2004/09/13 by S. Kettemann, Kettemann, S.
Physics and Astronomy · #FOS: Physical sciences #Mesoscale and Nanoscale Physics (cond-mat.mes-hall) #Strongly Correlated Electrons (cond-mat.str-el) #cond-mat.mes-hall #cond-mat.str-el
paper · pdf · doi:10.48550/arxiv.cond-mat/0409317
4 pages, Proceedings of the V. Rencontre de Moriond in Mesoscopic Physics January 2004
arxiv created 2004/09/13 · arxiv updated 2009/12/01
The Kondo temperature of a magnetic impurity in a weakly disordered metal is distributed due to the randomness in the local exchange coupling, and the local electronic density of states (LDOS). We show that in a closed, phase coherent metal particle the resulting distribution of TK is strongly asymmetric and scales with the mean level spacing Δ. Its width is 2 √(Δ/βTK), where Δ is the mean level spacing, and β=1,2, with, without time reversal symmetry, respectively. Increasing the density of magnetic impurities, the distribution of Kondo temperatures (DKT) is found to become more narrow. Corrections to these results due to Anderson localisation are discussed.