Serveur d'exploration sur le cobalt au Maghreb

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Synthesis, Nuclear, and Magnetic Structures and Magnetic Properties of [Mn3(OH)2(SO4)2(H2O)2]

Identifieur interne : 000963 ( Main/Exploration ); précédent : 000962; suivant : 000964

Synthesis, Nuclear, and Magnetic Structures and Magnetic Properties of [Mn3(OH)2(SO4)2(H2O)2]

Auteurs : Mohsen Ben Salah [France, Tunisie] ; Serge Vilminot [France] ; Gilles André [France] ; Mireille Richard-Plouet [France] ; Françoise Bourée-Vigneron [France] ; Tahar Mhiri [Tunisie] ; Mohamedally Kurmoo [France]

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RBID : ISTEX:EC88300ECDF9D384AE6091F55E31582693F09D9A

English descriptors

Abstract

[Mn3(OH)2(SO4)2(H2O)2] and its deuterated anlaogue were synthesized by a hydrothermal technique and characterized by differential thermal analysis, thermogravimetric analysis, and IR spectroscopy. Its nuclear structure, determined by single‐crystal X‐ray analysis and Rietveld analysis of neutron powder‐diffraction data, consists of a 3D network of chains of edge‐sharing Mn(1)O6, running along the c axis, connected by the apices of Mn(2)O6 and SO4 units. It is isostructural to the nickel analogue. Determination of the magnetic structure and measurements of magnetization and heat capacity indicate the coexistence of both magnetic long‐range ordering (LRO) and short‐range ordering (SRO) below a Néel temperature of 26 K, while the SRO is retained at higher temperatures. The moments of the two independent Mn atoms lie in the bc plane, and that of Mn(1) rotates continuously by 54° towards the c axis on decreasing the temperature from 25 to 1.4 K. While the SRO may be associated with frustration of the moments within a Mn3 trimer, the LRO is achieved by antiparallel alignment of the four symmetry‐related trimers within the magnetic unit cell. A spin‐flop field, measured by dc and ac magnetization on a SQUID, is observed at 15 kOe.

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DOI: 10.1002/chem.200305645


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<div type="abstract" xml:lang="en">[Mn3(OH)2(SO4)2(H2O)2] and its deuterated anlaogue were synthesized by a hydrothermal technique and characterized by differential thermal analysis, thermogravimetric analysis, and IR spectroscopy. Its nuclear structure, determined by single‐crystal X‐ray analysis and Rietveld analysis of neutron powder‐diffraction data, consists of a 3D network of chains of edge‐sharing Mn(1)O6, running along the c axis, connected by the apices of Mn(2)O6 and SO4 units. It is isostructural to the nickel analogue. Determination of the magnetic structure and measurements of magnetization and heat capacity indicate the coexistence of both magnetic long‐range ordering (LRO) and short‐range ordering (SRO) below a Néel temperature of 26 K, while the SRO is retained at higher temperatures. The moments of the two independent Mn atoms lie in the bc plane, and that of Mn(1) rotates continuously by 54° towards the c axis on decreasing the temperature from 25 to 1.4 K. While the SRO may be associated with frustration of the moments within a Mn3 trimer, the LRO is achieved by antiparallel alignment of the four symmetry‐related trimers within the magnetic unit cell. A spin‐flop field, measured by dc and ac magnetization on a SQUID, is observed at 15 kOe.</div>
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