Angular momentum compensation manipulation to room temperature of the ferrimagnet Ho3−xDyxFe5O12 detected by the Barnett effect
We demonstrate that the angular momentum compensation temperature TA, at which the net angular momentum in the sample disappears, can be controlled in Ho3Fe5O12 by partially substituting Dy for Ho. TA can be detected using the Barnett effect, by which mechanical rotation magnetizes an object due to...
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Published in | Applied physics letters Vol. 114; no. 16 |
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Main Authors | , , , , , , , |
Format | Journal Article |
Language | English |
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Melville
American Institute of Physics
22.04.2019
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Abstract | We demonstrate that the angular momentum compensation temperature TA, at which the net angular momentum in the sample disappears, can be controlled in Ho3Fe5O12 by partially substituting Dy for Ho. TA can be detected using the Barnett effect, by which mechanical rotation magnetizes an object due to spin-rotation coupling. We found that TA increases with the Dy content and clarified that TA of Ho1.5Dy1.5Fe5O12 coincides with room temperature. The Barnett effect enables us to explore materials applicable to magnetic devices utilizing the angular momentum compensation only by rotating the powder sample at room temperature. |
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AbstractList | We demonstrate that the angular momentum compensation temperature TA, at which the net angular momentum in the sample disappears, can be controlled in Ho3Fe5O12 by partially substituting Dy for Ho. TA can be detected using the Barnett effect, by which mechanical rotation magnetizes an object due to spin-rotation coupling. We found that TA increases with the Dy content and clarified that TA of Ho1.5Dy1.5Fe5O12 coincides with room temperature. The Barnett effect enables us to explore materials applicable to magnetic devices utilizing the angular momentum compensation only by rotating the powder sample at room temperature. |
Author | Chudo, Hiroyuki Ono, Masao Matsuo, Mamoru Ohnuma, Yuichi Imai, Masaki Saitoh, Eiji Harii, Kazuya Maekawa, Sadamichi |
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References_xml | – start-page: 217204 year: 2007 ident: c3 publication-title: Phys. Rev. Lett. – start-page: 239 year: 1915 ident: c6 publication-title: Phys. Rev. – start-page: 672 year: 1962 ident: c8 publication-title: Il Nuovo Cimento (1955-1965) – start-page: 134404 year: 2006 ident: c1 publication-title: Phys. Rev. B – start-page: 052402 year: 2018 ident: c5 publication-title: Appl. Phys. Lett. – start-page: 174424 year: 2015 ident: c9 publication-title: Phys. Rev. B – start-page: 072409 year: 2017 ident: c10 publication-title: Appl. Phys. Lett. – start-page: 329 year: 2017 ident: c11 publication-title: J. Magn. Magn. Mater. – start-page: 1187 year: 2017 ident: c4 publication-title: Nat. Mater. – start-page: 129 year: 1935 ident: c7 publication-title: Rev. Mod. Phys. – start-page: 220402 year: 2006 ident: c2 publication-title: Phys. Rev. B |
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Snippet | We demonstrate that the angular momentum compensation temperature TA, at which the net angular momentum in the sample disappears, can be controlled in... |
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SubjectTerms | Angular momentum Applied physics Compensation Dysprosium Ferrimagnetism Magnetic devices Room temperature Rotation |
Title | Angular momentum compensation manipulation to room temperature of the ferrimagnet Ho3−xDyxFe5O12 detected by the Barnett effect |
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