Abstract

Calculations are presented which support the view that the ferroelectric phase tnnnsition in gadolinium molybdate (GMO) arises from the softening and ultimate instability of a doubly degenerate zone-edge mode of the high- temperature paraelectric phase. A rigid-ion model was used in which the short- range force constants are obtained from a detailed knowledge of the crystal structure together wiih the conditions imposed by the requirement that the crystal must be in static equilibrium under the combined influence of both Coulomb and short-range forces. Results show that this type of approach is very useful when one is dealing with complex structures such as GMO, which has thirty- four ions per unit cell in the paraelectric phase. In view of the simplicity of the model, a surprisingly good correlation with experimental results was obtained. In particular, the calculated zone-center frequencies reproduce the basic features of the observed Raman spectruna. Dispersion curves are presented which show a pronounced softening of two phonon branches which become doubly degenerate at the M point, in agreement with inelastic neutron scattering. The displacements associated wiih the soft M-point modes correlate with the difference in the structures of the high- and low-temperature phases determined by x-ray diffraction. Thismore » provides further evidence that the ferroelectric domains in GMO are to be interpreted as frozen-in'' soft zoneboundary modes of the paraelectric phase. (auth)« less

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