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无序陈绝缘体中的基布尔-祖雷克行为。

Kibble-Zurek Behavior in Disordered Chern Insulators.

作者信息

Ulčakar Lara, Mravlje Jernej, Rejec Tomaž

机构信息

Jozef Stefan Institute, Jamova 39, SI-1000 Ljubljana, Slovenia and Faculty for Mathematics and Physics, University of Ljubljana, Jadranska 19, SI-1000 Ljubljana, Slovenia.

Jozef Stefan Institute, Jamova 39, SI-1000 Ljubljana, Slovenia.

出版信息

Phys Rev Lett. 2020 Nov 20;125(21):216601. doi: 10.1103/PhysRevLett.125.216601.

Abstract

Even though no local order parameter in the sense of the Landau theory exists for topological quantum phase transitions in Chern insulators, the highly nonlocal Berry curvature exhibits critical behavior near a quantum critical point. We investigate the critical properties of its real space analog, the local Chern marker, in weakly disordered Chern insulators. Because of disorder, inhomogeneities appear in the spatial distribution of the local Chern marker. Their size exhibits power-law scaling with the critical exponent matching the one extracted from the Berry curvature of a clean system. We drive the system slowly through such a quantum phase transition. The characteristic size of inhomogeneities in the nonequilibrium postquench state obeys the Kibble-Zurek scaling. In this setting, the local Chern marker thus does behave in a similar way as a local order parameter for a symmetry breaking second order phase transition. The Kibble-Zurek scaling also holds for the inhomogeneities in the spatial distribution of excitations and of the orbital polarization.

摘要

尽管在陈绝缘体中的拓扑量子相变不存在朗道理论意义上的局域序参量,但高度非局域的贝里曲率在量子临界点附近表现出临界行为。我们研究了其在实空间中的类似物——局域陈标记——在弱无序陈绝缘体中的临界性质。由于无序,局域陈标记的空间分布中出现了不均匀性。它们的大小呈现幂律标度,其临界指数与从清洁系统的贝里曲率中提取的指数相匹配。我们缓慢驱动系统通过这样一个量子相变。非平衡猝灭后状态下不均匀性的特征尺寸遵循基布尔-祖雷克标度。在这种情况下,局域陈标记的行为因此与对称性破缺二阶相变的局域序参量类似。基布尔-祖雷克标度也适用于激发和轨道极化的空间分布中的不均匀性。

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