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Modelling Early Stages of Relativistic Heavy Ion Collisions: Coupling Relativistic Transport Theory to Decaying Color-electric Flux Tubes

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arxiv 1505.08081 v2 pith:PTKSUFXW submitted 2015-05-29 hep-ph nucl-th

classification hep-phnucl-th
keywords evolutionfieldproducedrelativisticsystemtimescolorearly
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abstract

In this study we model early times dynamics of the system produced in relativistic heavy ion collisions by an initial color electric field which then decays to a plasma by the Schwinger mechanism, coupling the dynamical evolution of the initial color field to the dynamics of the many particles system produced by the decay. The latter is described by relativistic kinetic theory in which we fix the ratio $\eta/s$ rather than insisting on specific microscopic processes. We study isotropization and thermalization of the system produced by the field decay for a static box and for a $1+1$D expanding geometry. We find that regardless of the viscosity of the produced plasma, the initial color electric field decays within $1$ fm/c; however in the case $\eta/s$ is large, oscillations of the field are effective along all the entire time evolution of the system, which affect the late times evolution of the ratio between longitudinal and transverse pressure. In case of small $\eta/s$ ($\eta/s\lesssim0.3$) we find $\tau_{isotropization}\approx 0.8$ fm/c and $\tau_{thermalization}\approx 1$ fm/c in agreement with the common lore of hydrodynamics. Moreover we have investigated the effect of turning from the relaxation time approximation to the Chapman-Enskog one: we find that this improvement affects mainly the early times evolution of the physical quantities, the effect being milder in the late times evolution.

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  1. Non-perturbative quark production and transport in the evolving glasma: the WAGASHI event generator

    hep-ph 2026-08 conditional novelty 6.0 of 10

    Schwinger pair production in the evolving glasma generates hundreds of quarks and antiquarks per unit rapidity in central Pb-Pb collisions, with momentum broadening and spin randomization before hydrodynamics begins.

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