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First-order phase transition and anomalous hysteresis of Bose gases in optical lattices

机译:玻色气体中玻色气体的一阶相变和异常磁滞

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We study the first-order quantum phase transitions of Bose gases in optical lattices. A special emphasis is placed on an anomalous hysteresis behavior, in which the phase transition occurs in a unidirectional way and a hysteresis loop does not form. We first revisit the hardcore Bose-Hubbard model with dipole-dipole interactions on a triangular lattice to analyze accurately the ground-state phase diagram and the hysteresis using the cluster mean-field theory combined with cluster-size scaling. Details of the anomalous hysteresis are presented. We next consider the two-component and spin-1 Bose-Hubbard models on a hypercubic lattice and show that the anomalous hysteresis can emerge in these systems as well. In particular, for the former model, we discuss the experimental feasibility of the first-order transitions and the associated hysteresis. We also explain an underlying mechanism of the anomalous hysteresis by means of the Ginzburg-Landau theory. From the given cases, we conclude that the anomalous hysteresis is a ubiquitous phenomenon of systems with a phase region of lobe shape that is surrounded by the first-order boundary.
机译:我们研究了光学晶格中玻色气体的一阶量子相变。特别强调异常的磁滞行为,其中相变以单向方式发生,并且不形成磁滞回线。我们首先使用在三角形晶格上具有偶极子-偶极子相互作用的硬核Bose-Hubbard模型,使用聚类平均场理论和聚类尺寸缩放比例,准确分析基态相位图和磁滞。给出了异常磁滞的详细信息。接下来,我们考虑超立方晶格上的双组分和自旋1 Bose-Hubbard模型,并证明在这些系统中也可能出现异常磁滞现象。特别是,对于前一个模型,我们讨论了一阶跃迁及其相关滞后的实验可行性。我们还通过Ginzburg-Landau理论解释了异常磁滞现象的潜在机制。从给定的情况中,我们得出结论,异常磁滞现象是具有一阶边界包围的波瓣形相位区域的系统的普遍现象。

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