Layer Hall effect in a 2D topological Axion antiferromagnet

• Published in: arXiv.org
• Main Authors: Gao, Anyuan, Yu-Fei, Liu, Hu, Chaowei, Jian-Xiang Qiu, Tzschaschel, Christian, Ghosh, Barun, Sheng-Chin, Ho, Bérubé, Damien, Chen, Rui, Sun, Haipeng, Zhang, Zhaowei, Xin-Yue, Zhang, Yu-Xuan, Wang, Wang, Naizhou, Huang, Zumeng, Felser, Claudia, Agarwal, Amit, Ding, Thomas, Hung-Ju, Tien, Akey, Austin, Gardener, Jules, Singh, Bahadur, Watanabe, Kenji, Taniguchi, Takashi, Burch, Kenneth S, Bell, David C, Zhou, Brian B, Gao, Weibo, Hai-Zhou, Lu, Bansil, Arun, Lin, Hsin, Tay-Rong, Chang, Fu, Liang, Ma, Qiong, Ni, Ni, Su-Yang, Xu
• Format: Paper Journal Article
• Language: English
• Published: Ithaca Cornell University Library, arXiv.org 21.07.2021
• Subjects: Antiferromagnetism; Curvature; Electric fields; Electromagnetism; Ferromagnetism; Hall effect; Magnetic materials; Magnetic properties; Magnetism; Physics - Materials Science; Physics - Mesoscale and Nanoscale Physics; Topological insulators; Topology; Unit cell
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.2107.10233

While ferromagnets have been known and exploited for millennia, antiferromagnets (AFMs) were only discovered in the 1930s. The elusive nature indicates AFMs' unique properties: At large scale, due to the absence of global magnetization, AFMs may appear to behave like any non-magnetic material; However, such a seemingly mundane macroscopic magnetic property is highly nontrivial at microscopic level, where opposite spin alignment within the AFM unit cell forms a rich internal structure. In topological AFMs, such an internal structure leads to a new possibility, where topology and Berry phase can acquire distinct spatial textures. Here, we study this exciting possibility in an AFM Axion insulator, even-layered MnBi\(_2\)Te\(_4\) flakes, where spatial degrees of freedom correspond to different layers. Remarkably, we report the observation of a new type of Hall effect, the layer Hall effect, where electrons from the top and bottom layers spontaneously deflect in opposite directions. Specifically, under no net electric field, even-layered MnBi\(_2\)Te\(_4\) shows no anomalous Hall effect (AHE); However, applying an electric field isolates the response from one layer and leads to the surprising emergence of a large layer-polarized AHE (~50%\(\frac{e^2}{h}\)). Such a layer Hall effect uncovers a highly rare layer-locked Berry curvature, which serves as a unique character of the space-time \(\mathcal{PT}\)-symmetric AFM topological insulator state. Moreover, we found that the layer-locked Berry curvature can be manipulated by the Axion field, E\(\cdot\)B, which drives the system between the opposite AFM states. Our results achieve previously unavailable pathways to detect and manipulate the rich internal spatial structure of fully-compensated topological AFMs. The layer-locked Berry curvature represents a first step towards spatial engineering of Berry phase, such as through layer-specific moiré potential.