Classical and quantum stochastic thermodynamics

M. J. Oliveira
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引用次数: 4

Abstract

The stochastic thermodynamics provides a framework for the description of systems that are out of thermodynamic equilibrium. It is based on the assumption that the elementary constituents are acted by random forces that generate a stochastic dynamics, which is here represented by a Fokker-Planck-Kramers equation. We emphasize the role of the irreversible probability current, the vanishing of which characterizes the thermodynamic equilibrium and yields a special relation between fluctuation and dissipation. The connection to thermodynamics is obtained by the definition of the energy function and the entropy as well as the rate at which entropy is generated. The extension to quantum systems is provided by a quantum evolution equation which is a canonical quantization of the Fokker-Planck-Kramers equation. An example of an irreversible systems is presented which shows a nonequilibrium stationary state with an unceasing production of entropy. A relationship between the fluxes and the path integral is also presented.
经典和量子随机热力学
随机热力学为描述热力学不平衡的系统提供了一个框架。它基于一个假设,即基本成分受到随机力的作用,产生随机动力学,在这里用福克-普朗克-克莱默斯方程表示。我们强调不可逆概率电流的作用,它的消失是热力学平衡的特征,并在涨落和耗散之间产生一种特殊的关系。与热力学的联系是通过能量函数和熵的定义以及熵产生的速率来获得的。对量子系统的扩展由一个量子演化方程提供,该方程是福克-普朗克-克莱默斯方程的标准量子化。给出了一个不可逆系统的例子,该系统具有不断产生熵的非平衡定态。给出了通量与路径积分之间的关系。
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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