First principles calculation of the phonons modes in the hexagonal $\rm YMnO_3$ ferroelectric and paraelectric phases
Texte intégral
Documents relatifs
Fig, 2: Raman scattering from Fig. 3: The Eg Raman spectrum of V3Si at acoustic phonons in TaC0.99. 6) Lines repre- For each symmetry one and two phonon sent fits to a
The self-consistent phonon approximation (SPA) which leads to exact results in the very displacive limit predicts y=2, too13.The dimensionality crossover re- gime, appearing at
Calculation of the cross section.- The computed cross section for a coated surface is found to be the square modulus of the sum of four contributions(*), due to: a) scat tering
L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des
It should also be pointed out that F~ cannot be considered as a full order parameter, with its own temperature dependence, because the dielectnc susceptibihty remains
The transverse acoustic branch Ty[100] thus observed, exhibits no softening over the frequency range 10 GHz v 200 GHz, while a critical increase of the quasi-elastic
Abstract. 2014 We have made the first measurements of the polar modes in the cubic phase of the ferroelectric perov- skite KNbO3 by infrared reflectivity
Nous avons donne la premii.re observation d'un mode amorti de symetrie B2 dans le spectre Raman pour (NH4)H2P04.. La variation du temps de relaxation de Debye en fonction de