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$\gamma \gamma \rightarrow \ell^{+} \ell^{-}$ and $\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$ at CMS

Exclusive dilepton events are characterized by the presence of two back-to-back leptons, and no other detector activity above threshold. In $pp$ collisions in the CMS experiment, this signature can result from two-photon interactions ($\gamma \gamma \rightarrow \ell^{+}\ell^{-}$) or $\Upsilon$ photo...

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Autor principal: Hollar, J
Lenguaje:eng
Publicado: 2008
Materias:
Acceso en línea:http://cds.cern.ch/record/1110511
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author Hollar, J
author_facet Hollar, J
author_sort Hollar, J
collection CERN
description Exclusive dilepton events are characterized by the presence of two back-to-back leptons, and no other detector activity above threshold. In $pp$ collisions in the CMS experiment, this signature can result from two-photon interactions ($\gamma \gamma \rightarrow \ell^{+}\ell^{-}$) or $\Upsilon$ photoproduction ($\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$). In the early data from the LHC, these events will provide a calibration sample for luminosity and lepton reconstruction studies, and allow studies of diffraction and QCD.
id cern-1110511
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2008
record_format invenio
spelling cern-11105112019-09-30T06:29:59Zhttp://cds.cern.ch/record/1110511engHollar, J$\gamma \gamma \rightarrow \ell^{+} \ell^{-}$ and $\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$ at CMSDetectors and Experimental TechniquesExclusive dilepton events are characterized by the presence of two back-to-back leptons, and no other detector activity above threshold. In $pp$ collisions in the CMS experiment, this signature can result from two-photon interactions ($\gamma \gamma \rightarrow \ell^{+}\ell^{-}$) or $\Upsilon$ photoproduction ($\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$). In the early data from the LHC, these events will provide a calibration sample for luminosity and lepton reconstruction studies, and allow studies of diffraction and QCD.CMS-CR-2008-026oai:cds.cern.ch:11105112008-06-03
spellingShingle Detectors and Experimental Techniques
Hollar, J
$\gamma \gamma \rightarrow \ell^{+} \ell^{-}$ and $\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$ at CMS
title $\gamma \gamma \rightarrow \ell^{+} \ell^{-}$ and $\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$ at CMS
title_full $\gamma \gamma \rightarrow \ell^{+} \ell^{-}$ and $\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$ at CMS
title_fullStr $\gamma \gamma \rightarrow \ell^{+} \ell^{-}$ and $\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$ at CMS
title_full_unstemmed $\gamma \gamma \rightarrow \ell^{+} \ell^{-}$ and $\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$ at CMS
title_short $\gamma \gamma \rightarrow \ell^{+} \ell^{-}$ and $\gamma p \rightarrow \Upsilon p \rightarrow \ell^{+} \ell^{-} p$ at CMS
title_sort $\gamma \gamma \rightarrow \ell^{+} \ell^{-}$ and $\gamma p \rightarrow \upsilon p \rightarrow \ell^{+} \ell^{-} p$ at cms
topic Detectors and Experimental Techniques
url http://cds.cern.ch/record/1110511
work_keys_str_mv AT hollarj gammagammarightarrowellellandgammaprightarrowupsilonprightarrowellellpatcms