Lacerda Artur M, Kewming Michael J, Brenes Marlon, Jackson Conor, Clark Stephen R, Mitchison Mark T, Goold John
School of Physics, <a href="https://ror.org/02tyrky19">Trinity College Dublin</a>, College Green, Dublin 2, D02K8N4, Ireland.
Department of Physics and Centre for Quantum Information and Quantum Control, <a href="https://ror.org/03dbr7087">University of Toronto</a>, 60 Saint George St., Toronto, Ontario, Canada, M5S 1A7.
Phys Rev E. 2024 Jul;110(1-1):014125. doi: 10.1103/PhysRevE.110.014125.
Understanding the entropy production of systems strongly coupled to thermal baths is a core problem of both quantum thermodynamics and mesoscopic physics. While many techniques exist to accurately study entropy production in such systems, they typically require a microscopic description of the baths, which can become numerically intractable to study for large systems. Alternatively an open-systems approach can be employed with all the nuances associated with various levels of approximation. Recently, the mesoscopic leads approach has emerged as a powerful method for studying such quantum systems strongly coupled to multiple thermal baths. In this method, a set of discretized lead modes, each locally damped, provide a Markovian embedding. Here we show that this method proves extremely useful to describe entropy production of a strongly coupled open quantum system. We show numerically, for both noninteracting and interacting setups, that a system coupled to a single bath exhibits a thermal fixed point at the level of the embedding. This allows us to use various results from the thermodynamics of quantum dynamical semigroups to infer the nonequilibrium thermodynamics of the strongly coupled, non-Markovian central systems. In particular, we show that the entropy production in the transient regime recovers the well-established microscopic definitions of entropy production with a correction that can be computed explicitly for both the single- and multiple-lead cases.
理解与热库强耦合的系统的熵产生是量子热力学和介观物理学的核心问题。虽然存在许多技术可用于精确研究此类系统中的熵产生,但它们通常需要对热库进行微观描述,对于大型系统而言,这在数值计算上可能变得难以处理。或者,可以采用具有各种近似层次相关细微差别的开放系统方法。最近,介观引线方法已成为研究此类与多个热库强耦合的量子系统的有力方法。在这种方法中,一组离散的引线模式,每个模式局部阻尼,提供了一个马尔可夫嵌入。在这里,我们表明这种方法对于描述强耦合开放量子系统的熵产生非常有用。我们通过数值计算表明,对于非相互作用和相互作用的设置,耦合到单个热库的系统在嵌入层面表现出一个热固定点。这使我们能够利用量子动力学半群热力学的各种结果来推断强耦合、非马尔可夫中心系统的非平衡热力学。特别是,我们表明瞬态 regime 中的熵产生通过一个修正恢复了已确立的熵产生的微观定义,该修正对于单引线和多引线情况都可以明确计算。