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Anisotropic hydrodynamics for conformal Gubser flow

机译:保形Gubser流的各向异性流体动力学

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摘要

In this proceedings contribution, we review the exact solution of the anisotropic hydrodynamics equations for a system subject to Gubser flow. For this purpose, we use the leading-order anisotropic hydrodynamics equations which assume that the distribution function is ellipsoidally symmetric in local-rest-frame momentum. We then prove that the SO(3)(q) symmetry in de Sitter space constrains the anisotropy tensor to be of spheroidal form with only one independent anisotropy parameter remaining. As a consequence, the exact solution reduces to the problem of solving two coupled non-linear differential equations. We show that, in the limit that the relaxation time goes to zero, one obtains Gubser's ideal hydrodynamic solution and, in the limit that the relaxation time goes to infinity, one obtains the exact free streaming solution obtained originally by Denicol et al. For finite relaxation time, we solve the equations numerically and compare to the exact solution of the relaxation-time-approximation Boltzmann equation subject to Gubser flow. Using this as our standard, we find that anisotropic hydrodynamics describes the spatio-temporal evolution of the system better than all currently known dissipative hydrodynamics approaches.
机译:在此程序贡献中,我们回顾了受Gubser流量影响的系统的各向异性流体动力学方程的精确解。为此,我们使用前向各向异性流体力学方程,该方程假设分布函数在局部静止框架动量中为椭圆对称。然后,我们证明de Sitter空间中的SO(3)(q)对称性将各向异性张量约束为球面形式,只剩下一个独立的各向异性参数。结果,精确解减少了求解两个耦合的非线性微分方程的问题。我们表明,在弛豫时间为零的极限中,一个获得了古伯瑟的理想流体力学解;在弛豫时间变为无穷大的极限中,一个获得了Denicol等人最初获得的精确的自由流解。对于有限的弛豫时间,我们用数值方法求解方程,并与服从Gubser流动的弛豫时间近似Boltzmann方程的精确解进行比较。使用这个作为我们的标准,我们发现各向异性流体力学比所有当前已知的耗散流体力学方法更好地描述了系统的时空演化。

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