Intermediate mass dileptons as pre-equilibrium probes in heavy ion collisions
Drell-Yan process
heavy ion: scattering
[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]
Nuclear Theory
dilepton: production
dilepton: mass
QC1-999
density: ratio
FOS: Physical sciences
anisotropy
[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]
01 natural sciences
7. Clean energy
High Energy Physics - Experiment
Nuclear Theory (nucl-th)
High Energy Physics - Experiment (hep-ex)
High Energy Physics - Phenomenology (hep-ph)
quantum chromodynamics
0103 physical sciences
[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]
quark antiquark: annihilation
Nuclear Experiment (nucl-ex)
Nuclear Experiment
background
Physics
nucleus nucleus: scattering
quark: momentum spectrum
heavy quark: semileptonic decay
High Energy Physics - Phenomenology
[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]
viscosity: density
entropy: density
DOI:
10.1016/j.physletb.2021.136626
Publication Date:
2021-09-06T11:51:44Z
AUTHORS (5)
ABSTRACT
The production of dileptons with an invariant mass in the range 1 GeV < M < 5 GeV provides unique insight into the approach to thermal equilibrium in ultrarelativistic nucleus-nucleus collisions. In this mass range, they are produced through the annihilation of quark-antiquark pairs in the early stages of the collision. They are sensitive to the anisotropy of the quark momentum distribution, and also to the quark abundance, which is expected to be underpopulated relative to thermal equilibrium. We take into account both effects based on recent theoretical developments in QCD kinetic theory, and study how the dilepton mass spectrum depends on the shear viscosity to entropy ratio that controls the equilibration time. We evaluate the background from the Drell-Yan process and argue that future detector developments can suppress the additional background from semileptonic decays of heavy flavors.<br/>10 pages, 7 figures; computation of the effective area is defined more rigorously, figures are updated accordingly. Added paragraph on page 7, discussing the impact of inhomogeneities in transverse density profile. Added paragraph in the conclusion on page 9, on fitting the invariant mass spectrum with a power function<br/>
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