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

Identifieur interne : 001048 ( Istex/Corpus ); précédent : 001047; suivant : 001049

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

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

Source :

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.

Url:
DOI: 10.1002/chem.200305645

Links to Exploration step

ISTEX:EC88300ECDF9D384AE6091F55E31582693F09D9A

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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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<p>[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.</p>
</abstract>
<abstract xml:lang="fr">
<p>[Mn3(OH)2(SO4)2(H2O)2] et son équivalent deutérié ont été préparés par synthèse hydrothermale et caractérisés par ATG‐ATD et spectroscopie infrarouge. Sa structure, affinée à partir de données de diffraction RX sur monocristal, est analogue à celle du sel de nickel correspondant et fait apparaître un réseau 3D formé par des chaînes d′octaèdres Mn(1)O6 liés par une arête, chaînes connectées entre elles par un sommet commun à des octaèdres Mn(2)O6 et des tétraèdres SO4. La détermination de la structure magnétique et les mesures des propriétés magnétiques et de chaleur spécifique indiquent la coexistence d′un ordre magnétique à longue distance (LRO) et à courte distance (SRO) en‐dessous de la température de Néel TN de 26 K, l′ordre à courte distance s′établissant à plus haute température. Les moments magnétiques des deux atomes Mn indépendants se trouvent dans le plan bc. Alors que celui de Mn(2) est toujours dirigé selon l′axe c, celui de Mn(1) se rapproche progressivement de cette direction lorsque la température est abaissée de TN à 1,4 K, la rotation globale étant de 54°. Alors que l′ordre à courte distance peut être dû à la frustation des moments à l′intérieur des trimères Mn3, en interaction antiferromagnétique, l′ordre à longue distance résulte de l′alignement antiparallèle des quatre trimères de la maille magnétique. Un champ de spin‐flop, mesuré par aimantation dc et ac, est observé à 15 kOe.</p>
</abstract>
<abstract>
<p>Both long‐ and short‐range magnetic ordering below its Néel temperature of 26 K are exhibited by [Mn3(OH)2(SO4)2(H2O)2], which was obtained by hydrothermal synthesis and characterized by X‐ray and neutron diffraction. The crystal structure consists of a three‐dimensional arrangement of MnO6, μ3‐OH, and μ4‐SO4 units. In the magnetic structure (see picture), the moments lie in the bc plane, and the moment of Mn(1) rotates from 74 to 20° with respect to the c axis on cooling from 26 to 1.4 K, while that of Mn(2) remains along the c axis.</p>
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<title type="main" xml:lang="en">Synthesis, Nuclear, and Magnetic Structures and Magnetic Properties of [Mn
<sub>3</sub>
(OH)
<sub>2</sub>
(SO
<sub>4</sub>
)
<sub>2</sub>
(H
<sub>2</sub>
O)
<sub>2</sub>
]</title>
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<givenNames>Mohsen</givenNames>
<familyName>Ben Salah</familyName>
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<personName>
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<givenNames>Gilles</givenNames>
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<familyName>Richard‐Plouet</familyName>
<degrees>Dr.</degrees>
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<givenNames>Françoise</givenNames>
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<p>Supporting information for this article is available on the WWW under
<url href="http://www.wiley-vch.de/contents/jc_2111/2004/f5645_s.pdf">http://www.wiley‐vch.de/contents/jc_2111/2004/f5645_s.pdf</url>
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<p>[Mn
<sub>3</sub>
(OH)
<sub>2</sub>
(SO
<sub>4</sub>
)
<sub>2</sub>
(H
<sub>2</sub>
O)
<sub>2</sub>
] 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)O
<sub>6</sub>
, running along the
<i>c</i>
axis, connected by the apices of Mn(2)O
<sub>6</sub>
and SO
<sub>4</sub>
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
<i>bc</i>
plane, and that of Mn(1) rotates continuously by 54° towards the
<i>c</i>
axis on decreasing the temperature from 25 to 1.4 K. While the SRO may be associated with frustration of the moments within a Mn
<sub>3</sub>
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.</p>
</abstract>
<abstract type="main" xml:lang="fr">
<p>
<i>[Mn</i>
<sub>
<i>3</i>
</sub>
<i>(OH)</i>
<sub>
<i>2</i>
</sub>
<i>(SO</i>
<sub>
<i>4</i>
</sub>
<i>)</i>
<sub>
<i>2</i>
</sub>
<i>(H</i>
<sub>
<i>2</i>
</sub>
<i>O)</i>
<sub>
<i>2</i>
</sub>
<i>] et son équivalent deutérié ont été préparés par synthèse hydrothermale et caractérisés par ATG‐ATD et spectroscopie infrarouge</i>
.
<i>Sa structure</i>
,
<i>affinée à partir de données de diffraction RX sur monocristal</i>
,
<i>est analogue à celle du sel de nickel correspondant et fait apparaître un réseau 3D formé par des chaînes d′octaèdres Mn(1)O</i>
<sub>
<i>6</i>
</sub>
<i>liés par une arête</i>
,
<i>chaînes connectées entre elles par un sommet commun à des octaèdres Mn(2)O</i>
<sub>
<i>6</i>
</sub>
<i>et des tétraèdres SO</i>
<sub>
<i>4</i>
</sub>
.
<i>La détermination de la structure magnétique et les mesures des propriétés magnétiques et de chaleur spécifique indiquent la coexistence d′un ordre magnétique à longue distance (LRO) et à courte distance (SRO) en‐dessous de la température de Néel</i>
T
<sub>
<i>N</i>
</sub>
<i>de 26 K</i>
,
<i>l′ordre à courte distance s′établissant à plus haute température</i>
.
<i>Les moments magnétiques des deux atomes Mn indépendants se trouvent dans le plan bc</i>
.
<i>Alors que celui de Mn(2) est toujours dirigé selon l′axe c</i>
,
<i>celui de Mn(1) se rapproche progressivement de cette direction lorsque la température est abaissée de</i>
T
<sub>
<i>N</i>
</sub>
<i>à 1</i>
,
<i>4 K</i>
,
<i>la rotation globale étant de 54°</i>
.
<i>Alors que l′ordre à courte distance peut être dû à la frustation des moments à l′intérieur des trimères Mn</i>
<sub>
<i>3</i>
</sub>
,
<i>en interaction antiferromagnétique</i>
,
<i>l′ordre à longue distance résulte de l′alignement antiparallèle des quatre trimères de la maille magnétique</i>
.
<i>Un champ de spin‐flop</i>
,
<i>mesuré par aimantation dc et ac</i>
,
<i>est observé à 15 kOe</i>
.</p>
</abstract>
<abstract type="graphical" xml:lang="en">
<p>
<b>Both long‐ and short‐range magnetic ordering</b>
below its Néel temperature of 26 K are exhibited by [Mn
<sub>3</sub>
(OH)
<sub>2</sub>
(SO
<sub>4</sub>
)
<sub>2</sub>
(H
<sub>2</sub>
O)
<sub>2</sub>
], which was obtained by hydrothermal synthesis and characterized by X‐ray and neutron diffraction. The crystal structure consists of a three‐dimensional arrangement of MnO
<sub>6</sub>
, μ
<sub>3</sub>
‐OH, and μ
<sub>4</sub>
‐SO
<sub>4</sub>
units. In the magnetic structure (see picture), the moments lie in the
<i>bc</i>
plane, and the moment of Mn(1) rotates from 74 to 20° with respect to the
<i>c</i>
axis on cooling from 26 to 1.4 K, while that of Mn(2) remains along the
<i>c</i>
axis.
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<abstract 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.</abstract>
<abstract lang="fr">[Mn3(OH)2(SO4)2(H2O)2] et son équivalent deutérié ont été préparés par synthèse hydrothermale et caractérisés par ATG‐ATD et spectroscopie infrarouge. Sa structure, affinée à partir de données de diffraction RX sur monocristal, est analogue à celle du sel de nickel correspondant et fait apparaître un réseau 3D formé par des chaînes d′octaèdres Mn(1)O6 liés par une arête, chaînes connectées entre elles par un sommet commun à des octaèdres Mn(2)O6 et des tétraèdres SO4. La détermination de la structure magnétique et les mesures des propriétés magnétiques et de chaleur spécifique indiquent la coexistence d′un ordre magnétique à longue distance (LRO) et à courte distance (SRO) en‐dessous de la température de Néel TN de 26 K, l′ordre à courte distance s′établissant à plus haute température. Les moments magnétiques des deux atomes Mn indépendants se trouvent dans le plan bc. Alors que celui de Mn(2) est toujours dirigé selon l′axe c, celui de Mn(1) se rapproche progressivement de cette direction lorsque la température est abaissée de TN à 1,4 K, la rotation globale étant de 54°. Alors que l′ordre à courte distance peut être dû à la frustation des moments à l′intérieur des trimères Mn3, en interaction antiferromagnétique, l′ordre à longue distance résulte de l′alignement antiparallèle des quatre trimères de la maille magnétique. Un champ de spin‐flop, mesuré par aimantation dc et ac, est observé à 15 kOe.</abstract>
<abstract>Both long‐ and short‐range magnetic ordering below its Néel temperature of 26 K are exhibited by [Mn3(OH)2(SO4)2(H2O)2], which was obtained by hydrothermal synthesis and characterized by X‐ray and neutron diffraction. The crystal structure consists of a three‐dimensional arrangement of MnO6, μ3‐OH, and μ4‐SO4 units. In the magnetic structure (see picture), the moments lie in the bc plane, and the moment of Mn(1) rotates from 74 to 20° with respect to the c axis on cooling from 26 to 1.4 K, while that of Mn(2) remains along the c axis.</abstract>
<subject lang="en">
<genre>keywords</genre>
<topic>hydrothermal synthesis</topic>
<topic>hydroxide sulfates</topic>
<topic>magnetic properties</topic>
<topic>manganese</topic>
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<topic>Full Paper</topic>
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<identifier type="ISSN">0947-6539</identifier>
<identifier type="eISSN">1521-3765</identifier>
<identifier type="DOI">10.1002/(ISSN)1521-3765</identifier>
<identifier type="PublisherID">CHEM</identifier>
<part>
<date>2004</date>
<detail type="volume">
<caption>vol.</caption>
<number>10</number>
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<detail type="issue">
<caption>no.</caption>
<number>8</number>
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<start>2048</start>
<end>2057</end>
<total>10</total>
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<identifier type="DOI">10.1002/chem.200305645</identifier>
<identifier type="ArticleID">CHEM200305645</identifier>
<accessCondition type="use and reproduction" contentType="copyright">Copyright © 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim</accessCondition>
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<recordOrigin>WILEY‐VCH Verlag</recordOrigin>
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