Universal thermalization dynamics in (1+1)d QFTs

Richard A. Davison, Luca V. Delacretaz
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Abstract

We identify the universal mechanism behind the thermalization of (1+1)d QFTs at high and low temperatures. Viewing these theories as CFTs perturbed by relevant or irrelevant deformations, we show that conformal perturbation theory in the thermal state breaks down at late times allowing for the emergence of hydrodynamics. This breakdown occurs universally due to the unsuppressed exchange of stress tensors near the lightcone. Furthermore, for theories with central charge $c\rightarrow\infty$ we solve for the emergent hydrodynamic theory to all orders in the gradient expansion by arguing that all transport parameters appearing in two-point functions have universal expressions in terms of the scaling dimension $\Delta$ of the perturbation. The radius of convergence of the hydrodynamic dispersion relations provides an early time cutoff for hydrodynamics, which agrees with the time scale at which conformal perturbation theory breaks down.
(1+1)d QFT 中的通用热化动力学
我们确定了(1+1)d QFT在高温和低温下热化背后的普遍机制。我们将这些理论视为受到相关或无关变形扰动的CFT,结果表明,热态下的共形扰动理论在后期会崩溃,从而导致流体力学的出现。由于光锥附近应力张量的无抑制交换,这种崩溃普遍发生。此外,对于中心电荷为$c\rightarrow\infty$的理论,我们通过论证所有出现在两点函数中的输运参数在扰动的缩放维度$\Delta$上的通用表达式,求解了梯度展开中所有阶次的出现的流体力学理论。流体力学色散关系的收敛半径为流体力学提供了一个早期时间截止,它与共形扰动理论崩溃的时间尺度一致。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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