Numéro |
J. Phys. Colloques
Volume 33, Numéro C2, Avril 1972
2e CONGRÈS EUROPÉEN DE FERROÉLECTRICITÉ
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Page(s) | C2-54 - C2-54 | |
DOI | https://doi.org/10.1051/jphyscol:1972213 |
J. Phys. Colloques 33 (1972) C2-54-C2-54
DOI: 10.1051/jphyscol:1972213
STRUCTURE DISORDER AND RAMAN SCATTERING IN BaTiO3 AND KNbO3
M. P. FONTANA, M. LAMBERT and A. M. QUITTETLaboratoire de Physique des Solides , Faculté des Sciences, 91, Orsay, France
Abstract
We have shown [1] that the Raman scattering spectra observed in the cubic paraelectric phase of BaTiO3 by different investigators [2], [3] cannot be due to either impurity related effects or to ordinary second order process even if one of the two phonons participating in such a process were soft. The KNbO3 spectra are very similar. In particular, they also show prominent broad peaks at 260 and 560 cm-1 analogous to those found at about 270 and 530 cm-1 in BaTiO3. In both cases the spectrum does not disappear at the ferroelectric phase transition and its intensity begins only to decrease at quite higher temperatures (200 °C for BaTiO3 and 600 °C for KNbO3). Such an effect can be related to the structure disorder which has been proposed on the basis of X Ray diffuse scattering experiments [4]. This disorder can be described in terms of off-center atomic displacements : the structure has no local inversion symmetry center and thus Raman scattering can be observed even in the cubic phase. The Raman scattering can be interpreted as a second order process involving a phonon and a pseudo-spin excitation. The decrease with temperature of the Raman cross section must be correlated with the evolution of the disordered structure.