Serveur d'exploration sur le cobalt au Maghreb

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LiCo2As3O10: une nouvelle structure à tunnels inter­connectés

Identifieur interne : 000187 ( Pmc/Checkpoint ); précédent : 000186; suivant : 000188

LiCo2As3O10: une nouvelle structure à tunnels inter­connectés

Auteurs : Youssef Ben Smida [Tunisie] ; Abderrahmen Guesmi [Tunisie] ; Ahmed Driss [Tunisie]

Source :

RBID : PMC:3684868

Abstract

The title compound, lithium dicobalt(II) triarsenate, LiCo2As3O10, was synthesized by a solid-state reaction. The As atoms and four out of seven O atoms lie on special positions, all with site symmetry m. The Li atoms are disordered over two independent special (site symmetry -1) and general positions with occupancies of 0.54 (7) and 0.23 (4), respectively. The structure model is supported by bond-valence-sum (BVS) and charge-distribution (CHARDI) methods. The structure can be described as a three-dimensional framework constructed from bi-octahedral Co2O10 dimers edge-connected to As3O10 groups. It delimits two sets of tunnels, running parallel to the a and b axes, the latter being the larger. The Li+ ions are located within the inter­sections of the tunnels. The possible motion of the alkali cations has been investigated by means of the BVS model. This simulation shows that the Li+ motion appears to be easier mainly along the b-axis direction and that this material may possess inter­esting conduction properties.


Url:
DOI: 10.1107/S1600536813013548
PubMed: 23794970
PubMed Central: 3684868


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Le document en format XML

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<sub>2</sub>
As
<sub>3</sub>
O
<sub>10</sub>
: une nouvelle structure à tunnels inter­connectés</title>
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As
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: une nouvelle structure à tunnels inter­connectés</title>
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<country>Tunisia</country>
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<p>The title compound, lithium dicobalt(II) triarsenate, LiCo
<sub>2</sub>
As
<sub>3</sub>
O
<sub>10</sub>
, was synthesized by a solid-state reaction. The As atoms and four out of seven O atoms lie on special positions, all with site symmetry
<italic>m</italic>
. The Li atoms are disordered over two independent special (site symmetry -1) and general positions with occupancies of 0.54 (7) and 0.23 (4), respectively. The structure model is supported by bond-valence-sum (BVS) and charge-distribution (CHARDI) methods. The structure can be described as a three-dimensional framework constructed from bi-octahedral Co
<sub>2</sub>
O
<sub>10</sub>
dimers edge-connected to As
<sub>3</sub>
O
<sub>10</sub>
groups. It delimits two sets of tunnels, running parallel to the
<italic>a</italic>
and
<italic>b</italic>
axes, the latter being the larger. The Li
<sup>+</sup>
ions are located within the inter­sections of the tunnels. The possible motion of the alkali cations has been investigated by means of the BVS model. This simulation shows that the Li
<sup>+</sup>
motion appears to be easier mainly along the
<italic>b</italic>
-axis direction and that this material may possess inter­esting conduction properties.</p>
</div>
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<journal-id journal-id-type="nlm-ta">Acta Crystallogr Sect E Struct Rep Online</journal-id>
<journal-id journal-id-type="iso-abbrev">Acta Crystallogr Sect E Struct Rep Online</journal-id>
<journal-id journal-id-type="publisher-id">Acta Cryst. E</journal-id>
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<journal-title>Acta Crystallographica Section E: Structure Reports Online</journal-title>
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<issn pub-type="epub">1600-5368</issn>
<publisher>
<publisher-name>International Union of Crystallography</publisher-name>
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<article-id pub-id-type="pmid">23794970</article-id>
<article-id pub-id-type="pmc">3684868</article-id>
<article-id pub-id-type="publisher-id">br2224</article-id>
<article-id pub-id-type="doi">10.1107/S1600536813013548</article-id>
<article-id pub-id-type="coden">ACSEBH</article-id>
<article-id pub-id-type="pii">S1600536813013548</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Inorganic Papers</subject>
</subj-group>
</article-categories>
<title-group>
<article-title>LiCo
<sub>2</sub>
As
<sub>3</sub>
O
<sub>10</sub>
: une nouvelle structure à tunnels inter­connectés</article-title>
<alt-title>
<italic>LiCo
<sub>2</sub>
As
<sub>3</sub>
O
<sub>10</sub>
</italic>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name>
<surname>Ben Smida</surname>
<given-names>Youssef</given-names>
</name>
<xref ref-type="aff" rid="a">a</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Guesmi</surname>
<given-names>Abderrahmen</given-names>
</name>
<xref ref-type="aff" rid="a">a</xref>
<xref ref-type="aff" rid="b">b</xref>
<xref ref-type="corresp" rid="cor">*</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Driss</surname>
<given-names>Ahmed</given-names>
</name>
<xref ref-type="aff" rid="a">a</xref>
</contrib>
<aff id="a">
<label>a</label>
Laboratoire de Matériaux et Cristallochimie, Faculté des Sciences, El Manar II, 2092 Tunis,
<country>Tunisia</country>
</aff>
<aff id="b">
<label>b</label>
Institut Préparatoire aux Etudes d’Ingénieurs d’El Manar, BP 244 El Manar II, 2092 Tunis,
<country>Tunisia</country>
</aff>
</contrib-group>
<author-notes>
<corresp id="cor">Correspondence e-mail:
<email>abderrahmen.guesmi@ipeim.rnu.tn</email>
</corresp>
</author-notes>
<pub-date pub-type="collection">
<day>01</day>
<month>6</month>
<year>2013</year>
</pub-date>
<pub-date pub-type="epub">
<day>31</day>
<month>5</month>
<year>2013</year>
</pub-date>
<pub-date pub-type="pmc-release">
<day>31</day>
<month>5</month>
<year>2013</year>
</pub-date>
<pmc-comment> PMC Release delay is 0 months and 0 days and was based on the . </pmc-comment>
<volume>69</volume>
<issue>Pt 6</issue>
<issue-id pub-id-type="publisher-id">e130600</issue-id>
<fpage>i39</fpage>
<lpage>i39</lpage>
<history>
<date date-type="received">
<day>18</day>
<month>3</month>
<year>2013</year>
</date>
<date date-type="accepted">
<day>16</day>
<month>5</month>
<year>2013</year>
</date>
</history>
<permissions>
<copyright-statement>© Ben Smida et al. 2013</copyright-statement>
<copyright-year>2013</copyright-year>
<license license-type="open-access" xlink:href="http://creativecommons.org/licenses/by/2.0/uk/">
<license-p>This is an open-access article distributed under the terms of the Creative Commons Attribution Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.</license-p>
</license>
</permissions>
<self-uri xlink:type="simple" xlink:href="http://dx.doi.org/10.1107/S1600536813013548">A full version of this article is available from Crystallography Journals Online.</self-uri>
<abstract>
<p>The title compound, lithium dicobalt(II) triarsenate, LiCo
<sub>2</sub>
As
<sub>3</sub>
O
<sub>10</sub>
, was synthesized by a solid-state reaction. The As atoms and four out of seven O atoms lie on special positions, all with site symmetry
<italic>m</italic>
. The Li atoms are disordered over two independent special (site symmetry -1) and general positions with occupancies of 0.54 (7) and 0.23 (4), respectively. The structure model is supported by bond-valence-sum (BVS) and charge-distribution (CHARDI) methods. The structure can be described as a three-dimensional framework constructed from bi-octahedral Co
<sub>2</sub>
O
<sub>10</sub>
dimers edge-connected to As
<sub>3</sub>
O
<sub>10</sub>
groups. It delimits two sets of tunnels, running parallel to the
<italic>a</italic>
and
<italic>b</italic>
axes, the latter being the larger. The Li
<sup>+</sup>
ions are located within the inter­sections of the tunnels. The possible motion of the alkali cations has been investigated by means of the BVS model. This simulation shows that the Li
<sup>+</sup>
motion appears to be easier mainly along the
<italic>b</italic>
-axis direction and that this material may possess inter­esting conduction properties.</p>
</abstract>
</article-meta>
</front>
</pmc>
<affiliations>
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</orgName>
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