Turbulent thermalization process in heavy-ion collisions at ultrarelativistic energies

被引:184
|
作者
Berges, J. [1 ,2 ]
Boguslavski, K. [1 ]
Schlichting, S. [3 ]
Venugopalan, R. [3 ]
机构
[1] Heidelberg Univ, Inst Theoret Phys, D-69120 Heidelberg, Germany
[2] GSI Helmholtzzentrum Schwerionenforsch GmbH, ExtreMe Matter Inst EMMI, D-64291 Darmstadt, Germany
[3] Brookhaven Natl Lab, Dept Phys, Upton, NY 11973 USA
来源
PHYSICAL REVIEW D | 2014年 / 89卷 / 07期
关键词
COLOR GLASS CONDENSATE; QUARK-GLUON PLASMA;
D O I
10.1103/PhysRevD.89.074011
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The nonequilibrium evolution of heavy-ion collisions is studied in the limit of weak coupling at very high energy employing lattice simulations of the classical Yang-Mills equations. Performing the largest classical-statistical simulations to date, we find that the dynamics of the longitudinally expanding plasma becomes independent of the details of the initial conditions. After a transient regime dominated by plasma instabilities and free streaming, the subsequent space-time evolution is governed by a nonthermal fixed point, where the system exhibits the self-similar dynamics characteristic of wave turbulence. This allows us to distinguish between different kinetic scenarios in the classical regime. Within the accuracy of our simulations, the scaling behavior found is consistent with the "bottom-up" thermalization scenario [ R. Baier, A. H. Mueller, D. Schiff, and D. T. Son, Phys. Lett. B 502, 51 ( 2001)].
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页数:10
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