The Quantum Anomalous Hall Effect: Theory and Experiment

被引:423
|
作者
Liu, Chao-Xing [1 ]
Zhang, Shou-Cheng [2 ]
Qi, Xiao-Liang [2 ]
机构
[1] Penn State Univ, Dept Phys, 104 Davey Lab, University Pk, PA 16802 USA
[2] Stanford Univ, Dept Phys, Stanford, CA 94305 USA
基金
美国国家科学基金会;
关键词
topological state; quantum Hall effect; magnetic semiconductors; topological insulators; SINGLE DIRAC CONE; TOPOLOGICAL-INSULATOR; PHASE-TRANSITION; CONDUCTANCE; REALIZATION; SURFACE; ABSENCE; MODEL; FERROMAGNETISM; QUANTIZATION;
D O I
10.1146/annurev-conmatphys-031115-011417
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
The quantum anomalous Hall effect is defined as a quantized Hall effect realized in a system without an external magnetic field. The quantum anomalous Hall effect is a novel manifestation of topological structure in many-electron systems and may have potential applications in future electronic devices. In recent years, the quantum anomalous Hall effect was proposed theoretically and realized experimentally. In this review article, we provide a systematic overview of the theoretical and experimental developments in this field.
引用
收藏
页码:301 / 321
页数:21
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