Syntheses and crystal structures of new vanadium(IV) oxyphosphates M(VO)2(PO4)2 with M = Co, Ni
Identifieur interne : 000138 ( France/Analysis ); précédent : 000137; suivant : 000139Syntheses and crystal structures of new vanadium(IV) oxyphosphates M(VO)2(PO4)2 with M = Co, Ni
Auteurs : S. Kaoua [Maroc] ; P. Gravereau [France] ; J. P. Chaminade [France] ; S. Pechev [France] ; S. Krimi [Maroc] ; A. El Jazouli [Maroc]Source :
- Solid state sciences [ 1293-2558 ] ; 2009.
Descripteurs français
- Pascal (Inist)
- Wicri :
English descriptors
- KwdEn :
Abstract
We have extended our research interest on titanium oxyphosphates (MII(TiO)2(PO4)2, with MII = Mg, Fe, Co, Ni, Cu, Zn) to vanadium oxyphosphates MII(VIVO)2(PO4)2 (MII=Co, Ni). For each compound two phases, named a and β according to synthesis conditions, have been stabilized at room temperature, then characterized. The four crystal structures M(VO)2(PO4)2 (a and β for M = Co, Ni) have been determined in monoclinic P21/c space group using X-ray single crystals diffraction data. Structure of the a phase is derived from the Lí(TiO)(PO4) (orthorhombic Pnma) and LiNi0.50(TiO)2(PO4)2 (monoclinic P21/c) types, with cell parameters: a=6.310(1)Å, b=7.273(1)Å, c=7.432(1)Å, β=90.43(1)° for M=Co, and a = 6.297(2) A, b = 7.230(2) A, c = 7.421(2) A, β = 90.36(2)° for M = Ni. Structure of the β phase is derived from the Ni(TiO)2(PO4)2-tyPe (monoclinic P21/c) with cell parameters: a=7.2742(2) Å, b=7.2802(2)Å, c = 7.4550(2) A β=120.171(2)° for M = Co, and a = 7.2691(2) A, b = 7.2366(2) A c = 7.4453(2) A, β = 120.231(2)° for M = Ni. All these structures consist of a three dimensional (3D) framework built up of infinite chains of tilted corner-sharing [VO6] octahedra, cross-linked by corner-sharing [PO4] tetrahedra. The M2+ ion (M = Co, Ni) is located in a triangular based antiprism which shares faces with two [VO6] octahedra. Structural filiation is discussed based on a common structural unit, a sheet where divalent cations M2+ (M = Co, Ni) are inserted. A thermal study of the a ↔ β transition is also presented.
Affiliations:
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(PO<sub>4</sub>
)<sub>2</sub>
with M = Co, Ni</title>
<author><name sortKey="Kaoua, S" sort="Kaoua, S" uniqKey="Kaoua S" first="S." last="Kaoua">S. Kaoua</name>
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<author><name sortKey="Chaminade, J P" sort="Chaminade, J P" uniqKey="Chaminade J" first="J. P." last="Chaminade">J. P. Chaminade</name>
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<author><name sortKey="Pechev, S" sort="Pechev, S" uniqKey="Pechev S" first="S." last="Pechev">S. Pechev</name>
<affiliation wicri:level="4"><inist:fA14 i1="02"><s1>Institut de Chimie de la Matière Condensée de Bordeaux (ICMCB-CNRS), Université Bordeaux I</s1>
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<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Laboratoire de Physico Chimie des Matériaux Inorganiques, Faculté des Sciences Aïn Chock</s1>
<s2>Casablanca</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
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</inist:fA14>
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</affiliation>
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<author><name sortKey="El Jazouli, A" sort="El Jazouli, A" uniqKey="El Jazouli A" first="A." last="El Jazouli">A. El Jazouli</name>
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<series><title level="j" type="main">Solid state sciences</title>
<title level="j" type="abbreviated">Solid state sci.</title>
<idno type="ISSN">1293-2558</idno>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Ambient temperature</term>
<term>Beta phase</term>
<term>Copper</term>
<term>Cross-linking</term>
<term>Crystal structure</term>
<term>Iron</term>
<term>Lattice parameters</term>
<term>Monoclinic lattices</term>
<term>Monocrystals</term>
<term>Nickel</term>
<term>Orthorhombic lattices</term>
<term>Space groups</term>
<term>Structural unit</term>
<term>Titanium</term>
<term>Titanium oxide</term>
<term>Vanadium</term>
<term>XRD</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Structure cristalline</term>
<term>Titane</term>
<term>Phase bêta</term>
<term>Température ambiante</term>
<term>Réseau monoclinique</term>
<term>Groupe espace</term>
<term>Diffraction RX</term>
<term>Réseau orthorhombique</term>
<term>Paramètre cristallin</term>
<term>Réticulation</term>
<term>Motif structural</term>
<term>Monocristal</term>
<term>Vanadium</term>
<term>Nickel</term>
<term>Oxyde de titane</term>
<term>Fer</term>
<term>Cuivre</term>
<term>Ti</term>
<term>LiNi0.50(TiO)2(PO4)2</term>
<term>8120K</term>
<term>6166F</term>
</keywords>
<keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Titane</term>
<term>Vanadium</term>
<term>Nickel</term>
<term>Fer</term>
<term>Cuivre</term>
</keywords>
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<front><div type="abstract" xml:lang="en">We have extended our research interest on titanium oxyphosphates (M<sup>II</sup>
(TiO)<sub>2</sub>
(PO<sub>4</sub>
)<sub>2</sub>
, with M<sup>II</sup>
= Mg, Fe, Co, Ni, Cu, Zn) to vanadium oxyphosphates M<sup>II</sup>
(V<sup>IV</sup>
O)<sub>2</sub>
(PO<sub>4</sub>
)<sub>2</sub>
(M<sup>II</sup>
=Co, Ni). For each compound two phases, named a and β according to synthesis conditions, have been stabilized at room temperature, then characterized. The four crystal structures M(VO)<sub>2</sub>
(PO<sub>4</sub>
)<sub>2</sub>
(a and β for M = Co, Ni) have been determined in monoclinic P2<sub>1</sub>
/c space group using X-ray single crystals diffraction data. Structure of the a phase is derived from the Lí(TiO)(PO<sub>4</sub>
) (orthorhombic Pnma) and LiNi<sub>0.50</sub>
(TiO)<sub>2</sub>
(PO<sub>4</sub>
)<sub>2</sub>
(monoclinic P2<sub>1</sub>
/c) types, with cell parameters: a=6.310(1)Å, b=7.273(1)Å, c=7.432(1)Å, β=90.43(1)° for M=Co, and a = 6.297(2) A, b = 7.230(2) A, c = 7.421(2) A, β = 90.36(2)° for M = Ni. Structure of the β phase is derived from the Ni(TiO)<sub>2</sub>
(PO<sub>4</sub>
)<sub>2</sub>
-tyPe (monoclinic P2<sub>1</sub>
/c) with cell parameters: a=7.2742(2) Å, b=7.2802(2)Å, c = 7.4550(2) A β=120.171(2)° for M = Co, and a = 7.2691(2) A, b = 7.2366(2) A c = 7.4453(2) A, β = 120.231(2)° for M = Ni. All these structures consist of a three dimensional (3D) framework built up of infinite chains of tilted corner-sharing [VO<sub>6</sub>
] octahedra, cross-linked by corner-sharing [PO<sub>4</sub>
] tetrahedra. The M<sup>2+</sup>
ion (M = Co, Ni) is located in a triangular based antiprism which shares faces with two [VO<sub>6</sub>
] octahedra. Structural filiation is discussed based on a common structural unit, a sheet where divalent cations M<sup>2+</sup>
(M = Co, Ni) are inserted. A thermal study of the a ↔ β transition is also presented.</div>
</front>
</TEI>
<affiliations><list><country><li>France</li>
<li>Maroc</li>
</country>
<region><li>Aquitaine</li>
<li>Nouvelle-Aquitaine</li>
</region>
<settlement><li>Pessac</li>
</settlement>
<orgName><li>Université Bordeaux I</li>
</orgName>
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<tree><country name="Maroc"><noRegion><name sortKey="Kaoua, S" sort="Kaoua, S" uniqKey="Kaoua S" first="S." last="Kaoua">S. Kaoua</name>
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<name sortKey="El Jazouli, A" sort="El Jazouli, A" uniqKey="El Jazouli A" first="A." last="El Jazouli">A. El Jazouli</name>
<name sortKey="Krimi, S" sort="Krimi, S" uniqKey="Krimi S" first="S." last="Krimi">S. Krimi</name>
</country>
<country name="France"><region name="Nouvelle-Aquitaine"><name sortKey="Gravereau, P" sort="Gravereau, P" uniqKey="Gravereau P" first="P." last="Gravereau">P. Gravereau</name>
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<name sortKey="Chaminade, J P" sort="Chaminade, J P" uniqKey="Chaminade J" first="J. P." last="Chaminade">J. P. Chaminade</name>
<name sortKey="Pechev, S" sort="Pechev, S" uniqKey="Pechev S" first="S." last="Pechev">S. Pechev</name>
</country>
</tree>
</affiliations>
</record>
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