Abstract
We reinvestigate the large degeneracy solution of the multichannel Kondo problem, and show how in the universal regime the complicated integral equations simplifying the problem can be mapped onto a first-order differential equation. This leads to an explicit expression for the full zero-temperature scaling functions at—and away from—the intermediate non-Fermi-liquid fixed point, providing complete analytic information on the universal low—and intermediate—energy properties of the model. These results also apply to the widely used noncrossing approximation of the Anderson model, taken in the Kondo regime. An extension of this formalism for studying finite-temperature effects is also proposed and offers a simple approach to solve models of strongly correlated electrons with relevance to the physics of heavy fermion compounds.
- Received 13 October 2003
DOI:https://doi.org/10.1103/PhysRevB.69.113103
©2004 American Physical Society