1994
DOI: 10.1088/0953-8984/6/24/016
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On the multichannel Kondo model

Abstract: A detailed and comprehensive study of the one-impurity multichannel Kondo model is presented. In the limit of a large number of conduction electron channels k ≫ 1, the low energy fixed point is accessible to a renormalization group improved perturbative expansion in 1/k. This straightforward approach enables us to examine the scaling, thermodynamics and dynamical response functions in great detail and make clear the following features: i) the criticality of the fixed point; ii) the universal non-integer degene… Show more

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Cited by 37 publications
(55 citation statements)
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“…The first non-zero contribution to S z 1 is second order in t/J. Since 8) we find that only the second term in Eq. (7.6) will contribute and we get…”
Section: B Wave-functionmentioning
confidence: 66%
See 1 more Smart Citation
“…The first non-zero contribution to S z 1 is second order in t/J. Since 8) we find that only the second term in Eq. (7.6) will contribute and we get…”
Section: B Wave-functionmentioning
confidence: 66%
“…We have adopted the notation of Ref. ( 8). Note that the sum of these correlation functions is independent of τ since the total spin is conserved, so that the τ -integral simply gives a factor of β.…”
Section: Renormalization Group Argumentsmentioning
confidence: 99%
“…For the three different susceptibilities: γ tt = 0, γ ti = γ imp , and γ ii = 2γ imp . The low-order perturbative results for β(λ) [14] and γ imp (λ) [7] are:…”
mentioning
confidence: 99%
“…The ground state of the Kondo system is a non-magnetic Fermi-liquid type. As we have shown, the screening of the local spin can be eliminated by the polarization of the local spin, which is important to understanding the microscopic origin of non-Fermi liquid behavior of the oxide compounds, especially the high T c cuprates [8].…”
Section: Summary and Discussionmentioning
confidence: 94%