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Fizika Tverdogo Tela, 2013 Volume 55, Issue 6, Pages 1103–1109 (Mi ftt12449)

This article is cited in 5 papers

Ferroelectricity

Mössbauer studies of PbFe$_{2/3}$W$_{1/3}$O$_3$ multiferroics

A. S. Kamzin, V. A. Bokov

Ioffe Institute, St. Petersburg

Abstract: Mössbauer studies of ceramic samples of the antiferromagnetic perovskite PbFe$_{2/3}$W$_{1/3}$O$_3$ have been carried out. It has been established that the temperature of transition to the magnetically ordered state is $T_{\mathrm{N}}$ = 365 K. Iron ions in PbFe$_{2/3}$W$_{1/3}$O$_3$ are found to reside in the high-spin Fe$^{3+}$ state. The Fe$^{3+}$ ions occupy inequivalent positions differing in the nearest cation environment, or more precisely, tungsten and iron ions are distributed in a random manner over the sites of the octahedral sublattice. The inequivalent positions arise as a result of the Fe and W ions being statistically distributed over the octahedral sublattice. For $T >$ 0 K, magnetic fields at the nuclei and, hence, the average thermodynamic values of the magnetic moments of Fe$^{3+}$ ions occupying inequivalent positions are different and, at a given temperature, are determined by the number of the nearest magnetic neighbors, with the effective magnetic fields $(H_{\mathrm{eff}})$ varying differently with temperature. As the temperature is lowered, the fields $H_{\mathrm{eff}}$ level off gradually in response to the effective magnetic fields of iron ions having different numbers of exchange bonds leveling off with decreasing temperature which lowers thermal excitation.

Received: 05.12.2012


 English version:
Physics of the Solid State, 2013, 55:6, 1191–1197

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