Li Mobility in the Orthorhombic Li0.18La0.61TiO3 Perovskite Studied by NMR and Impedance Spectroscopies

Electrical conductivity and NMR relaxation times (T 1 and T 2) have been determined in the Li0.18La0.61TiO3 perovskite. At room temperature, the unit cell constants are a = 3.865(1), b = 3.876(1), and c = 7.788(2) Å and the space group Pmmm (orthorhombic). In this doubled perovskite, the Rietveld an...

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Veröffentlicht in:Chemistry of materials 2000-06, Vol.12 (6), p.1694-1701
Hauptverfasser: París, M. A, Sanz, J, León, C, Santamaría, J, Ibarra, J, Várez, A
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Sprache:eng
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Zusammenfassung:Electrical conductivity and NMR relaxation times (T 1 and T 2) have been determined in the Li0.18La0.61TiO3 perovskite. At room temperature, the unit cell constants are a = 3.865(1), b = 3.876(1), and c = 7.788(2) Å and the space group Pmmm (orthorhombic). In this doubled perovskite, the Rietveld analysis of the X-ray powder pattern showed that La ions occupy preferentially one type of sites (z/c = 0), and Li and vacancies accommodate with the remaining La at the second site (z/c = 0.5). From this fact, Li motion should be favored in the plane ab; however, exchanges of Li between contiguous layers are detected above 200 K by NMR spectroscopy. From T 1 and T 2 NMR data, two main relaxation mechanisms have been detected, which have been ascribed to localized exchanges (200−273 K) and extended motions of Li (above 273 K). The dc conductivity shows a non-Arrhenius temperature dependence, and local activation energies of 0.41 and 0.26 eV were obtained in the low- and high-temperature ranges, respectively. Both NMR and electrical conductivity relaxations are described by “stretched exponential” functions, characteristic of correlated ion motions.
ISSN:0897-4756
1520-5002
DOI:10.1021/cm9911159