fischler, \ \ \href{http://cepa.fnal.gov/psm/stdhep/c++}{cepa.fnal.gov/psm/stdhep/c++}\bibitem{bib:hepmc} M. Dobbs and J.B. Hansen, \textbf{Comput. Phys. Commun.} \href{http://dx.doi.org/10.1016/S0010-4655(00)00189-2}{134 (2001) 41}.821 \bibitem{bib:stdhep} L.A. Garren, M. Fischler, \href{http://cepa.fnal.gov/psm/stdhep/c++}{cepa.fnal.gov/psm/stdhep/c++}\bibitem{bib:hepmc} M. Dobbs and J.B. Hansen, \textbf{Comput. Phys. Commun.} \href{http://dx.doi.org/10.1016/S0010-4655(00)00189-2}{134 (2001) 41}. 822 822 \bibitem{bib:lhe} J. Alwall, et al., \textbf{Comput. Phys. Commun.} \href{http://dx.doi.org/10.1016/j.cpc.2006.11.010}{176:300-304,2007}. 823 823 \bibitem{bib:Root} %\textsc{Root}, \textit{An Object Oriented Data Analysis Framework}, … … 825 825 \bibitem{bib:ExRootAnalysis} %\textit{The} \textsc{ExRootAnalysis} \textit{analysis steering utility}, 826 826 P. Demin, (2006), unpublished. Now part of \textsc{MadGraph/MadEvent}. 827 \bibitem{bib:cmsjetresolution} The CMS Collaboration, \textbf{CERN/LHCC} \ \ \href{http://documents.cern.ch/cgi-bin/setlink?base=lhcc&categ=public&id=lhcc-2006-001}{2006-001}.827 \bibitem{bib:cmsjetresolution} The CMS Collaboration, \textbf{CERN/LHCC} \href{http://documents.cern.ch/cgi-bin/setlink?base=lhcc&categ=public&id=lhcc-2006-001}{2006-001}. 828 828 \bibitem{bib:ATLASresolution} The ATLAS Collaboration, \textbf{CERN-OPEN} 2008-020, arXiv:\href{http://arxiv.org/abs/arxiv:0901.0512}{0901.0512v1}[hep-ex]. 829 829 \bibitem{bib:Hector} %\textsc{Hector}, \textit{a fast simulator for the transport of particles in beamlines}, … … 1070 1070 # In case FROG event display allowed 1071 1071 NEvents_Frog 100 1072 # Number of events to process1073 NEvents -1 // -1 means 'all'1074 1072 1075 1073 # input PDG tables … … 1079 1077 1080 1078 In general, energies, momenta and masses are expressed in GeV, GeV$/c$, GeV$/c^2$ respectively, and magnetic fields in T. 1081 Geometrical extension are often referred in terms of pseudorapidity $\eta$, as the detectors are supposed to be symmetric in $\phi$. The number of events to run is alsoincluded in the detector card (\texttt{NEvents}).1079 Geometrical extension are often referred in terms of pseudorapidity $\eta$, as the detectors are supposed to be symmetric in $\phi$. From version 1.8 onwards, the number of events to run will also be included in the detector card (\texttt{NEvents}). 1082 1080 1083 1081 \item{\bf The trigger card }
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