Transition from Anomalous Hall Effect to Topological Hall Effect in Hexagonal Non-Collinear Magnet Mn3Ga
Abstract We report experimental observation of large anomalous Hall effect exhibited in non-collinear triangular antiferromagnet D019-type Mn3Ga with coplanar spin structure at temperatures higher than 100 K. The value of anomalous Hall resistivity increases with increasing temperature, which reache...
Guardado en:
Autores principales: | , , , , , , , , , |
---|---|
Formato: | article |
Lenguaje: | EN |
Publicado: |
Nature Portfolio
2017
|
Materias: | |
Acceso en línea: | https://doaj.org/article/2bcc723654974e58b27c5545384d7c49 |
Etiquetas: |
Agregar Etiqueta
Sin Etiquetas, Sea el primero en etiquetar este registro!
|
id |
oai:doaj.org-article:2bcc723654974e58b27c5545384d7c49 |
---|---|
record_format |
dspace |
spelling |
oai:doaj.org-article:2bcc723654974e58b27c5545384d7c492021-12-02T16:06:17ZTransition from Anomalous Hall Effect to Topological Hall Effect in Hexagonal Non-Collinear Magnet Mn3Ga10.1038/s41598-017-00621-x2045-2322https://doaj.org/article/2bcc723654974e58b27c5545384d7c492017-03-01T00:00:00Zhttps://doi.org/10.1038/s41598-017-00621-xhttps://doaj.org/toc/2045-2322Abstract We report experimental observation of large anomalous Hall effect exhibited in non-collinear triangular antiferromagnet D019-type Mn3Ga 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 Mn3Ga. Present study suggests that Mn3Ga shows promising possibility to be antiferromagnetic spintronics or topological Hall effect-based data storage devices.Z. H. LiuY. J. ZhangG. D. LiuB. DingE. K. LiuHasnain Mehdi JafriZ. P. HouW. H. WangX. Q. MaG. H. WuNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 7, Iss 1, Pp 1-7 (2017) |
institution |
DOAJ |
collection |
DOAJ |
language |
EN |
topic |
Medicine R Science Q |
spellingShingle |
Medicine R Science Q Z. H. Liu Y. J. Zhang G. D. Liu B. Ding E. K. Liu Hasnain Mehdi Jafri Z. P. Hou W. H. Wang X. Q. Ma G. H. Wu Transition from Anomalous Hall Effect to Topological Hall Effect in Hexagonal Non-Collinear Magnet Mn3Ga |
description |
Abstract We report experimental observation of large anomalous Hall effect exhibited in non-collinear triangular antiferromagnet D019-type Mn3Ga 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 Mn3Ga. Present study suggests that Mn3Ga shows promising possibility to be antiferromagnetic spintronics or topological Hall effect-based data storage devices. |
format |
article |
author |
Z. H. Liu Y. J. Zhang G. D. Liu B. Ding E. K. Liu Hasnain Mehdi Jafri Z. P. Hou W. H. Wang X. Q. Ma G. H. Wu |
author_facet |
Z. H. Liu Y. J. Zhang G. D. Liu B. Ding E. K. Liu Hasnain Mehdi Jafri Z. P. Hou W. H. Wang X. Q. Ma G. H. Wu |
author_sort |
Z. H. Liu |
title |
Transition from Anomalous Hall Effect to Topological Hall Effect in Hexagonal Non-Collinear Magnet Mn3Ga |
title_short |
Transition from Anomalous Hall Effect to Topological Hall Effect in Hexagonal Non-Collinear Magnet Mn3Ga |
title_full |
Transition from Anomalous Hall Effect to Topological Hall Effect in Hexagonal Non-Collinear Magnet Mn3Ga |
title_fullStr |
Transition from Anomalous Hall Effect to Topological Hall Effect in Hexagonal Non-Collinear Magnet Mn3Ga |
title_full_unstemmed |
Transition from Anomalous Hall Effect to Topological Hall Effect in Hexagonal Non-Collinear Magnet Mn3Ga |
title_sort |
transition from anomalous hall effect to topological hall effect in hexagonal non-collinear magnet mn3ga |
publisher |
Nature Portfolio |
publishDate |
2017 |
url |
https://doaj.org/article/2bcc723654974e58b27c5545384d7c49 |
work_keys_str_mv |
AT zhliu transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga AT yjzhang transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga AT gdliu transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga AT bding transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga AT ekliu transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga AT hasnainmehdijafri transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga AT zphou transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga AT whwang transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga AT xqma transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga AT ghwu transitionfromanomaloushalleffecttotopologicalhalleffectinhexagonalnoncollinearmagnetmn3ga |
_version_ |
1718385012761427968 |