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Electric conductivity of Fe2SiO4–Fe3O4 spinel solid solutions
Authors:T Yamanaka  H Shimazu  K Ota
Institution:(1) Department of Earth and Space Science, Graduate School of Science, Osaka University, 1-1 Machikaneyama Toyonaka, Osaka 560-0043, Japan e-mail: 61400@center.osaka-u.ac.jp Fax/Tel.: 081-6-6850-5793, JP;(2) Institute of Scientific and Industrial Researches, Osaka University, 1-1 Yamadaoka Suita, Osaka 565-0871, Japan, JP
Abstract: The spinel solid solution was found to exist in the whole range between Fe3O4 and γ-Fe2SiO4 at over 10 GPa. The resistivity of Fe3− x Si x O4 (0.0<x<0.288) was measured in the temperature range of 80∼300 K by the AC impedance method. Electron hopping between Fe3+ and Fe2+ in the octahedral site of iron-rich phases gives a large electric conductivity at room temperature. The activation energy of the electron hopping becomes larger with increasing γ-Fe2SiO4 component. A nonlinear change in electric conductivity is not simply caused by the statistical probability of Fe3+–Fe2+ electron hopping with increasing the total Si content. This is probably because a large number of Si4+ ions occupies the octahedral site and the adjacent Fe2+ keeping the local electric neutrality around Si4+ makes a cluster, which generates a local deformation by Si substitution. The temperature dependence of the conductivity of solid solutions indicates the Verwey transition temperature, which decreases from 124(±2) K at x=0 (Fe3O4) to 102(±5) K at x=0.288, and the electric conductivity gap at the transition temperature decreases with Si4+ substitution. Received: 15 March 2000 / Accepted: 4 September 2000
Keywords:  Fe3 –  xSixO4  Solid solution  Cation distribution  Electric conductivity  Verwey transition temperature  Nonstoichiometry
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