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阻尼谐振子的冯·诺依曼熵与熵产生

von Neumann entropy and entropy production of a damped harmonic oscillator.

作者信息

Weiderpass G A, Caldeira A O

机构信息

Instituto de Física Gleb Wataghin, Universidade Estadual de Campinas, 13083-859 Campinas, SP, Brazil.

出版信息

Phys Rev E. 2020 Sep;102(3-1):032102. doi: 10.1103/PhysRevE.102.032102.

Abstract

In this paper we analyze the entropy and entropy production of a nonisolated quantum system described within the quantum Brownian motion framework. This is a very general and paradigmatic framework for describing nonisolated quantum systems and can be used in any kind of coupling regime. We start by considering the application of von Neumann entropy to an arbitrarily damped quantum system making use of its reduced density operator. We argue that this application is formally valid and develop a path-integral method to evaluate that quantity analytically. We apply this technique to a harmonic oscillator in contact with a heat bath and obtain an exact form for its entropy. Then we study the entropy production of this system and enlighten important characteristics of its thermodynamical behavior on the pure quantum realm and also address their transition to the classical limit.

摘要

在本文中,我们分析了在量子布朗运动框架内描述的非孤立量子系统的熵和熵产生。这是一个用于描述非孤立量子系统的非常通用且具有代表性的框架,可用于任何类型的耦合 regime。我们首先考虑将冯·诺依曼熵应用于利用其约化密度算符的任意阻尼量子系统。我们认为这种应用在形式上是有效的,并开发了一种路径积分方法来解析地评估该量。我们将此技术应用于与热浴接触的谐振子,并获得其熵的精确形式。然后我们研究该系统的熵产生,并揭示其在纯量子领域的热力学行为的重要特征,还讨论它们向经典极限的转变。

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