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arXiv 2210.03076hep-ph
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用Gribov-Zwanziger action估计重夸克的扩散系数

Estimation of the diffusion coefficient of Heavy Quarks in light of Gribov-Zwanziger action

Sadaf Madni, Arghya Mukherjee, Aritra Bandyopadhyay, Najmul Haque

摘要:

重夸克动量扩散系数($κ$)是重夸克动力学朗之万描述的重要组成部分。在与重离子碰撞现象相关的温度范围内,$κ$的晶格估计与硬热环(HTL)微扰理论的首阶(LO)结果之间存在很大差异.此外,在次领先阶(NLO)微扰分析的收敛性差的迹象,促使了几种方法的发展,将非微扰效应的重夸克现象学。在这项工作中,我们估计重夸克扩散系数的Gribov-Zwanziger处方的基础上。在这个框架中,胶子传播子依赖于依赖于温度的Gribov质量参数,该参数已从单圈能隙方程自洽地获得。在分析中对这种修正的胶子传播子进行了解释,在模型不确定性的范围内,我们发现它与现有的$κ$的格点估计有着合理的一致性。

英文摘要:

The heavy quark momentum diffusion coefficient ($κ$) is one of the most essential ingredients for the Langevin description of heavy quark dynamics. In the temperature regime relevant to the heavy ion collision phenomenology, a substantial difference exists between the lattice estimations of $κ$ and the corresponding leading order (LO) result from the hard thermal loop (HTL) perturbation theory. Moreover, the indication of poor convergence in the next-to-leading order (NLO) perturbative analysis has motivated the development of several approaches to incorporate the non-perturbative effects in the heavy quark phenomenology. In this work, we estimate the heavy quark diffusion coefficient based on the Gribov-Zwanziger prescription. In this framework, the gluon propagator depends on the temperature-dependent Gribov mass parameter, which has been obtained self-consistently from the one-loop gap equation. Incorporating this modified gluon propagator in the analysis, we find a reasonable agreement with the existing lattice estimations of $κ$ within the model uncertainties.

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