在分离量子相关相的边界处的分岔和突变

M. Yurischev
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摘要

考虑了均匀磁场中处于热平衡状态下自旋为1/2的XXZ链。对于这个模型,我们给出了单向量子功亏损(热失谐)的相图。这些图可以包含平稳和可变(状态相关)最佳测量角度的区域。我们还建立了不同区域边界附近最佳测量角的行为与朗道第二类和第一类相变理论之间的关系。即,当从平稳的最佳测量角(0或π/2)区域跨越边界到可变的最佳测量角(0 < φ < π/2)区域时,量子失谐和单向量子功亏的行为会发生突然变化(“突变”)。突变伴随着表征量子相关平稳点的最小值分裂为两个最小值(即初始单个最小值发生分岔)。这种现象类似于朗道理论中描述的相变,或者更一般地说,是由突变理论的数学形式描述的相变。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Bifurcations and catastrophes at the boundaries separating the phases of quantum correlations
The spin-1/2 XXZ chain in a uniform magnetic field at thermal equilibrium is considered. For this model, we give phase diagrams for the one-way quantum work deficit (thermal discord). The diagrams can contain regions with both stationary and variable (state-dependent) angles of optimal measurement. We also established a relationship between the behavior of optimal measurement angles near the boundaries separated different regions and Landau’s theory of phase transitions of the second and first kind. Namely, when crossing the boundary from a region with a stationary optimal measurement angle (0 or π/2) to the region with a variable angle of optimal measurement (0 < ϑ < π/2), quantum discord and one-way quantum work deficit experience a sudden change (“catastrophe”) in their behavior. The sudden change is accompanied by a splitting of the minimum characterizing stationary point of quantum correlation into two minima (i.e., bifurcation of the initial single minimum occurs). Such phenomena are analogous to phase transitions described within the Landau theory, or, more generally, by the mathematical formalism of catastrophe theory.
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