Heavy quark diffusion coefficient in heavy-ion collisions via kinetic theory
arXiv:2303.12520 · doi:10.1103/PhysRevD.109.014025
Abstract
We compute the heavy quark momentum diffusion coefficient using QCD kinetic theory for a system going through bottom-up isotropization in the initial stages of a heavy ion collision. We find that the values of are within 30% from a thermal system at the same energy density. When matching for other quantities we observe considerably larger deviations. We also observe that the diffusion coefficient in the transverse direction is larger at high occupation numbers, whereas for an underoccupied system the longitudinal diffusion coefficient dominates. The behavior of the diffusion coefficient can be understood on a qualitative level based on the Debye mass and the effective temperature of soft modes . Our results for the kinetic evolution of in different directions can be used in phenomenological descriptions of heavy quark diffusion and quarkonium dynamics to include the impact of pre-equilibrium stages.
16 pages, 11 figures, v2: sec IV added including new figures, accepted for publication in PRD
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- The impact of glasma on heavy flavor azimuthal correlations and spectra
- Soft-gluon exchange matters: isotropic screening in QCD kinetic theory
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- Effect of Coriolis Force on Diffusion of D Meson
- Heavy quark diffusion coefficient during hydrodynamization -- non-equilibrium vs. equilibrium
- Anisotropy effects on heavy quark dynamics in Gribov modified gluon plasma