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Magnetization process and magnetic structure of the TmFe2H3.4 hydride in ultrahigh magnetic fields up to 100 T

Identifieur interne : 002A98 ( Main/Exploration ); précédent : 002A97; suivant : 002A99

Magnetization process and magnetic structure of the TmFe2H3.4 hydride in ultrahigh magnetic fields up to 100 T

Auteurs : N. V. Mushnikov [Russie] ; N. K. Zajkov [Russie] ; M. I. Bartashevich [Japon] ; T. Goto [Japon] ; H. Aruga Katori [Japon] ; M. Yamaguchi [Japon] ; I. Yamamoto [Japon]

Source :

RBID : Pascal:97-0205178

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English descriptors

Abstract

Copyright (c) 1996 Elsevier Science B.V. All rights reserved. Complete magnetization process was measured on the TmFe2H3.4 hydride without spontaneous magnetization at 4.2 K in ultrahigh magnetic fields up to 100 T. The absence of the spontaneous magnetization comes from both the weakening of the Tm-Fe exchange interaction and the appearance of uniaxial anisotropy due to a rhombohedral distortion of the parent cubic lattice upon hydrogenation. The magnetic structure is considered to consist of noncollinear Tm moments nearly parallel to the compressed [111 axis and collinear Fe moments antiparallel to the sum of the Tm moments. From the analysis of the observed magnetization process, the Tm-Fe exchange interaction and the uniaxial anisotropy constant can be estimated.


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Le document en format XML

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<term>Magnetization</term>
<term>Quantity ratio</term>
<term>Strong fields</term>
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<term>Thulium hydrides</term>
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<term>Etude expérimentale</term>
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<div type="abstract" xml:lang="en">Copyright (c) 1996 Elsevier Science B.V. All rights reserved. Complete magnetization process was measured on the TmFe
<sub>2</sub>
H
<sub>3.4</sub>
hydride without spontaneous magnetization at 4.2 K in ultrahigh magnetic fields up to 100 T. The absence of the spontaneous magnetization comes from both the weakening of the Tm-Fe exchange interaction and the appearance of uniaxial anisotropy due to a rhombohedral distortion of the parent cubic lattice upon hydrogenation. The magnetic structure is considered to consist of noncollinear Tm moments nearly parallel to the compressed [111 axis and collinear Fe moments antiparallel to the sum of the Tm moments. From the analysis of the observed magnetization process, the Tm-Fe exchange interaction and the uniaxial anisotropy constant can be estimated.</div>
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