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hal.structure.identifierLaboratoire de Physico-Chimie des Matériaux Inorganiques
dc.contributor.authorKAOUA, S.
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorGRAVEREAU, Pierre
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorCHAMINADE, Jean-Pierre
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorPECHEV, Stanislav
hal.structure.identifierLaboratoire de Physico-Chimie des Matériaux Inorganiques
dc.contributor.authorKRIMI, S.
hal.structure.identifierLaboratoire de Chimie des Matériaux Solides
dc.contributor.authorEL JAZOULI, Abdelaziz
dc.date.issued2009
dc.identifier.issn1293-2558
dc.description.abstractEnWe 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 α 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> (α and β for M = Co, Ni) have been determined in monoclinic <i>P</i>2<sub>1</sub>/<i>c</i> space group using X-ray single crystals diffraction data. Structure of the α phase is derived from the Li(TiO)(PO<sub>4</sub>) (orthorhombic <i>Pnma</i>) and LiNi<sub>0.50</sub>(TiO)<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub> (monoclinic <i>P</i>2<sub>1</sub>/<i>c</i>) types, with cell parameters: <i>a</i> = 6.310(1) Å, <i>b</i> = 7.273(1) Å, <i>c</i> = 7.432(1) Å, <i>β</i> = 90.43(1)° for M = Co, and <i>a</i> = 6.297(2) Å, <i>b</i> = 7.230(2) Å, <i>c</i> = 7.421(2) Å, <i>β</i> = 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 <i>P</i>2<sub>1</sub>/<i>c</i>) with cell parameters: <i>a</i> = 7.2742(2) Å, <i>b</i> = 7.2802(2) Å, <i>c</i> = 7.4550(2) Å, <i>β</i> = 120.171(2)° for M = Co, and <i>a</i> = 7.2691(2) Å, <i>b</i> = 7.2366(2) Å, <i>c</i> = 7.4453(2) Å, <i>β</i> = 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 α ↔ β transition is also presented.
dc.language.isoen
dc.publisherElsevier
dc.subject.enCo(VO)<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>
dc.subject.enNi(VO)<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub>
dc.subject.enVanadium(IV) oxyphosphate compound
dc.subject.enSingle crystal and powder X-ray diffraction
dc.title.enSyntheses and crystal structures of new vanadium(IV) oxyphosphates M(VO)<sub>2</sub>(PO<sub>4</sub>)<sub>2</sub> with M = Co, Ni
dc.typeArticle de revue
dc.identifier.doi10.1016/j.solidstatesciences.2008.11.011
dc.subject.halChimie/Matériaux
bordeaux.journalSolid State Sciences
bordeaux.page628-634
bordeaux.volume11
bordeaux.issue3
bordeaux.peerReviewedoui
hal.identifierhal-00367469
hal.version1
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-00367469v1
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