Abstract
In addition to the dielectric relaxation around 170 K in the cubic structure of Sr1−3x/2LaxTiO3, a similar relaxation was observed at about 70 K in the tetragonal structure with an activation energy in the range 0.13–0.16 eV which increases as x in Sr1−3x/2LaxTiO3 varies from 0.60–3.00 at%. This relaxation is explained by Skanavi's model and is discussed in terms of thermal motions of Ti4+ between potential minima produced by lattice distortions in the tetragonal structure. In order to provide a direct evidence for the suggestion that the dielectric relaxation around 170 K in the cubic is due to thermal motions of Ti4+, dielectric properties on manganese-doped specimens, Sr1−3x/2LaxMnyTi1−y),O3 with x=1.40×10−2 and y=0.1×10−2, were investigated because Mn4+ substitutes for Ti4+. As well as the relaxation due to Ti4+, this specimen exhibits another peak due to Mn4+ with an activation energy somewhat smaller than that of Ti4+. The activation energies and the relative intensity of these relaxation processes are explained by the difference in ionic radii of Mn4+ and Ti4+ and the difference in formation energies of a strontium vacancy adjacent to Mn4+ and that to Ti4+, which were calculated theoretically using a shell model.
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Iguchi, E., Lee, K.J. Dielectric relaxations in SrTiO3 doped with La2O3 and MnO2 at low temperatures. JOURNAL OF MATERIAL SCIENCE 28, 5809–5813 (1993). https://doi.org/10.1007/BF00365185
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DOI: https://doi.org/10.1007/BF00365185