The dynamic structure factor S(Q,omega), of vitreous silica, has been measured by inelastic x-ray scattering in the exchanged wave-vector (Q) region Q=4-16.5 nm(-1) and up to energies (h) over bar omega=115 meV in the Stokes side. The unprecedented statistical accuracy in such an extended energy range allows us to accurately determine the longitudinal current spectra and the energies of the vibrational excitations. The simultaneous observation of two excitations in the acoustic region and the persistence of propagating sound waves up to Q values comparable with the (pseudo-)Brillouin-zone edge allow us to observe a positive dispersion in the generalized sound velocity that, around Qapproximate to5 nm(-1), varies from approximate to6500 to approximate to9000 m/s; this phenomenon was never experimentally observed in a glass.
Evidence of anomalous dispersion of the generalized sound velocity in glasses
Ruzicka B;Scopigno T;Caponi S;
2004
Abstract
The dynamic structure factor S(Q,omega), of vitreous silica, has been measured by inelastic x-ray scattering in the exchanged wave-vector (Q) region Q=4-16.5 nm(-1) and up to energies (h) over bar omega=115 meV in the Stokes side. The unprecedented statistical accuracy in such an extended energy range allows us to accurately determine the longitudinal current spectra and the energies of the vibrational excitations. The simultaneous observation of two excitations in the acoustic region and the persistence of propagating sound waves up to Q values comparable with the (pseudo-)Brillouin-zone edge allow us to observe a positive dispersion in the generalized sound velocity that, around Qapproximate to5 nm(-1), varies from approximate to6500 to approximate to9000 m/s; this phenomenon was never experimentally observed in a glass.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
