Phase stability and non-stoichiometry in M-phase solid solutions in the system LiO0.5-NbO2.5-TiO2
Identifieur interne : 00AB51 ( Main/Exploration ); précédent : 00AB50; suivant : 00AB52Phase stability and non-stoichiometry in M-phase solid solutions in the system LiO0.5-NbO2.5-TiO2
Auteurs : I. E. Grey [Australie] ; P. Bordet [France] ; C. Li [Australie] ; R. S. Roth [États-Unis]Source :
- Journal of solid state chemistry : (Print) [ 0022-4596 ] ; 2004.
Descripteurs français
- Pascal (Inist)
- Etude expérimentale, Stabilité phase, Diagramme phase, Non stoechiométrie, Trempe, Composition chimique, Lacune, Paramètre cristallin, Dépendance température, Joint phase, Solution solide, Lithium oxyde, Niobium oxyde, Titane oxyde, Système ternaire, Réseau rhomboédrique, Structure corindon, Système LiO0,5 NbO2,5 TiO2, Li Nb O Ti, 8130D, 6166F.
English descriptors
- KwdEn :
Abstract
Phase relations at 1050°C have been determined for M-phase solid solutions in the LiO0.5-NbO2.5-TiO2 ternary phase system by the quench method. Rietveld analysis has been used to help determine phase boundaries and to study structure composition relations. The M-phases have trigonal structures based on intergrowth of corundum-like layers, [Ti2O3]2+, with slabs of (N-1) layers of LiNbO3-type parallel to (0001). Ideal compositions are defined along the pseudobinary join LiNbO3-Li4Ti5O12 by the homologous series formula LiNNbN-4Ti5O3N, N≥4. Homologues with N≤10 lie to the low-lithia side of the LiNbO3-Li4Ti5O12 join and show extended single-phase solid solution ranges separated by two-phase regions. The composition variations along the solid solutions are controlled by a major substitution mechanism, Li+ +3Nb5+ ↔4Ti4+, coupled with a minor substitution 4Li+ ↔ Ti4+ + 3□, where □=vacancy. The latter substitution results in increasing deviations from the stoichiometric compositions A2N+1O3N with increasing Ti substitution. The non-stoichiometry can be reduced by re-equilibration at lower temperatures. Expressions have been developed to describe the compositional changes along the solid solutions.
Affiliations:
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Le document en format XML
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-NbO<sub>2.5</sub>
-TiO<sub>2</sub>
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-TiO<sub>2</sub>
</title>
<author><name sortKey="Grey, I E" sort="Grey, I E" uniqKey="Grey I" first="I. E." last="Grey">I. E. Grey</name>
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<s2>Clayton South, Victoria 3168</s2>
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<country>Australie</country>
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<author><name sortKey="Bordet, P" sort="Bordet, P" uniqKey="Bordet P" first="P." last="Bordet">P. Bordet</name>
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<author><name sortKey="Li, C" sort="Li, C" uniqKey="Li C" first="C." last="Li">C. Li</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>CSIRO Minerals, Box 312</s1>
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<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
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<series><title level="j" type="main">Journal of solid state chemistry : (Print)</title>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Chemical composition</term>
<term>Corundum structure</term>
<term>Experimental study</term>
<term>Lattice parameters</term>
<term>Lithium oxides</term>
<term>Niobium oxides</term>
<term>Nonstoichiometry</term>
<term>Phase boundaries</term>
<term>Phase diagrams</term>
<term>Phase stability</term>
<term>Quenching</term>
<term>Solid solutions</term>
<term>Temperature dependence</term>
<term>Ternary systems</term>
<term>Titanium oxides</term>
<term>Trigonal lattices</term>
<term>Vacancies</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Etude expérimentale</term>
<term>Stabilité phase</term>
<term>Diagramme phase</term>
<term>Non stoechiométrie</term>
<term>Trempe</term>
<term>Composition chimique</term>
<term>Lacune</term>
<term>Paramètre cristallin</term>
<term>Dépendance température</term>
<term>Joint phase</term>
<term>Solution solide</term>
<term>Lithium oxyde</term>
<term>Niobium oxyde</term>
<term>Titane oxyde</term>
<term>Système ternaire</term>
<term>Réseau rhomboédrique</term>
<term>Structure corindon</term>
<term>Système LiO0,5 NbO2,5 TiO2</term>
<term>Li Nb O Ti</term>
<term>8130D</term>
<term>6166F</term>
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<front><div type="abstract" xml:lang="en">Phase relations at 1050°C have been determined for M-phase solid solutions in the LiO<sub>0.5</sub>
-NbO<sub>2.5</sub>
-TiO<sub>2</sub>
ternary phase system by the quench method. Rietveld analysis has been used to help determine phase boundaries and to study structure composition relations. The M-phases have trigonal structures based on intergrowth of corundum-like layers, [Ti<sub>2</sub>
O<sub>3</sub>
]<sup>2+</sup>
, with slabs of (N-1) layers of LiNbO<sub>3</sub>
-type parallel to (0001). Ideal compositions are defined along the pseudobinary join LiNbO<sub>3</sub>
-Li<sub>4</sub>
Ti<sub>5</sub>
O<sub>12</sub>
by the homologous series formula Li<sub>N</sub>
Nb<sub>N-4</sub>
Ti<sub>5</sub>
O<sub>3N</sub>
, N≥4. Homologues with N≤10 lie to the low-lithia side of the LiNbO<sub>3</sub>
-Li<sub>4</sub>
Ti<sub>5</sub>
O<sub>12</sub>
join and show extended single-phase solid solution ranges separated by two-phase regions. The composition variations along the solid solutions are controlled by a major substitution mechanism, Li<sup>+</sup>
+3Nb<sup>5+</sup>
↔4Ti<sup>4+</sup>
, coupled with a minor substitution 4Li<sup>+</sup>
↔ Ti<sup>4+</sup>
+ 3□, where □=vacancy. The latter substitution results in increasing deviations from the stoichiometric compositions A<sub>2N+1</sub>
O<sub>3N</sub>
with increasing Ti substitution. The non-stoichiometry can be reduced by re-equilibration at lower temperatures. Expressions have been developed to describe the compositional changes along the solid solutions.</div>
</front>
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<tree><country name="Australie"><noRegion><name sortKey="Grey, I E" sort="Grey, I E" uniqKey="Grey I" first="I. E." last="Grey">I. E. Grey</name>
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<country name="France"><region name="Auvergne-Rhône-Alpes"><name sortKey="Bordet, P" sort="Bordet, P" uniqKey="Bordet P" first="P." last="Bordet">P. Bordet</name>
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<country name="États-Unis"><noRegion><name sortKey="Roth, R S" sort="Roth, R S" uniqKey="Roth R" first="R. S." last="Roth">R. S. Roth</name>
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