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Three values of the electron-phonon mass enhancement λ for zinc and cadmium are compared: one obtained from the ratio of the electronic-specific-heat density of states and the band-structure value calculated from a pseudopotential approach, one calculated directly by means of the same pseudopotential, and one extracted by other authors from values of the superconducting transition temperature Tc and the Debye temperature {}. For both metals the agreement between all three λ values is very good, indicating the correctness and uniqueness of the pseudopotential. Calculations performed with other proposed pseudopotentials give very different values of λ.
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Allen et al. (1968) studied this question.
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