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Quantum Hall states stabilized in semi-magnetic bilayers of topological insulators

机译:在拓扑绝缘体的半磁性双层中稳定的量子霍尔态

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摘要

By breaking the time-reversal symmetry in three-dimensional topological insulators with the introduction of spontaneous magnetization or application of magnetic field, the surface states become gapped, leading to quantum anomalous Hall effect or quantum Hall effect, when the chemical potential locates inside the gap. Further breaking of inversion symmetry is possible by employing magnetic topological insulator heterostructures that host non-degenerate top and bottom surface states. Here we demonstrate the tailored-material approach for the realization of robust quantum Hall states in the bilayer system, in which the cooperative or cancelling combination of the anomalous and ordinary Hall responses from the respective magnetic and non-magnetic layers is exemplified. The appearance of quantum Hall states at filling factor 0 and +1 can be understood by the relationship of energy band diagrams for the two independent surface states. The designable heterostructures of magnetic topological insulator may explore a new arena for intriguing topological transport and functionality.
机译:通过引入自发磁化或施加磁场来打破三维拓扑绝缘体中的时间反转对称性,当化学势位于间隙内部时,表面态变得空缺,从而导致量子异常霍尔效应或量子霍尔效应。通过采用磁性拓扑绝缘体异质结构,可承载非简并的顶部和底部表面状态,从而可以进一步打破反对称性。在这里,我们演示了在双层系统中实现鲁棒量子霍尔状态的量身定制的材料方法,其中例示了来自相应磁性层和非磁性层的异常和普通霍尔响应的协作或抵消组合。可以通过两个独立表面态的能带图之间的关系来理解填充系数为0和+1时的量子霍尔态的出现。磁性拓扑绝缘子的可设计异质结构可能会为吸引拓扑传输和功能性探索一个新领域。

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