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Exclusive Photoproduction of $\Upsilon$ and lepton pairs in Pb-Pb at 5.5 TeV

Electromagnetic interactions of heavy-ions give access to a unique programme of photon-induced studies in the QCD and QED sectors of the Standard Model. On the one hand, exclusive photoproduction of bottomonium ($\gamma\,A \rightarrow \Upsilon\,A$, where the nucleus $A$ remains intact) offers a usef...

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Detalles Bibliográficos
Autores principales: d'Enterria, D, Kumar, V, Mohanty, A
Lenguaje:eng
Publicado: 2008
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysbps.2008.07.019
http://cds.cern.ch/record/1127312
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author d'Enterria, D
Kumar, V
Mohanty, A
author_facet d'Enterria, D
Kumar, V
Mohanty, A
author_sort d'Enterria, D
collection CERN
description Electromagnetic interactions of heavy-ions give access to a unique programme of photon-induced studies in the QCD and QED sectors of the Standard Model. On the one hand, exclusive photoproduction of bottomonium ($\gamma\,A \rightarrow \Upsilon\,A$, where the nucleus $A$ remains intact) offers a useful means to constrain the small-$x$ nuclear gluon density. On the other, two-photon exclusive dilepton production ($\gamma\,\gamma\rightarrow l^{+}\,l^{-}$) allows us to study QED at field-strengths close or above the Schwinger limit ($E_{\rm crit}\approx$~1.5 $\times$10$^{16}$~V/cm). We present full simulation studies of exclusively photo-produced $\Upsilon$ and high-mass dileptons in Pb-Pb collisions at the LHC.
id cern-1127312
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2008
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spelling cern-11273122019-09-30T06:29:59Zdoi:10.1016/j.nuclphysbps.2008.07.019http://cds.cern.ch/record/1127312engd'Enterria, DKumar, VMohanty, AExclusive Photoproduction of $\Upsilon$ and lepton pairs in Pb-Pb at 5.5 TeVDetectors and Experimental TechniquesElectromagnetic interactions of heavy-ions give access to a unique programme of photon-induced studies in the QCD and QED sectors of the Standard Model. On the one hand, exclusive photoproduction of bottomonium ($\gamma\,A \rightarrow \Upsilon\,A$, where the nucleus $A$ remains intact) offers a useful means to constrain the small-$x$ nuclear gluon density. On the other, two-photon exclusive dilepton production ($\gamma\,\gamma\rightarrow l^{+}\,l^{-}$) allows us to study QED at field-strengths close or above the Schwinger limit ($E_{\rm crit}\approx$~1.5 $\times$10$^{16}$~V/cm). We present full simulation studies of exclusively photo-produced $\Upsilon$ and high-mass dileptons in Pb-Pb collisions at the LHC.CMS-CR-2008-049oai:cds.cern.ch:11273122008-07-06
spellingShingle Detectors and Experimental Techniques
d'Enterria, D
Kumar, V
Mohanty, A
Exclusive Photoproduction of $\Upsilon$ and lepton pairs in Pb-Pb at 5.5 TeV
title Exclusive Photoproduction of $\Upsilon$ and lepton pairs in Pb-Pb at 5.5 TeV
title_full Exclusive Photoproduction of $\Upsilon$ and lepton pairs in Pb-Pb at 5.5 TeV
title_fullStr Exclusive Photoproduction of $\Upsilon$ and lepton pairs in Pb-Pb at 5.5 TeV
title_full_unstemmed Exclusive Photoproduction of $\Upsilon$ and lepton pairs in Pb-Pb at 5.5 TeV
title_short Exclusive Photoproduction of $\Upsilon$ and lepton pairs in Pb-Pb at 5.5 TeV
title_sort exclusive photoproduction of $\upsilon$ and lepton pairs in pb-pb at 5.5 tev
topic Detectors and Experimental Techniques
url https://dx.doi.org/10.1016/j.nuclphysbps.2008.07.019
http://cds.cern.ch/record/1127312
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