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arXiv 2402.06996nucl-thhep-ph
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强子共振气体与热质量准粒子模型的瞬态流体力学输运系数

Transport coefficients of transient hydrodynamics for the hadron-resonance gas and thermal-mass quasiparticle models

Gabriel S. Rocha, Gabriel S. Denicol

AI总结:

本文在强子共振气体和热质量准粒子模型中计算了二阶瞬态流体力学的全部输运系数,发现其归一化体粘滞系数与常用单组分气体结果存在定性差异,并验证了所得系数满足线性稳定性与因果性条件。

摘要:

我们在两种有效动力学理论模型中计算了二阶瞬态流体力学的全部输运系数:一种是强子共振气体,另一种是热质量经过调节以重现QCD热力学的准粒子模型。我们将相应结果与超相对论单组分气体的计算结果进行比较,后者被广泛用于重离子碰撞的流体力学模拟中。我们发现,与单组分气体的计算结果相比,这两种有效模型都表现出定性不同的归一化体粘滞系数。实际上,对于强子共振气体模型,有 $ζ/[τ_Π(\varepsilon_{0} + P_{0})] \simeq 16.91(1/3-c_{s}^{2})^{2}$;对于准粒子模型,有 $ζ/[τ_Π(\varepsilon_{0} + P_{0})] \simeq 5 (1/3-c_{s}^{2})$。在许多二阶输运系数中也观察到差异,特别是那些与体粘滞压强相关的系数。所导出的输运系数被证明与基本的线性稳定性和因果性条件一致。

英文摘要:

We calculate all transport coefficients of second order transient hydrodynamics in two effective kinetic theory models: a hadron-resonance gas and a quasiparticle model with thermal masses tuned to reproduce QCD thermodynamics. We compare the corresponding results with calculations for an ultrarelativistic single-component gas, that are widely employed in hydrodynamic simulations of heavy ion collisions. We find that both of these effective models display a qualitatively different normalized bulk viscosity, when compared to the calculation for the single-component gas. Indeed, $ζ/[τ_Π(\varepsilon_{0} + P_{0})] \simeq 16.91(1/3-c_{s}^{2})^{2}$, for the hadron-resonance gas model, and $ζ/[τ_Π(\varepsilon_{0} + P_{0})] \simeq 5 (1/3-c_{s}^{2})$ for the quasiparticle model. Differences are also observed for many second-order transport coefficients, specially those related to the bulk viscous pressure. The transport coefficients derived are shown to be consistent with fundamental linear stability and causality conditions.

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