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From a large number of T-T-oxide---Ag tunneling junctions, with T=TaandNb, an empirical correlation was observed between the slope S of the normal conductance-versus-voltage characteristics and the strength of the phonon-induced features of the superconductor density of states. This correlation allows for a tentative extrapolation to the bulk tantalum density of states which, when inverted according to the Rowell-McMillan scheme, leads to parameters (λ=0.80, μ*=0.15) which deviate markedly from values accepted hitherto and stronger high-energy (longitudinal phonon) contributions to α²F(ω). For niobium, high-energy contributions to α²F(ω) stronger than recently assumed are highly probable. The slope S is governed by a zero-bias conductance dip. This anomaly as well as the nonideal features of the tunneling density of states in the superconducting state are attributed to a metal-semiconductor transition layer between the superconductor and its oxide with spatial extent of 3-10 {}, and at least 10 {} in the tantalum and niobium cases, respectively.
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Hahn et al. (1982) studied this question.
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