[HTML][HTML] Effect of heavy-quark energy loss on the muon differential production cross section in Pb–Pb collisions at sNN= 5.5 TeV

ZC Del Valle, A Dainese, HT Ding, GM Garcia… - Physics Letters B, 2008 - Elsevier
ZC Del Valle, A Dainese, HT Ding, GM Garcia, DC Zhou
Physics Letters B, 2008Elsevier
We study the nuclear modification factors RAA and RCP of the high transverse momentum
(5< pt< 60 GeV/c) distribution of muons in Pb–Pb collisions at LHC energies. We consider
two pseudo-rapidity ranges covered by the LHC experiments:| η|< 2.5 and 2.5< η< 4. Muons
from semi-leptonic decays of heavy quarks (c and b) and from leptonic decays of weak
gauge bosons (W and Z) are the main contributions to the muon pt distribution above a few
GeV/c. We compute the heavy quark contributions using available pQCD-based programs …
We study the nuclear modification factors RAA and RCP of the high transverse momentum (5<pt<60 GeV/c) distribution of muons in Pb–Pb collisions at LHC energies. We consider two pseudo-rapidity ranges covered by the LHC experiments: |η|<2.5 and 2.5<η<4. Muons from semi-leptonic decays of heavy quarks (c and b) and from leptonic decays of weak gauge bosons (W and Z) are the main contributions to the muon pt distribution above a few GeV/c. We compute the heavy quark contributions using available pQCD-based programs. We include the nuclear shadowing modification of the parton distribution functions and the in-medium radiative energy loss for heavy quarks, using the mass-dependent BDMPS quenching weights. Muons from W and Z leptonic decays, that dominate the yield at high pt, can be used as a medium-blind reference to observe the medium-induced suppression of beauty quarks.
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