Abstract
A relation between the ultrasonic attenuation coefficient and the Eliashburg function α2F is derived, which holds up to leading order in the impurity density. This shows that all electron-phonon interaction models which yield Pippard’s result for the sound attenuation are equivalent with respect to calculation of electronic properties as well. The low-frequency behavior of α2F(ω) is calculated for a jellium model, and several mutually contradicting results in the literature are discussed.

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