Abstract

We study here the role randomly-placed non-magnetic scatterers play on the Kondo effect. We show that spin relaxation effects (with time Ο„so\tau_s^o)in the vertex corrections to the Kondo self-energy lead to an exact cancellation of the singular temperature dependence arising from the diffusion poles. For a thin film of thickness LL and a mean-free path β„“\ell, disorder provides a correction to the Kondo resistivity of the form Ο„so/(kFLβ„“2)ln⁑T\tau_s^o/(k_FL\ell^2)\ln T that explains both the disorder and sample-size depression of the Kondo effect observed by Blachly and Giordano (PRB {\bf 51}, 12537 (1995)).Comment: 11 pages, LaTeX, 2 Postscript figure

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