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arXiv 1809.01946cond-mat.stat-mechquant-ph
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单能量本征态的功提取

Work Extraction from a Single Energy Eigenstate

Kazuya Kaneko, Eiki Iyoda, Takahiro Sagawa

摘要:

从吉布斯系综中通过循环操作提取功是不可能的,如热力学第二定律所示。另一方面,本征态热化假说(ETH)指出,只有一个单一的能量本征态可以描述一个热平衡状态。在这里,我们试图统一这两个观点,并调查在个人的能量本征态的水平上的第二定律,通过检查从一个单一的能量本征态提取工作的可能性。具体来说,我们进行了数值精确对角化的淬火协议的本地哈密顿和评估的工作可提取的能量本征态的数量。我们发现,它在一个有限的系统大小完全为零,这意味着一个积极的工作量不能从任何能量本征态提取,如果一个或两个前和后淬火哈密顿是不可积的。我们认为,这种数值观测背后的机制是基于ETH的非本地可观测。我们的结果意味着,量子混沌,其特征在于不可积性,导致一个更强的版本的第二定律比传统的配方的基础上的统计系综。

英文摘要:

Work extraction from the Gibbs ensemble by a cyclic operation is impossible, as represented by the second law of thermodynamics. On the other hand, the eigenstate thermalization hypothesis (ETH) states that just a single energy eigenstate can describe a thermal equilibrium state. Here we attempt to unify these two perspectives and investigate the second law at the level of individual energy eigenstates, by examining the possibility of extracting work from a single energy eigenstate. Specifically, we performed numerical exact diagonalization of a quench protocol of local Hamiltonians and evaluated the number of work-extractable energy eigenstates. We found that it becomes exactly zero in a finite system size, implying that a positive amount of work cannot be extracted from any energy eigenstate, if one or both of the pre- and the post-quench Hamiltonians are non-integrable. We argue that the mechanism behind this numerical observation is based on the ETH for a non-local observable. Our result implies that quantum chaos, characterized by non-integrability, leads to a stronger version of the second law than the conventional formulation based on the statistical ensembles.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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