Abstract

The bulk viscosity of thermalized QCD matter at temperatures above a few hundred MeV could be significantly influenced by charm quarks because their contribution arises four perturbative orders before purely gluonic effects. In an attempt to clarify the challenges of a lattice study, we determine the relevant imaginary-time correlator (of massive scalar densities) up to NLO in perturbation theory, and compare with existing data. We find discrepancies much larger than in the vector channel; this may hint, apart from the importance of taking a continuum limit, to larger non-perturbative effects in the scalar channel. We also recall how a transport peak related to the scalar density spectral function encodes non-perturbative information concerning the charm quark chemical equilibration rate close to equilibrium.

Highlights

  • The physical processes relevant for the bulk viscosity are those associated with the breaking of scale invariance

  • We recall how a transport peak related to the scalar density spectral function encodes non-perturbative information concerning the charm quark chemical equilibration rate close to equilibrium

  • The purpose of this paper has been to investigate the influence of a finite charm quark mass on a 2-point imaginary-time correlator in the so-called bulk channel, corresponding to the trace of the energy-momentum tensor in continuum QCD

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Summary

Physics background

The expectation value in eq (2.4) vanishes in the chiral limit Mi ≪ πT and, because of Boltzmann suppression, for large masses, Mi ≫ πT It can give a rather substantial contribution for Mi ∼ πT ; for temperatures relevant for heavy ion collision experiments, this could be the case with charm quarks [31]–[34], which have a mass Mc < MD0 = 1.86 GeV. If Γchem > ω, a hydrodynamical description applies and the heavy quark contribution should be added to the bulk viscosity. In each case the chemical equilibration rate Γchem is seen to be a fundamental quantity, whose non-perturbative determination as a function of the heavy quark mass would be more than welcome

Setup of the computation
Wick contractions
Infrared and ultraviolet regimes
Parameter choices
Normalization to a free correlator
Comparison with gluonic effects
Normalization to a reconstructed correlator
Conclusions
A Master sum-integrals
B Renormalization of the scalar channel correlator
M2 8π2 Ep2

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