Changeset 460 in svn for trunk/paper

Timestamp:

Jul 10, 2009, 10:49:17 AM (15 years ago)

Author:

Xavier Rouby

Message:

update + renumbering of figures according to the editor's scheme

Location:

trunk/paper/CommPhysComp

Files:

• enumitem.sty (added)
• figures/fig0.eps (added)
• figures/fig1.eps (modified) ( previous)
• figures/fig10.eps (modified) ( previous)
• figures/fig11.eps (modified) ( previous)
• figures/fig12.eps (modified) ( previous)
• figures/fig2.eps (modified) ( previous)
• figures/fig3.eps (modified) ( previous)
• figures/fig4.eps (modified) ( previous)
• figures/fig5.eps (modified) ( previous)
• figures/fig6.eps (modified) ( previous)
• figures/fig7.eps (modified) ( previous)
• figures/fig8.eps (modified) ( previous)
• figures/fig9.eps (modified) ( previous)
• notes.pdf (added)
• notes.tex (modified) (17 diffs)

trunk/paper/CommPhysComp/notes.tex

@@ -57 +57 @@
 \textit{Preprint:} \texttt{CP3-09-01}, \texttt{arXiv:0903.2225 [hep-ph]}\\ \\
 %\includegraphics[scale=0.8]{DelphesLogoSml}\\
-\includegraphics[scale=0.8]{fig1}\\
+\includegraphics[scale=0.8]{fig0}\\
 {\bf PROGRAM SUMMARY}\\
 \begin{small}
@@ -133 +133 @@
 \begin{center}
 %\includegraphics[scale=0.78]{FlowDelphes}
-\includegraphics[scale=0.78]{fig2}
+\includegraphics[scale=0.78]{fig1}
 \caption{Flow chart describing the principles behind \textsc{Delphes}. Event files coming from external Monte Carlo generators are read by a converter stage (top). 
 The kinematics variables of the final-state particles are then smeared according to the tunable subdetector resolutions. 
@@ -185 +185 @@
 \begin{center}
 %\includegraphics[width=\columnwidth]{Detector_Delphes_3}
-\includegraphics[width=\columnwidth]{fig3}
+\includegraphics[width=\columnwidth]{fig2}
 \caption{
 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}
 %\includegraphics[width=\columnwidth]{calosegmentation}
-\includegraphics[width=\columnwidth]{fig4}
-\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.}
+\includegraphics[width=\columnwidth]{fig3}
+\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.}
 \label{fig:calosegmentation}
 \end{center}
@@ -290 +290 @@
 \begin{center}
 %\includegraphics[width=\columnwidth]{fdets}
-\includegraphics[width=\columnwidth]{fig5}
+\includegraphics[width=\columnwidth]{fig4}
 \caption{Default location of the very forward detectors, including \textsc{zdc}, \textsc{rp220} and \textsc{fp420} in the \textsc{lhc} beamline. 
 Incoming (red) and outgoing (black) beams on one side of the interaction point ($s=0~\textrm{m}$). 
@@ -489 +489 @@
 \begin{center}
 %\includegraphics[width=0.6\columnwidth]{Tau}
-\includegraphics[width=0.6\columnwidth]{fig6}
+\includegraphics[width=0.6\columnwidth]{fig5}
 \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.}
 \label{h_WW_ss_cut1}
@@ -528 +528 @@
 \begin{center}
 %\includegraphics[width=\columnwidth]{Tau2}
-\includegraphics[width=\columnwidth]{fig7}
+\includegraphics[width=\columnwidth]{fig6}
 \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 $\ell = e, \mu, \tau$.
 Events generated with \textsc{MadGraph/MadEvent}~\citep{bib:mgme}.
@@ -547 +547 @@
 \begin{center}
 %\includegraphics[width=\columnwidth]{Tau1}
-\includegraphics[width=\columnwidth]{fig8}
+\includegraphics[width=\columnwidth]{fig7}
 \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}. 
 Histogram entries correspond to true $\tau$-jets, matched with generator-level data.}
@@ -636 +636 @@
 \begin{center}
 %\includegraphics[width=\columnwidth]{resolutionJet}
-\includegraphics[width=\columnwidth]{fig9}
+\includegraphics[width=\columnwidth]{fig8}
 \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.}
 \label{fig:jetresol}
@@ -668 +668 @@
 \begin{center}
 %\includegraphics[width=\columnwidth]{resolutionETmis}
-\includegraphics[width=\columnwidth]{fig10}
+\includegraphics[width=\columnwidth]{fig9}
 \caption{$\sigma(E^\textrm{miss}_{x})$ as a function on the scalar sum of all towers ($\Sigma E_T$) for $pp \rightarrow gg$ events.}
 \label{fig:resolETmis}
@@ -732 +732 @@
 \begin{center}
 %\includegraphics[width=\columnwidth]{Detector_Delphes_2b}
-\includegraphics[width=\columnwidth]{fig11}
+\includegraphics[width=\columnwidth]{fig10}
 \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.}
 \label{fig:GenDet2}
@@ -754 +754 @@
 %%\includegraphics[width=\columnwidth]{Events_Delphes_1}
 %\includegraphics[width=\columnwidth]{DisplayWt}
-\includegraphics[width=\columnwidth]{fig12}
+\includegraphics[width=\columnwidth]{fig11}
 \caption{Example of $pp(\gamma p \rightarrow Wt)pY$ event display in different orientations, with $t \rightarrow Wb$. 
 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}
 %\includegraphics[width=\columnwidth]{Displayppgg}
-\includegraphics[width=\columnwidth]{fig13}
+\includegraphics[width=\columnwidth]{fig12}
 \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).}
 \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}
 %hepforge:
-\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}.
+\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}.
 \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}.
 \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}, 
 P. Demin, (2006), unpublished. Now part of \textsc{MadGraph/MadEvent}.
-\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}.
+\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}.
 \bibitem{bib:ATLASresolution} The ATLAS Collaboration, \textbf{CERN-OPEN} 2008-020, arXiv:\href{http://arxiv.org/abs/arxiv:0901.0512}{0901.0512v1}[hep-ex].
 \bibitem{bib:Hector} %\textsc{Hector}, \textit{a fast simulator for the transport of particles in beamlines}, 
@@ -1070 +1070 @@
 # In case FROG event display allowed
 NEvents_Frog      100
-# Number of events to process
-NEvents           -1                    // -1 means 'all'
 
 # input PDG tables
@@ -1079 +1077 @@
 
 In general, energies, momenta and masses are expressed in GeV, GeV$/c$, GeV$/c^2$ respectively, and  magnetic fields in T.
-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 also included in the detector card (\texttt{NEvents}).
+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}).
  
 \item{\bf The trigger card }