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Hydrodynamic Excitations from Chiral Kinetic Theory and the Hydrodynamic Frames

机译:手性动力学理论与水动力学的水动力激发   框架

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摘要

In the framework of chiral kinetic theory (CKT), we consider a system ofright- and left-handed Weyl fermions out of thermal equilibrium in ahomogeneous weak magnetic field. We show that the Lorentz invariance implies amodification in the definition of the momentum current in the phase space,compared to the case in which the system is in global equilibrium. Using thismodified momentum current, we derive the linearized conservation equations fromthe kinetic equation up to second order in the derivative expansion. It turnsout that the eigenmodes of these equations, namely the hydrodynamic modes,differ from those obtained from the hydrodynamic in the Landau-Lifshitz (LL)frame at the same order. We show that the modes of the former case may betransformed to the corresponding modes in the latter case by a global boost.The velocity of the boost is proportional to the magnetic field as well as thedifference between the right- and left-handed charges susceptibility. We thencompute the chiral transport coefficients in a system of non-Abelian chiralfermions in the no-drag frame and by making the above boost, obtain thewell-known transport coeffiecients of the system in the LL frame. Finally byusing the idea of boost, we reproduce the AdS/CFT result for the chiral dragforce exerted on a quark at rest in the rest frame of the fluid, withoutperforming any holographic computations.
机译:在手性动力学理论(CKT)的框架下,我们考虑了在均匀弱磁场中热平衡不平衡的右手和左手Weyl费米系统。我们证明,与系统处于全局平衡的情况相比,洛伦兹不变性意味着相空间中动量电流的定义发生了变化。使用这种修正的动量电流,我们从动力学方程推导了线性化的守恒方程,直到微分展开中的二阶。事实证明,这些方程的本征模,即流体动力学模,与从Landau-Lifshitz(LL)框架中的流体动力学获得的模本征模式相同。我们表明,前者的模式可以通过整体提升而转换为后者的相应模式。提升的速度与磁场以及左右手电荷磁化率的差异成正比。然后我们在无拖曳框架下计算了非阿贝尔手性铁素体系统中的手征输运系数,并通过进行上述增强,获得了该系统在LL框架中的众所周知的输运系数。最后,通过使用增强的想法,我们再现了静息在流体其余帧中的夸克上施加的手性拖曳力的AdS / CFT结果,而无需执行任何全息计算。

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