弱测量和量子不可分性的统计力学

S. A. Saleh
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引用次数: 0

摘要

在弱测量思想实验中,一个系综由M个量子粒子和N个态组成。我们观察到粒子的可分性丧失,因此我们有模糊的粒子在系综中的占据数。不需要精确测量每个粒子的状态,量子干涉增加了额外的可能的组合,这解释了量子鸽子洞原理。这个原理给系统增加了更多的熵;因此,粒子似乎有一种新的相关性,从没有单一的、明确定义的状态的粒子中涌现出来。我们用抽象希尔伯特空间的语言表述了量子鸽子洞原理,然后将其推广到由混合状态组成的系统。这种对量子统计力学基本原理的洞察可以帮助我们更深入地理解量子力学的解释,并可能对量子计算和信息理论产生影响。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Statistical Mechanics for Weak Measurements and Quantum Inseparability
In weak measurement thought experiment, an ensemble consists of M quantum particles and N states. We observe that separability of the particles is lost, and hence we have fuzzy occupation numbers for the particles in the ensemble. Without sharply measuring each particle state, quantum interferences add extra possible configurations of the ensemble, this explains the Quantum Pigeonhole Principle. This principle adds more entropy to the system; hence the particles seem to have a new kind of correlations emergent from particles not having a single, well-defined state. We formulated the Quantum Pigeonhole Principle in the language of abstract Hilbert spaces, then generalized it to systems consisting of mixed states. This insight into the fundamentals of quantum statistical mechanics could help us understand the interpretation of quantum mechanics more deeply, and possibly have implication on quantum computing and information theory.
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