Abstract

The influence of magnetic impurities on the transition temperature of superconducting alloys is investigated by means of the higher order parquet theory, which is essentially a self-consistent renormalization of the s-d interaction vertex and the quasi-fermion self-energy. The effective electron-electron interaction is evaluated beyond the logarithmic approximation, in terms of the renormalized spin-flip amplitude, which is responsible for the pair-breaking effect of the magnetic impurities. An expression for the maximal pair breaking, which is dependent on the spin and the superconducting coupling constant, is derived.

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