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Raman study of LiTaO3-related non-stoichiometric solid solutions isolated inside the ternary systems Li2O-Ta2O5-(M'O)2 with M' = Mn, Co

Identifieur interne : 000065 ( Maroc/Analysis ); précédent : 000064; suivant : 000066

Raman study of LiTaO3-related non-stoichiometric solid solutions isolated inside the ternary systems Li2O-Ta2O5-(M'O)2 with M' = Mn, Co

Auteurs : A. Assani [Maroc] ; El. M. Lotfi [Maroc] ; P. Bourson [France] ; M. Aillerie [France] ; B. Lahbabi [Maroc] ; M. Zriouil [Maroc] ; B. Elouadi [France]

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RBID : Pascal:09-0307143

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Abstract

We have characterized by Raman spectroscopy the disorder and the local modifications of cation environment in the lithium tantalate structure resulting from the incorporation of bivalent cations Co2+ and Mn2+ as potential substitutes for Li and/or Ta ions. Frequency and damping of the E(TO1), E(T06) and E(TO8) phonon modes of ceramic powders are studied along seven lines in the ternary phase diagrams Li2O-Ta2O5-(M'O)2 with M' = Mn and Co, and compared to those of the pure stoichiometric LiTaO3. Raman spectroscopy is found to be very sensitive to the substitution ions and defects generated in the lattice vibration. Dopants occupy primarily the Li site in the region of lithium oxide excess. The site of Ta becomes progressively implicated in the substitution process when the concentration of dopant increases. In the Li-poor region of the ternary-phase diagram, corresponding to under- stoichiometric compositions, we retain the charge compensation mechanism involving both Li and Ta site according to: 3Li++Ta5+→4M'2+ with M'2+ = Mn2+ or Co2+.


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<title xml:lang="en" level="a">Raman study of LiTaO
<sub>3</sub>
-related non-stoichiometric solid solutions isolated inside the ternary systems Li
<sub>2</sub>
O-Ta
<sub>2</sub>
O
<sub>5</sub>
-(M'O)
<sub>2</sub>
with M' = Mn, Co</title>
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<title xml:lang="en" level="a">Raman study of LiTaO
<sub>3</sub>
-related non-stoichiometric solid solutions isolated inside the ternary systems Li
<sub>2</sub>
O-Ta
<sub>2</sub>
O
<sub>5</sub>
-(M'O)
<sub>2</sub>
with M' = Mn, Co</title>
<author>
<name sortKey="Assani, A" sort="Assani, A" uniqKey="Assani A" first="A." last="Assani">A. Assani</name>
<affiliation wicri:level="3">
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<s3>MAR</s3>
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<sZ>2 aut.</sZ>
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<settlement type="city">Rabat</settlement>
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<name sortKey="Bourson, P" sort="Bourson, P" uniqKey="Bourson P" first="P." last="Bourson">P. Bourson</name>
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<inist:fA14 i1="03">
<s1>Laboratoire Matériaux Optiques, Photonique et Systèmes, CNRS UMR 7132, Université Paul Verlaine de Metz-Supelec, 2 rue E. Belin</s1>
<s2>57070 Metz</s2>
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<s3>MAR</s3>
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<sZ>6 aut.</sZ>
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<region nuts="2">Rabat-Salé-Kénitra</region>
</placeName>
</affiliation>
</author>
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<sZ>7 aut.</sZ>
</inist:fA14>
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<series>
<title level="j" type="main">The Journal of physics and chemistry of solids</title>
<title level="j" type="abbreviated">J. phys. chem. solids</title>
<idno type="ISSN">0022-3697</idno>
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<title level="j" type="main">The Journal of physics and chemistry of solids</title>
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<keywords scheme="KwdEn" xml:lang="en">
<term>Charge compensation</term>
<term>Cobalt additions</term>
<term>Doping</term>
<term>Impurity density</term>
<term>Impurity site</term>
<term>Ion substitution</term>
<term>Lithium tantalates</term>
<term>Manganese additions</term>
<term>Phase diagrams</term>
<term>Phonon mode</term>
<term>Raman spectra</term>
<term>Vibrational modes</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr">
<term>Addition manganèse</term>
<term>Spectre Raman</term>
<term>Addition cobalt</term>
<term>Mode phonon</term>
<term>Diagramme phase</term>
<term>Substitution ion</term>
<term>Site impureté</term>
<term>Mode vibration</term>
<term>Dopage</term>
<term>Concentration impureté</term>
<term>Compensation charge</term>
<term>Tantalate de lithium</term>
</keywords>
<keywords scheme="Wicri" type="topic" xml:lang="fr">
<term>Dopage</term>
</keywords>
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<front>
<div type="abstract" xml:lang="en">We have characterized by Raman spectroscopy the disorder and the local modifications of cation environment in the lithium tantalate structure resulting from the incorporation of bivalent cations Co
<sup>2+</sup>
and Mn
<sup>2+</sup>
as potential substitutes for Li and/or Ta ions. Frequency and damping of the E(TO1), E(T06) and E(TO8) phonon modes of ceramic powders are studied along seven lines in the ternary phase diagrams Li
<sub>2</sub>
O-Ta
<sub>2</sub>
O
<sub>5</sub>
-(M'O)
<sub>2</sub>
with M' = Mn and Co, and compared to those of the pure stoichiometric LiTaO
<sub>3</sub>
. Raman spectroscopy is found to be very sensitive to the substitution ions and defects generated in the lattice vibration. Dopants occupy primarily the Li site in the region of lithium oxide excess. The site of Ta becomes progressively implicated in the substitution process when the concentration of dopant increases. In the Li-poor region of the ternary-phase diagram, corresponding to under- stoichiometric compositions, we retain the charge compensation mechanism involving both Li and Ta site according to: 3Li
<sup>+</sup>
+Ta
<sup>5+</sup>
→4M'
<sup>2+</sup>
with M'
<sup>2+</sup>
= Mn
<sup>2+</sup>
or Co
<sup>2+</sup>
.</div>
</front>
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<li>France</li>
<li>Maroc</li>
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<name sortKey="Lotfi, El M" sort="Lotfi, El M" uniqKey="Lotfi E" first="El. M." last="Lotfi">El. M. Lotfi</name>
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<name sortKey="Bourson, P" sort="Bourson, P" uniqKey="Bourson P" first="P." last="Bourson">P. Bourson</name>
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