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Open heavy flavour production via semi-leptonic decay muons in lead lead collisions at $\sqrt{s_nn}$ = 2.76$ TeV with the ATLAS detector at the LHC

Measurements of heavy quark production and suppression in ultra-relativistic nuclear collisions probe the interactions of heavy quarks with the hot, dense medium created in the collisions. ATLAS has measured heavy quark production in $\sqrtsnn = 2.76$ \TeV \PbPb collisions via semi-leptonic decays o...

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Autor principal: Chen, Yujiao
Lenguaje:eng
Publicado: 2012
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysa.2012.12.011
http://cds.cern.ch/record/1482016
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author Chen, Yujiao
author_facet Chen, Yujiao
author_sort Chen, Yujiao
collection CERN
description Measurements of heavy quark production and suppression in ultra-relativistic nuclear collisions probe the interactions of heavy quarks with the hot, dense medium created in the collisions. ATLAS has measured heavy quark production in $\sqrtsnn = 2.76$ \TeV \PbPb collisions via semi-leptonic decays of open heavy flavour hadrons to muons. Results are presented for the per-event muon yield as a function of muon transverse momentum, \pT, over the range of $4 < \pT < 14$ \GeV. The centrality dependence of the muon yields is characterized by the "central to peripheral" ratio, \Rcp. Muon production is suppressed by approximately a factor of two in central collisions relative to peripheral collisions. Within the experimental errors, the observed suppression is independent of muon \pT\ for all centralities.
id cern-1482016
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2012
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spelling cern-14820162019-09-30T06:29:59Zdoi:10.1016/j.nuclphysa.2012.12.011http://cds.cern.ch/record/1482016engChen, YujiaoOpen heavy flavour production via semi-leptonic decay muons in lead lead collisions at $\sqrt{s_nn}$ = 2.76$ TeV with the ATLAS detector at the LHCNuclear Physics - Experimentnucl-exNuclear Physics - ExperimentMeasurements of heavy quark production and suppression in ultra-relativistic nuclear collisions probe the interactions of heavy quarks with the hot, dense medium created in the collisions. ATLAS has measured heavy quark production in $\sqrtsnn = 2.76$ \TeV \PbPb collisions via semi-leptonic decays of open heavy flavour hadrons to muons. Results are presented for the per-event muon yield as a function of muon transverse momentum, \pT, over the range of $4 < \pT < 14$ \GeV. The centrality dependence of the muon yields is characterized by the "central to peripheral" ratio, \Rcp. Muon production is suppressed by approximately a factor of two in central collisions relative to peripheral collisions. Within the experimental errors, the observed suppression is independent of muon \pT\ for all centralities.Measurements of heavy quark production and suppression in ultra-relativistic nuclear collisions probe the interactions of heavy quarks with the hot, dense medium created in the collisions. ATLAS has measured heavy quark production in $\sqrt{s_{NN}}$=2.76 TeV Pb + Pb collisions via semi-leptonic decays of open heavy flavour hadrons to muons. Results are presented for the per-event muon yield as a function of muon transverse momentum, p_T, over the range of 4<p_T<14 GeV. The centrality dependence of the muon yields is characterized by the ''central to peripheral'' ratio, R_C_P. Using this measure, muon production from heavy quark decays is found to be suppressed by a centrality-dependent factor that increases smoothly from peripheral to central collisions. Muon production is suppressed by approximately a factor of two in central collisions relative to peripheral collisions. Within the experimental errors, the observed suppression is independent of muon p_T for all centralities.Measurements of heavy quark production and suppression in ultra-relativistic nuclear collisions probe the interactions of heavy quarks with the hot, dense medium created in the collisions. ATLAS has measured heavy quark production in $\sqrtsnn = 2.76$ \TeV \PbPb collisions via semi-leptonic decays of open heavy flavour hadrons to muons. Results are presented for the per-event muon yield as a function of muon transverse momentum, \pT, over the range of $4 < \pT < 14$ \GeV. The centrality dependence of the muon yields is characterized by the "central to peripheral" ratio, \Rcp. Muon production is suppressed by approximately a factor of two in central collisions relative to peripheral collisions. Within the experimental errors, the observed suppression is independent of muon \pT for all centralities.arXiv:1209.6282oai:cds.cern.ch:14820162012-09-28
spellingShingle Nuclear Physics - Experiment
nucl-ex
Nuclear Physics - Experiment
Chen, Yujiao
Open heavy flavour production via semi-leptonic decay muons in lead lead collisions at $\sqrt{s_nn}$ = 2.76$ TeV with the ATLAS detector at the LHC
title Open heavy flavour production via semi-leptonic decay muons in lead lead collisions at $\sqrt{s_nn}$ = 2.76$ TeV with the ATLAS detector at the LHC
title_full Open heavy flavour production via semi-leptonic decay muons in lead lead collisions at $\sqrt{s_nn}$ = 2.76$ TeV with the ATLAS detector at the LHC
title_fullStr Open heavy flavour production via semi-leptonic decay muons in lead lead collisions at $\sqrt{s_nn}$ = 2.76$ TeV with the ATLAS detector at the LHC
title_full_unstemmed Open heavy flavour production via semi-leptonic decay muons in lead lead collisions at $\sqrt{s_nn}$ = 2.76$ TeV with the ATLAS detector at the LHC
title_short Open heavy flavour production via semi-leptonic decay muons in lead lead collisions at $\sqrt{s_nn}$ = 2.76$ TeV with the ATLAS detector at the LHC
title_sort open heavy flavour production via semi-leptonic decay muons in lead lead collisions at $\sqrt{s_nn}$ = 2.76$ tev with the atlas detector at the lhc
topic Nuclear Physics - Experiment
nucl-ex
Nuclear Physics - Experiment
url https://dx.doi.org/10.1016/j.nuclphysa.2012.12.011
http://cds.cern.ch/record/1482016
work_keys_str_mv AT chenyujiao openheavyflavourproductionviasemileptonicdecaymuonsinleadleadcollisionsatsqrtsnn276tevwiththeatlasdetectoratthelhc