Wave attenuation in glasses: Rayleigh and generalized-Rayleigh scattering scaling
arXiv:1905.03378 · doi:10.1063/1.5111192
Abstract
The attenuation of long-wavelength phonons (waves) by glassy disorder plays a central role in various glass anomalies, yet it is neither fully characterized, nor fully understood. Of particular importance is the scaling of the attenuation rate with small wavenumbers in the thermodynamic limit of macroscopic glasses. Here we use a combination of theory and extensive computer simulations to show that the macroscopic low-frequency behavior emerges at intermediate frequencies in finite-size glasses, above a recently identified crossover wavenumber , where phonons are no longer quantized into bands. For , finite-size effects dominate , which is quantitatively described by a theory of disordered phonon bands. For , we find that is affected by the number of quasilocalized nonphononic excitations, a generic signature of glasses that feature a universal density of states. In particular, we show that in a frequency range in which this number is small, follows a Rayleigh scattering scaling ( is the spatial dimension), and that in a frequency range in which this number is sufficiently large, the recently observed generalized-Rayleigh scaling of the form emerges ( is a characteristic wavenumber). Our results suggest that macroscopic glasses --- and, in particular, glasses generated by conventional laboratory quenches that are known to strongly suppress quasilocalized nonphononic excitations --- exhibit Rayleigh scaling at the lowest wavenumbers and a crossover to generalized-Rayleigh scaling at higher . Some supporting experimental evidence from recent literature is presented.
arXiv comment15 pages, 10 figures (including appendices). v2 includes a new appendix with 2 figures (Fig.7 & Fig.8)
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