Bosonization in the two-channel Kondo model
arXiv:cond-mat/9606063 · doi:10.1103/PhysRevB.55.5627
Abstract
The bosonization of the anisotropic two-channel Kondo model is shown to yield two equivalent representations of the original problem. In a straight forward extension of the Emery-Kivelson approach, the interacting resonant level model previously derived by the Anderson-Yuval technique is obtained. In addition, however, a ``(,)'' description is also found. The strong coupling fixed point of the (,) model was originally postulated to be related to the intermediate coupling fixed point of the two-channel Kondo model. The equivalence of the , model to the two-channel Kondo model is formally established. A summary of what one may learn from a simple study of these different representations is also given.
5 pages, latex (uses revtex and epsf macros) with 1 postscript figure
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