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Tail states in disordered superconductors with magnetic impurities: the unitarity limit

F M Marchetti1,2 and B D Simons1

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When subject to a weak magnetic impurity distribution, the order parameter and quasi-particle energy gap of a weakly disordered bulk s-wave superconductor are suppressed. In the Born scattering limit, recent investigations have shown that 'optimal fluctuations' of the random impurity potential can lead to the nucleation of 'domains' of localized states within the gap region predicted by the conventional Abrikosov–Gor'kov mean-field theory, rendering the superconducting system gapless at any finite impurity concentration. By implementing a field theoretic scheme tailored to the weakly disordered system, the aim of the present paper is to extend this analysis to the consideration of magnetic impurities in the unitarity scattering limit. This investigation reveals that the qualitative behaviour is maintained while the density of states exhibits a rich structure.


PACS

75.30.Hx Magnetic impurity interactions

74.40.+k Fluctuations (noise, chaos, nonequilibrium superconductivity, localization, etc.)

74.20.Rp Pairing symmetries (other than s-wave)

73.63.-b Electronic transport in nanoscale materials and structures

MSC

82D40 Magnetic materials

82D55 Superconductors

Subjects

Superconductivity

Condensed matter: electrical, magnetic and optical

Nanoscale science and low-D systems

Dates

Issue 19 (17 May 2002)

Received 12 November 2001, in final form 21 March 2002

Published 3 May 2002



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