Abstract
Diffraction model calculations of electrical resistance for strong electron-phonon coupling in two- and three-dimensional alloys, incorporating Pippard-Ziman phonon ineffectiveness, are reported. It is shown that in an electron-phonon scattering based theory, although strong electron-phonon coupling is necessary, it is not a sufficient condition for the production of strong saturation in the normal-state resistivity. Thus, absence of saturation does not preclude strong electron-phonon coupling.
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