Quarkonium Suppression from Coherent Energy Loss in Fixed-Target Experiments Using LHC Beams
Quarkonium production in proton-nucleus collisions is a powerful tool to disentangle cold nuclear matter effects. A model based on coherent energy loss is able to explain the available quarkonium suppression data in a broad range of rapidities, from fixed-target to collider energies, suggesting coh...
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2015-01-01
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Series: | Advances in High Energy Physics |
Online Access: | http://dx.doi.org/10.1155/2015/961951 |
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doaj-9e234e8b831149d1ab5ce94488d10df12020-11-24T21:35:24ZengHindawi LimitedAdvances in High Energy Physics1687-73571687-73652015-01-01201510.1155/2015/961951961951Quarkonium Suppression from Coherent Energy Loss in Fixed-Target Experiments Using LHC BeamsFrançois Arleo0Stéphane Peigné1Laboratoire Leprince-Ringuet (LLR), École Polytechnique, CNRS/IN2P3, 91128 Palaiseau, FranceSUBATECH, UMR 6457, Université de Nantes, Ecole des Mines de Nantes, IN2P3/CNRS, 4 rue Alfred Kastler, 44307 Nantes Cedex 3, FranceQuarkonium production in proton-nucleus collisions is a powerful tool to disentangle cold nuclear matter effects. A model based on coherent energy loss is able to explain the available quarkonium suppression data in a broad range of rapidities, from fixed-target to collider energies, suggesting coherent energy loss in cold nuclear matter to be the dominant effect in quarkonium suppression in p-A collisions. This could be further tested in a high-energy fixed-target experiment using a proton or nucleus beam. The nuclear modification factors of J/ψ and Υ as a function of rapidity are computed in p-A collisions at s=114.6 GeV, and in p-Pb and Pb-Pb collisions at s=72 GeV. These center-of-mass energies correspond to the collision on fixed-target nuclei of 7 TeV protons and 2.76 TeV (per nucleon) lead nuclei available at the LHC.http://dx.doi.org/10.1155/2015/961951 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
François Arleo Stéphane Peigné |
spellingShingle |
François Arleo Stéphane Peigné Quarkonium Suppression from Coherent Energy Loss in Fixed-Target Experiments Using LHC Beams Advances in High Energy Physics |
author_facet |
François Arleo Stéphane Peigné |
author_sort |
François Arleo |
title |
Quarkonium Suppression from Coherent Energy Loss in Fixed-Target Experiments Using LHC Beams |
title_short |
Quarkonium Suppression from Coherent Energy Loss in Fixed-Target Experiments Using LHC Beams |
title_full |
Quarkonium Suppression from Coherent Energy Loss in Fixed-Target Experiments Using LHC Beams |
title_fullStr |
Quarkonium Suppression from Coherent Energy Loss in Fixed-Target Experiments Using LHC Beams |
title_full_unstemmed |
Quarkonium Suppression from Coherent Energy Loss in Fixed-Target Experiments Using LHC Beams |
title_sort |
quarkonium suppression from coherent energy loss in fixed-target experiments using lhc beams |
publisher |
Hindawi Limited |
series |
Advances in High Energy Physics |
issn |
1687-7357 1687-7365 |
publishDate |
2015-01-01 |
description |
Quarkonium production in proton-nucleus collisions is a powerful tool to disentangle cold nuclear matter effects. A model based on coherent energy loss is able to explain the available quarkonium suppression data in a broad range of rapidities, from fixed-target to collider energies, suggesting coherent energy loss in cold nuclear matter to be the dominant effect in quarkonium suppression in p-A collisions. This could be further tested in a high-energy fixed-target experiment using a proton or nucleus beam. The nuclear modification factors of J/ψ and Υ as a function of rapidity are computed in p-A collisions at s=114.6 GeV, and in p-Pb and Pb-Pb collisions at s=72 GeV. These center-of-mass energies correspond to the collision on fixed-target nuclei of 7 TeV protons and 2.76 TeV (per nucleon) lead nuclei available at the LHC. |
url |
http://dx.doi.org/10.1155/2015/961951 |
work_keys_str_mv |
AT francoisarleo quarkoniumsuppressionfromcoherentenergylossinfixedtargetexperimentsusinglhcbeams AT stephanepeigne quarkoniumsuppressionfromcoherentenergylossinfixedtargetexperimentsusinglhcbeams |
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1725945152593199104 |