The low-temperature drift mobility of the polaron is calculated in perturbation theory with the aid of the Kubo formula. The result is μ=μ₀(1-α6), where μ₀ is the weak coupling mobility μ₀=(e2αωm)exp(ωkT). A comparison is made with the perturbation expansion of various intermediate coupling mobility theories. The expansion of Osaka, μ=μ₀(1-0.173α+⋯), agrees most closely with the exact perturbation expansion. It is concluded that the Osaka formula is probably the best in the intermediate coupling range α<6. It is explicitly shown to lowest nontrivial order in α that various quasiparticle concepts are valid, viz., that μ=eτm*, and that the electron density is a momentum integral over f(E(p)).
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Langreth et al. (1964) studied this question.
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