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首页> 外文期刊>Journal of Mathematical Sciences >ON THE GENERAL DEFINITION OF THE PRODUCTION OF ENTROPY IN OPEN MARKOV QUANTUM SYSTEMS
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ON THE GENERAL DEFINITION OF THE PRODUCTION OF ENTROPY IN OPEN MARKOV QUANTUM SYSTEMS

机译:马尔可夫开放量子系统中熵产生的一般定义

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We discuss the question of the general definition of the production of entropy per unit time for a quantum system governed by the Lindblad equation. The difficulty is as follows: in order to determine the total production of entropy, one must know the entropy flow from the system into the environment. This requires additional information on the environment and on its interaction with the system. The Lindblad equation for the reduced density matrix of the system does not contain such information. Therefore, the following question arises: What minimum additional information about the environment must be added to the Lindblad equation in order to find the flow of entropy into the environment and the total production of entropy? To answer this question, we use the concept of a complementary quantum channel known from the the quantum information theory. We also prove a theorem on the nonnegativity of production of entropy, and, under certain assumptions, the adiabatic and nonadiabatic contribution to it.
机译:我们讨论由Lindblad方程控制的量子系统每单位时间熵产生的一般定义问题。困难如下:为了确定熵的总产生量,必须知道从系统到环境的熵流。这需要有关环境及其与系统交互的其他信息。系统的降低密度矩阵的Lindblad方程不包含此类信息。因此,出现了以下问题:必须向Lindblad方程添加关于环境的最少最少附加信息,以便找到进入环境的熵流和熵的总产量?为了回答这个问题,我们使用了量子信息理论中已知的互补量子通道的概念。我们还证明了关于熵产生的非负性的一个定理,并且在某些假设下,证明了绝热和非绝热的贡献。

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