Non-Equilibrium Trace Anomaly And Bulk Viscosity in Heavy Ion Collisions From Kinetic Theory

TL;DR

This paper studies the non-equilibrium behavior and transport properties of a relativistic gas with different quantum statistics during heavy-ion collisions, revealing complex time evolution of trace anomaly and bulk viscosity.

Contribution

It provides a detailed analysis of the time evolution of non-equilibrium quantities in a relativistic gas using kinetic theory, highlighting the effects of quantum statistics and initial conditions.

Findings

Non-monotonic time dependence of trace anomaly with a maximum and dip.

Sensitivity of bulk pressure to particle statistics and initial chemical potential.

Convergence of scaled bulk pressure and pressure anisotropy at late times.

Abstract

We investigate the far-from-equilibrium dynamics and transport properties of a relativistic massive gas obeying Maxwell-Boltzmann (MB), Bose-Einstein (BE), and Fermi-Dirac (FD) statistics undergoing a boost-invariant Bjorken expansion. We solve the relativistic Boltzmann equation in the relaxation-time approximation (RTA) using the method of moments. We focus on the time evolution of the trace of the energy-momentum tensor $\Theta^{\mu}{}_{\mu}$ and the bulk viscous pressure $\Pi$, which are key diagnostics of conformal-symmetry breaking in the rapidly evolving fireball created in heavy-ion collisions. We find that the non-equilibrium quantity $\Theta^{\mu}{}_{\mu}/T^{4}$ exhibits a non-monotonic time dependence, with a local maximum at early times and a pronounced dip around the characteristic relaxation time scale $\tau_{R}$. We further show that the scaled bulk pressure $\Pi/P_{0}$, where $P_{0}$ denotes the isotropic equilibrium pressure, depends sensitively on the particle statistics. In addition, increasing the initial chemical potential enhances the magnitudes of both $\Pi$ and $\Theta^{\mu}{}_{\mu}/T^{4}$. Finally, by initializing the system with random non-equilibrium configurations, we demonstrate that the evolution of the scaled bulk pressure and the pressure anisotropy converges to a common late-time solution.