The pair-breaking effect of inelastic scattering of electrons off boson fluctuations is examined for anisotropic and isotropic superconductors. We show that the ratio g of the couplings of the boson fluctuations to the pairing and normal electron self-energies is an important parameter. Phonon-mediated s-wave superconductivity corresponds to a value of g=1, and spin-fluctuation-mediated d-wave superconductivity to g<1. For g<1, there is a critical frequency ωc{~}Tc{e}1/gin the boson spectrum: bosons at ω{{ω}}c$ are pair breaking. We give an approximate expression for the pair-breaking effect of low-lying bosons. We also study the dependence of ${T}c$ upon g in an Einstein model in which the boson spectral weight is concentrated at a frequency ${{ω}}E$. We show that for fixed electron-boson coupling, ${T}c$/${{ω}}Edecreases rapidly as g decreases from 1, and for g≠1{T}c$/${{ω}}E$ saturates at a low value as the coupling tends to infinity. Applications to heavy-fermion superconductors and to the new high-${T}c$ materials are discussed.
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Millis et al. (1988) studied this question.
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