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Magnetic and Structural Studies on Two-Dimensional Antiferromagnets (MCl)LaNb sub( 2)O sub( 7) (M = Mn, Co, Cr)
We report magnetic and structural studies on the two-dimensional antiferromagnets (MCl)LaNb...O... (M = Mn, Cr, Co), prepared by topochemical reactions of a layered perovskite RbLaNb...O... Electron diffraction of these oxyhalides revealed a superstructure with a ...a x ...a cell for M = Mn and Co,...
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Published in: | Journal of the Physical Society of Japan 2016-03, Vol.85 (3), p.1-1 |
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container_title | Journal of the Physical Society of Japan |
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creator | Kitada, Atsushi Tsujimoto, Yoshihiro Nishi, Masakazu Matsuo, Akira Kindo, Koichi Ueda, Yutaka Ajiro, Yoshitami Kageyama, Hiroshi |
description | We report magnetic and structural studies on the two-dimensional antiferromagnets (MCl)LaNb...O... (M = Mn, Cr, Co), prepared by topochemical reactions of a layered perovskite RbLaNb...O... Electron diffraction of these oxyhalides revealed a superstructure with a ...a x ...a cell for M = Mn and Co, and a 2a x 2a cell for M = Cr, indicating that the MCl networks are distorted from an ideal square lattice. Neutron diffraction experiments showed that M = Mn and Co exhibit a (... 0 ...) antiferromagnetic order as observed for the S = 1/2 counterparts. (CoCl)LaNb...O... with a strong spin anisotropy shows an antiferro to weak-ferromagnetic transition at low field, followed by novel two-step metamagnetic transitions likely associated with a 1/2 plateau for 27-54 T. Possible spin structures under magnetic field are discussed in terms of an Ising-type model. By contrast, (CrCl)LaNb...O... exhibits a (... ... ...) order, which is the first observation among related oxyhalides, and a spin-flop transition at 12 T due to a weak spin anisotropy. These results suggest that a slight difference in the MCl structure and spin anisotropy provides a crucial influence on the magnetic properties. (ProQuest: ... denotes formulae/symbols omitted.) |
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(M = Mn, Cr, Co), prepared by topochemical reactions of a layered perovskite RbLaNb...O... Electron diffraction of these oxyhalides revealed a superstructure with a ...a x ...a cell for M = Mn and Co, and a 2a x 2a cell for M = Cr, indicating that the MCl networks are distorted from an ideal square lattice. Neutron diffraction experiments showed that M = Mn and Co exhibit a (... 0 ...) antiferromagnetic order as observed for the S = 1/2 counterparts. (CoCl)LaNb...O... with a strong spin anisotropy shows an antiferro to weak-ferromagnetic transition at low field, followed by novel two-step metamagnetic transitions likely associated with a 1/2 plateau for 27-54 T. Possible spin structures under magnetic field are discussed in terms of an Ising-type model. By contrast, (CrCl)LaNb...O... exhibits a (... ... ...) order, which is the first observation among related oxyhalides, and a spin-flop transition at 12 T due to a weak spin anisotropy. These results suggest that a slight difference in the MCl structure and spin anisotropy provides a crucial influence on the magnetic properties. (ProQuest: ... denotes formulae/symbols omitted.)</description><identifier>ISSN: 0031-9015</identifier><identifier>EISSN: 1347-4073</identifier><language>eng</language><subject>Anisotropy ; Antiferromagnetism ; Chromium ; Distortion ; Manganese ; Oxyhalides ; Superstructures ; Two dimensional</subject><ispartof>Journal of the Physical Society of Japan, 2016-03, Vol.85 (3), p.1-1</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780</link.rule.ids></links><search><creatorcontrib>Kitada, Atsushi</creatorcontrib><creatorcontrib>Tsujimoto, Yoshihiro</creatorcontrib><creatorcontrib>Nishi, Masakazu</creatorcontrib><creatorcontrib>Matsuo, Akira</creatorcontrib><creatorcontrib>Kindo, Koichi</creatorcontrib><creatorcontrib>Ueda, Yutaka</creatorcontrib><creatorcontrib>Ajiro, Yoshitami</creatorcontrib><creatorcontrib>Kageyama, Hiroshi</creatorcontrib><title>Magnetic and Structural Studies on Two-Dimensional Antiferromagnets (MCl)LaNb sub( 2)O sub( 7) (M = Mn, Co, Cr)</title><title>Journal of the Physical Society of Japan</title><description>We report magnetic and structural studies on the two-dimensional antiferromagnets (MCl)LaNb...O... (M = Mn, Cr, Co), prepared by topochemical reactions of a layered perovskite RbLaNb...O... Electron diffraction of these oxyhalides revealed a superstructure with a ...a x ...a cell for M = Mn and Co, and a 2a x 2a cell for M = Cr, indicating that the MCl networks are distorted from an ideal square lattice. Neutron diffraction experiments showed that M = Mn and Co exhibit a (... 0 ...) antiferromagnetic order as observed for the S = 1/2 counterparts. (CoCl)LaNb...O... with a strong spin anisotropy shows an antiferro to weak-ferromagnetic transition at low field, followed by novel two-step metamagnetic transitions likely associated with a 1/2 plateau for 27-54 T. Possible spin structures under magnetic field are discussed in terms of an Ising-type model. By contrast, (CrCl)LaNb...O... exhibits a (... ... ...) order, which is the first observation among related oxyhalides, and a spin-flop transition at 12 T due to a weak spin anisotropy. These results suggest that a slight difference in the MCl structure and spin anisotropy provides a crucial influence on the magnetic properties. 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(M = Mn, Cr, Co), prepared by topochemical reactions of a layered perovskite RbLaNb...O... Electron diffraction of these oxyhalides revealed a superstructure with a ...a x ...a cell for M = Mn and Co, and a 2a x 2a cell for M = Cr, indicating that the MCl networks are distorted from an ideal square lattice. Neutron diffraction experiments showed that M = Mn and Co exhibit a (... 0 ...) antiferromagnetic order as observed for the S = 1/2 counterparts. (CoCl)LaNb...O... with a strong spin anisotropy shows an antiferro to weak-ferromagnetic transition at low field, followed by novel two-step metamagnetic transitions likely associated with a 1/2 plateau for 27-54 T. Possible spin structures under magnetic field are discussed in terms of an Ising-type model. By contrast, (CrCl)LaNb...O... exhibits a (... ... ...) order, which is the first observation among related oxyhalides, and a spin-flop transition at 12 T due to a weak spin anisotropy. These results suggest that a slight difference in the MCl structure and spin anisotropy provides a crucial influence on the magnetic properties. (ProQuest: ... denotes formulae/symbols omitted.)</abstract></addata></record> |
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source | American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list) |
subjects | Anisotropy Antiferromagnetism Chromium Distortion Manganese Oxyhalides Superstructures Two dimensional |
title | Magnetic and Structural Studies on Two-Dimensional Antiferromagnets (MCl)LaNb sub( 2)O sub( 7) (M = Mn, Co, Cr) |
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