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Significant Unconventional Anomalous Hall Effect in Heavy Metal/Antiferromagnetic Insulator Heterostructures.


ABSTRACT: The anomalous Hall effect (AHE) is a quantum coherent transport phenomenon that conventionally vanishes at elevated temperatures because of thermal dephasing. Therefore, it is puzzling that the AHE can survive in heavy metal (HM)/antiferromagnetic (AFM) insulator (AFMI) heterostructures at high temperatures yet disappears at low temperatures. In this paper, an unconventional high-temperature AHE in HM/AFMI is observed only around the Néel temperature of AFM, with large anomalous Hall resistivity up to 40 nΩ cm is reported. This mechanism is attributed to the emergence of a noncollinear AFM spin texture with a non-zero net topological charge. Atomistic spin dynamics simulation shows that such a unique spin texture can be stabilized by the subtle interplay among the collinear AFM exchange coupling, interfacial Dyzaloshinski-Moriya interaction, thermal fluctuation, and bias magnetic field.

SUBMITTER: Liang Y 

PROVIDER: S-EPMC10015866 | biostudies-literature | 2023 Mar

REPOSITORIES: biostudies-literature

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Significant Unconventional Anomalous Hall Effect in Heavy Metal/Antiferromagnetic Insulator Heterostructures.

Liang Yuhan Y   Wu Liang L   Dai Minyi M   Zhang Yujun Y   Zhang Qinghua Q   Wang Jie J   Zhang Nian N   Xu Wei W   Le Zhao   Chen Hetian H   Ma Ji J   Wu Jialu J   Cao Yanwei Y   Yi Di D   Ma Jing J   Jiang Wanjun W   Hu Jia-Mian JM   Nan Ce-Wen CW   Lin Yuan-Hua YH  

Advanced science (Weinheim, Baden-Wurttemberg, Germany) 20230126 8


The anomalous Hall effect (AHE) is a quantum coherent transport phenomenon that conventionally vanishes at elevated temperatures because of thermal dephasing. Therefore, it is puzzling that the AHE can survive in heavy metal (HM)/antiferromagnetic (AFM) insulator (AFMI) heterostructures at high temperatures yet disappears at low temperatures. In this paper, an unconventional high-temperature AHE in HM/AFMI is observed only around the Néel temperature of AFM, with large anomalous Hall resistivity  ...[more]

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