Heavy quark diffusion in perturbative QCD at next-to-leading order

Abstract

We compute the momentum diffusion coefficient of a nonrelativistic heavy quark in a hot QCD plasma, to next-to-leading order in the weak coupling expansion. Corrections arise at O(g); physically they represent interference between overlapping scatterings, as well as soft, electric scale ($p\sim gT$) gauge field physics, which we treat using the hard thermal loop (HTL) effective theory. In 3-color, 3-flavor QCD, the momentum diffusion constant of a fundamental representation heavy quark at NLO is $\kappa =\frac{16\pi }{3}{\alpha }_s^2{T}^3(\ln \frac{1}{g}+0.07428+1.8869g)$. The convergence of the weak coupling expansion is poor.

4 pages, 3 figures

Cited by in corpus (3)

• Nonperturbative Heavy-Quark Diffusion in the Quark-Gluon Plasma
• Heavy Quark Diffusion as a Probe of the Quark-Gluon Plasma
• Transport and spectral functions in high-temperature QCD