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Transition from Anomalous Hall Effect to Topological Hall Effect in Hexagonal Non-Collinear Magnet Mn(3)Ga

We report experimental observation of large anomalous Hall effect exhibited in non-collinear triangular antiferromagnet D0(19)-type Mn(3)Ga with coplanar spin structure at temperatures higher than 100 K. The value of anomalous Hall resistivity increases with increasing temperature, which reaches 1.2...

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Detalles Bibliográficos
Autores principales: Liu, Z. H., Zhang, Y. J., Liu, G. D., Ding, B., Liu, E. K., Jafri, Hasnain Mehdi, Hou, Z. P., Wang, W. H., Ma, X. Q., Wu, G. H.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2017
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5428815/
https://www.ncbi.nlm.nih.gov/pubmed/28364119
http://dx.doi.org/10.1038/s41598-017-00621-x
Descripción
Sumario:We report experimental observation of large anomalous Hall effect exhibited in non-collinear triangular antiferromagnet D0(19)-type Mn(3)Ga with coplanar spin structure at temperatures higher than 100 K. The value of anomalous Hall resistivity increases with increasing temperature, which reaches 1.25 μΩ · cm at a low field of ~300 Oe at room temperature. The corresponding room-temperature anomalous Hall conductivity is about 17 (Ω · cm)(−1). Most interestingly, as temperature falls below 100 K, a temperature-independent topological-like Hall effect was observed. The maximum peak value of topological Hall resistivity is about 0.255 μΩ · cm. The appearance of the topological Hall effect is attributed to the change of spin texture as a result of weak structural distortion from hexagonal to orthorhombic symmetry in Mn(3)Ga. Present study suggests that Mn(3)Ga shows promising possibility to be antiferromagnetic spintronics or topological Hall effect-based data storage devices.