Abstract

The pre-equilibrium evolution of a quark-gluon plasma produced in a heavy-ion collision is studied in the framework of kinetic theory. We discuss the approach to local thermal equilibrium, and the onset of hydrodynamics, in terms of a particular set of moments of the distribution function. These moments quantify the momentum anisotropies to a finer degree than the commonly used ratio of longitudinal to transverse pressures. They are found to be in direct correspondence with viscous corrections of hydrodynamics, and provide therefore an alternative measure of these corrections in terms of the distortion of the momentum distribution. As an application, we study the evolution of these moments by solving the Boltzmann equation for a boost invariant expanding system, first analytically in the relaxation time approximation, and then numerically for a quark-gluon plasma with a collision kernel given by leading order 2 ↔ 2 QCD matrix elements in the small angle approximation.

Highlights

  • Possible to recast the solution of the Boltzmann equation in terms of an infinite hierarchy of equations for a particular set of moments of the distribution function

  • We study the evolution of these moments by solving the Boltzmann equation for a boost invariant expanding system, first analytically in the relaxation time approximation, and numerically for a quark-gluon plasma with a collision kernel given by leading order 2 ↔ 2 QCD matrix elements in the small angle approximation

  • Near the hydrodynamic regime, these moments are in correspondence to the viscous corrections that emerge from a gradient expansion

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Summary

Formulation of moments in expanding systems

After a brief review of the main features of expanding boost invariant systems, we define a set of moments of the distribution function that are suited to the. Near the hydrodynamic regime, these moments are in correspondence to the viscous corrections that emerge from a gradient expansion

Kinetic theory in a boost invariant expanding system
The moments Ln in the hydrodynamic regime
Evolution of the Ln moments in expanding systems
Relaxation time approximation
L2L4 4 L23
Quark-gluon system with small angle approximation
Summary and conclusions
A Contraction of irreducible tensors and Legendre polynomials
B Hydrodynamics with a with non-zero chemical potential
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