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Fate of quantum anomalous Hall effect in the presence of external magnetic fields and particle-hole asymmetry

机译:在外部磁场和粒子孔不对称存在下量子异常霍尔效应的命运

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摘要

The quantum anomalous Hall (QAH) effect, a condensed matter analog of the parity anomaly, is characterized by a quantized Hall conductivity in the absence of an external magnetic field. However, it has been recently shown that, even in the presence of Landau levels, the QAH effect can be distinguished from the conventional quantum Hall (QH) effect due to the parity anomaly. As a signature of this effect, we predicted coexistent counterpropagating QAH and QH edge states. In the present work, we generalize these findings to QAH insulators with broken particle-hole symmetry. In particular, we derive the connection to the spectral asymmetry, which is a topological quantity arising in the context of Dirac-like systems. Moreover, it is shown that, depending on the magnetic field direction, particle-hole asymmetry strengthens or weakens the hybridization of the counterpropagating QH and QAH edge states. Implications for ferro- or paramagnetic topological insulators are derived which pave the way towards identifying signatures of the QAH effect even in external magnetic fields.
机译:量子异常霍尔(QAH)效应是截止异常的凝聚态模拟,其特征在于在没有外部磁场的情况下的量化霍尔电导率。然而,最近已经表明,即使在Landau水平的存在下,QAH效果也可以与由于平衡异常引起的传统量子大厅(QH)效应区分开。作为这种效果的签名,我们预测了共存的反向QAH和QH边缘状态。在目前的工作中,我们将这些发现概括为具有破碎的粒子对称性的QAH绝缘体。特别地,我们导出了与光谱不对称性的连接,这是在狄拉氏系统的上下文中产生的拓扑量。此外,示出了,根据磁场方向,粒子孔不对称强化或削弱反向QH和QAH边缘状态的杂交。导出对铁磁性拓扑绝缘体的影响,即使在外部磁场中,也铺平了探讨衡量QAH效果的签名。

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