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Changeset 520 in svn for trunk


Ignore:
Timestamp:
Jul 27, 2009, 11:20:18 PM (15 years ago)
Author:
Xavier Rouby
Message:

update footnotes VFDs

Location:
trunk/paper
Files:
4 edited

Legend:

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  • trunk/paper/CommPhysComp/notes.tex

    r517 r520  
    383383While neutral particles propagate along a straight line to the \textsc{zdc}, a dedicated simulation of the transport of charged particles is needed for \textsc{rp220} and \textsc{fp420}. This fast simulation uses the \textsc{Hector} software~\citep{bib:Hector}, which includes the chromaticity effects and the geometrical aperture of the beamline elements of any arbitrary collider.
    384384
    385 Forward taggers are able to measure the hit positions ($x,y$) and angles ($\theta_x,\theta_y$) in the transverse plane at the location of the detector ($s$ meters away from the \textsc{ip}), as well as the time-of-flight\footnote{It should be noted that for both \textsc{cms} and \textsc{atlas} experiments, the taggers located at $220$~m are not able to measure the time-of-flight, contrary to \textsc{fp}420 detectors.} ($t$). Out of these the particle energy ($E$) and the momentum transfer it underwent during the interaction ($q^2$) can be reconstructed\footnote{The reconstruction of $E$ and $q^2$ are not implemeted in \textsc{Delphes} but can be performed at the analysis level.}.
     385Forward taggers are able to measure the hit positions ($x,y$) and angles ($\theta_x,\theta_y$) in the transverse plane at the location of the detector ($s$ meters away from the \textsc{ip}), as well as the time-of-flight\footnote{It should be noted that for both \textsc{cms} and \textsc{atlas} experiments, the taggers located at $220$~m are not able to measure the time-of-flight, contrary to \textsc{fp}420 detectors.} ($t$). Out of these the particle energy ($E$) and the momentum transfer it underwent during the interaction ($q^2$) can be reconstructed\footnote{The reconstruction of $E$ and $q^2$ are not implemeted in \textsc{Delphes} but can be performed at the analysis level.}. The time-of-flight measurement can be smeared with a Gaussian distribution (default value\footnote{\texttt{[code] } The resolution is defined by the \texttt{RP220\_T\_resolution} and \texttt{RP420\_T\_resolution} parameters in the detector card.} $\sigma_t = 0~\textrm{s}$).
    386386
    387387
  • trunk/paper/notes.tex

    r517 r520  
    3838
    3939\title{\textsc{Delphes}, a framework for fast simulation \\of a generic collider experiment}
    40 \author{S. Ovyn$^*$ and X. Rouby$^\textrm{a}$\\
    41         \small{Center for Particle Physics and Phenomenology (CP3)}\\
     40\author{S. Ovyn$^*$\\
     41        \small{Center for Particle Physics and Phenomenology,}
    4242        \small{Universit\'e catholique de Louvain}\\
    43         \small{B-1348 Louvain-la-Neuve, Belgium}\\ \\
    44         \texttt{severine.ovyn@uclouvain.be, xavier.rouby@cern.ch} \\
     43        \small{B-1348 Louvain-la-Neuve, Belgium}\\
     44        \texttt{severine.ovyn@uclouvain.be} \\ \\
     45X. Rouby\\
     46        \small{Physikalisches Institut,}
     47        \small{Albert-Ludwigs-Universit\"at Freiburg}\\
     48        \small{B-79104 Freiburg-im-Breisgau, Germany}\\
     49        \texttt{xavier.rouby@cern.ch} \\
    4550}
    4651\date{}
     
    7681\end{abstract}
    7782\small{$^{*}$ Corresponding author: +32.10.47.32.29.}
    78 \small{$^\textrm{a}$ Now in Physikalisches Institut, Albert-Ludwigs-Universit\"at Freiburg}
    7983]
    8084%\saythanks
     
    343347While neutral particles propagate along a straight line to the \textsc{zdc}, a dedicated simulation of the transport of charged particles is needed for \textsc{rp220} and \textsc{fp420}. This fast simulation uses the \textsc{Hector} software~\cite{bib:Hector}, which includes the chromaticity effects and the geometrical aperture of the beamline elements of any arbitrary collider.
    344348
    345 Forward taggers are able to measure the hit positions ($x,y$) and angles ($\theta_x,\theta_y$) in the transverse plane at the location of the detector ($s$ meters away from the \textsc{ip}), as well as the time-of-flight\footnote{It should be noted that for both \textsc{cms} and \textsc{atlas} experiments, the taggers located at $220$~m are not able to measure the time-of-flight, contrary to \textsc{fp}420 detectors.} ($t$). Out of these the particle energy ($E$) and the momentum transfer it underwent during the interaction ($q^2$) can be reconstructed\footnote{The reconstruction of $E$ and $q^2$ are not implemeted in \textsc{Delphes} but can be performed at the analysis level.}.
     349Forward taggers are able to measure the hit positions ($x,y$) and angles ($\theta_x,\theta_y$) in the transverse plane at the location of the detector ($s$ meters away from the \textsc{ip}), as well as the time-of-flight\footnote{It should be noted that for both \textsc{cms} and \textsc{atlas} experiments, the taggers located at $220$~m are not able to measure the time-of-flight, contrary to \textsc{fp}420 detectors.} ($t$). Out of these the particle energy ($E$) and the momentum transfer it underwent during the interaction ($q^2$) can be reconstructed\footnote{The reconstruction of $E$ and $q^2$ are not implemeted in \textsc{Delphes} but can be performed at the analysis level.}. The time-of-flight measurement can be smeared with a Gaussian distribution (default value\footnote{\texttt{[code] } The resolution is defined by the \texttt{RP220\_T\_resolution} and \texttt{RP420\_T\_resolution} parameters in the detector card.} $\sigma_t = 0~\textrm{s}$).
    346350
    347351
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