混沌量子电路中出现的纳维-斯托克斯流体力学

Hansveer Singh, Ewan McCulloch, Sarang Gopalakrishnan, Romain Vasseur
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引用次数: 0

摘要

我们构建了一个二维不可解量子电路集合,它是混沌的,但具有守恒的粒子电流,因此具有有限的德鲁德权。这种系统的长波流体力学由不可压缩的纳维-斯托克斯方程给出。通过分析集合中回路间的波动,我们认为这些波动可以忽略不计,因此像粘度这样的传输系数的回路平均值也是(在长时间极限内)典型回路中的值。电路平均传输系数可以映射到经典的不可逆马尔可夫过程中。因此,值得注意的是,我们的构造允许我们高效地计算强相互作用混沌二维量子系统族的粘度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Emergence of Navier-Stokes hydrodynamics in chaotic quantum circuits
We construct an ensemble of two-dimensional nonintegrable quantum circuits that are chaotic but have a conserved particle current, and thus a finite Drude weight. The long-wavelength hydrodynamics of such systems is given by the incompressible Navier-Stokes equations. By analyzing circuit-to-circuit fluctuations in the ensemble we argue that these are negligible, so the circuit-averaged value of transport coefficients like the viscosity is also (in the long-time limit) the value in a typical circuit. The circuit-averaged transport coefficients can be mapped onto a classical irreversible Markov process. Therefore, remarkably, our construction allows us to efficiently compute the viscosity of a family of strongly interacting chaotic two-dimensional quantum systems.
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