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This paper is concerned with the derivation of selection rules for light scattering by soft modes in displacive incommensurate structures, when the latter result from the condensation of a single pair of non-degenerate modes at q 0 and -q 0 , the high-temperature phase being centrosymmetric. The analysis is based on a direct second-order high-temperature Raman process involving the soft modes which condense at the transition temperature T i . Special attention is given to the case of the pseudo-acoustic phason. It is shown that its integrated intensity is proportional to (T i -T) near T i , and that its selection rules are similar to those obtained in Brillouin scattering. It is further shown that the latter are somewhat relaxed by the acoustic phonon-phason coupling. The method is finally extended to light scattering by hard phonons at q 0 and -q 0 .
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Poulet et al. (1981) studied this question.
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