Structure and conductivity of B-site substituted (Li,La)TiO3

The crystal structure and the ionic and partial electronic conductivity of the LixLayMzTi1-xO3 (M = Ni, V, Cu, 0.25 < x/y < 1.44 and z = 0.0,0.,0.2) and of the LixLayCozTi1-zO3 (0.19 < or = x < or = 0.55; 0.55 < or = y < or = 0.8 and z = 0.0,0.1,0.30) systems, with perovskite-relat...

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Veröffentlicht in:Materials science & engineering. B, Solid-state materials for advanced technology Solid-state materials for advanced technology, 2004-10, Vol.113 (1), p.85-90
Hauptverfasser: Stramare, S., Weppner, W.
Format: Artikel
Sprache:eng
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Zusammenfassung:The crystal structure and the ionic and partial electronic conductivity of the LixLayMzTi1-xO3 (M = Ni, V, Cu, 0.25 < x/y < 1.44 and z = 0.0,0.,0.2) and of the LixLayCozTi1-zO3 (0.19 < or = x < or = 0.55; 0.55 < or = y < or = 0.8 and z = 0.0,0.1,0.30) systems, with perovskite-related structure, have been studied. Partial substitution (5,10 and 30%) of Ti4+ ions by slightly larger Co2+ and Ni2+ ions was found to stabilise the cubic perovskite structure (S.G. Pm3m; Co, a = 3.88450(6) A and Ni, a = 3.8849(1) A), with one exception (Li0.19La0.67Co0.1Ti0.9O3) giving a tetragonal symmetry plus supercell reflections.
ISSN:0921-5107
DOI:10.1016/j.mseb.2004.07.003