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The topological quantum phase transitions in Lieb lattice driven by the Rashba SOC and exchange field

机译:由Rashba SOC和交换场驱动的Lieb晶格中的拓扑量子相变

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摘要

The quantum spin Hall (QSH) effect and the quantum anomalous Hall (QAH) effect in Lieb lattice are investigated in the presence of both Rashba spin-orbit coupling (SOC) and uniform exchange field. The Lieb lattice has a simple cubic symmetry, which is characterized by the single Dirac-cone per Brillouin zone and the middle flat band in the band structure. The intrinsic SOC is essentially needed to open the full energy gap in the bulk. The QSH effect could survive even in the presence of the exchange field. In terms of the first Chern number and the spin Chern number, we study the topological nature and the topological phase transition from the time-reversal symmetry broken QSH effect to the QAH effect. For Lieb lattice ribbons, the energy spectrum and the wave-function distributions are obtained numerically, where the helical edge states and the chiral edge states reveal the non-trivial topological QSH and QAH properties, respectively.
机译:研究了在存在Rashba自旋轨道耦合(SOC)和均匀交换场的情况下,Lieb晶格中的量子自旋霍尔(QSH)效应和量子异常霍尔(QAH)效应。 Lieb晶格具有简单的立方对称性,其特征是每个布里渊区具有单个狄拉克锥,带结构中的中间平坦带。根本上需要SOC来打开块中的全部能隙。即使存在交换场,QSH效应也可以保留。根据第一切恩数和自旋切恩数,我们研究了时间反对称打破QSH效应到QAH效应的拓扑性质和拓扑相变。对于利勃氏晶格带,通过数值获得能谱和波函数分布,其中螺旋边缘状态和手性边缘状态分别显示了非平凡的拓扑QSH和QAH性质。

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