The calculated structure factor of a disordered fee crystal formed by
a disparate-mass mixture shows at low wave vectors (k) a broad high-fr
equency band in addition to hydrodynamic phonons. The former shows a p
ronounced k dependence. The average phase velocity of such excitations
is lower than that of the longitudinal sound in a crystal of light pa
rticles. At larger k, the hydrodynamic frequencies decrease with incre
asing k, well below the linear dispersion regime, and finally disappea
r. The findings are rationalized on the basis of a ''two-solid model.'
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