Shear viscosity of a nonperturbative gluon plasma
Dmitri Antonov (CFIF, Lisbon)

TL;DR
This paper models the shear viscosity of a gluon plasma using nonperturbative stochastic fields, identifying corrections to the perturbative result and providing a unified approach to include nonperturbative effects.
Contribution
It introduces a model based on stochastic nonperturbative fields to evaluate shear viscosity, incorporating both perturbative and nonperturbative corrections within a unified formalism.
Findings
Nonperturbative excitations produce O(g^{10}) corrections.
Interference effects yield O(g^7) corrections.
The formalism reproduces known perturbative shear viscosity results.
Abstract
Shear viscosity is evaluated within a model of the gluon plasma, which is based entirely on the stochastic nonperturbative fields. We consider two types of excitations of such fields, which are characterized by the thermal correlation lengths ~ 1/(g^2 T) and ~ 1/(g^4 T), where "g" is the finite-temperature Yang-Mills coupling. Excitations of the first type correspond to the genuine nonperturbative stochastic Yang-Mills fields, while excitations of the second type mimic the known result for the shear viscosity of the perturbative Yang-Mills plasma. We show that the excitations of the first type produce only an O(g^{10})-correction to this result. Furthermore, a possible interference between excitations of these two types yields a somewhat larger, O(g^7), correction to the leading perturbative Yang-Mills result. Our analysis is based on the Fourier transformed Euclidean Kubo formula,…
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Taxonomy
TopicsHigh-Energy Particle Collisions Research · Quantum Chromodynamics and Particle Interactions · Cosmology and Gravitation Theories
