1984
DOI: 10.1088/0022-3719/17/14/013
|View full text |Cite
|
Sign up to set email alerts
|

Bethe ansatz and 1/N expansion results for N-fold degenerate magnetic impurity models

Abstract: The authors calculate the ground state susceptibility chi 0, to leading and next-leading order in a 1/n expansion, for the N-fold degenerate Anderson model in the integral valent limit. From this and perturbational results they are able to calculate the Wilson numbers W(N), which relate to chi 0 and TK, to first order in 1/N.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
13
0

Year Published

1985
1985
2010
2010

Publication Types

Select...
3
3
2

Relationship

0
8

Authors

Journals

citations
Cited by 56 publications
(13 citation statements)
references
References 28 publications
0
13
0
Order By: Relevance
“…We can then infer a value of T K by using T K ϭ (RlnN)/␥ (22) or by using T K ϭ (N Ϫ 1) 2 Rw N /3N␥ (where w N is a multiplicative factor that is a function of N as discussed in ref. 21). These expressions produce T K values that are within 5% of each other for 2 Յ N Յ 8.…”
Section: Discussionmentioning
confidence: 99%
“…We can then infer a value of T K by using T K ϭ (RlnN)/␥ (22) or by using T K ϭ (N Ϫ 1) 2 Rw N /3N␥ (where w N is a multiplicative factor that is a function of N as discussed in ref. 21). These expressions produce T K values that are within 5% of each other for 2 Յ N Յ 8.…”
Section: Discussionmentioning
confidence: 99%
“…The low temperature part of the specific heat data can be well fit by assuming that a quadruplet is Kondo screened and that there is a doublet CEF As the degeneracies of the Yb ions were inferred, by the analysis above, when they enter the Kondo screening states (see Table 9.1), the values of their T K can be then inferred by using T K = (R ln N )/γ, a rough estimation from magnetic entropy [Fisk et al, 1988], or by using T K = (N − 1)π 2 Rω N /3Nγ, the Bethe ansatz results of N-fold CoqblinSchrieffer model [Hewson, 1993] where ω N is the so called Wilson number and that is a function of N as discussed in ref. [Rasul and Hewson, 1984]. These expressions produce T K values that are within 5% of each other for 2 ≤ N ≤ 8.…”
Section: Discussionmentioning
confidence: 75%
“…where ω N is Wilson number [Rasul and Hewson, 1984]. The broad peak appearing in the temperature dependent susceptibility [2.11 (a)] is usually called as 'Kondo peak' and observed in many heavy Fermion systems.…”
Section: Kadowaki-woods Ratiomentioning
confidence: 99%
“…where w N is the generalization of the Wilson number, given by w N = e 1+C−3/2N /2πΓ N (1 + 1/N ) [Rasul, 1984]. The electronic specific heat coefficient, γ, deduced from the thermodynamic equations in the Coqblin-Schrieffer limit [Coqblin, 1969] is given by…”
Section: Wilson Ratio -mentioning
confidence: 99%
“…where γ is expressed using high temperature limit of T K , as defined by Wilson [Rasul, 1984], and this equation is equivalent to Eq. 3.14.…”
Section: Wilson Ratio -mentioning
confidence: 99%