Temperature dependence of the static quark diffusion coefficient
arXiv:2206.15471 · doi:10.1016/j.nuclphysa.2023.122721
Abstract
The energy loss pattern of a low momentum heavy quark in a deconfined quark-gluon plasma can be understood in terms of a Langevin description. In thermal equilibrium, the motion can then be parametrized in terms of a single heavy quark momentum diffusion coefficient kappa, which needs to be determined nonperturbatively. In this work, we study the temperature dependence of kappa for a static quark in a gluonic plasma, with a particular emphasis on the temperature range of interest for heavy ion collision experiments.
12 pages, 9 figures. The discussion section and the appendix substantially modified, two figures added, typos fixed
References in corpus (3)
Cited by in corpus (9)
- Quark Mass Dependence of Heavy Quark Diffusion Coefficient from Lattice QCD
- Heavy quark diffusion coefficient in heavy-ion collisions via kinetic theory
- Heavy Quark Momentum Broadening in a Non-Abelian Plasma away from Thermal Equilibrium
- Lattice -field correlators for heavy quarks
- Temperature Dependence of Heavy Quark Diffusion from (2+1)-flavor Lattice QCD
- Heavy quark diffusion and radiation at intermediate momentum
- Finite Temperature Quarkonia Spectral Functions in the Pseudoscalar Channel
- Production of leptons from decay of heavy-flavor hadrons in high-energy nuclear collisions
- Non-Markovian dynamics of bottomonia in the QGP