Abstract
The Wolff-Moriya model for the localized magnetic moments in metals is treated self-consistently by using the decoupling method of the double-time Green functions. The resulting scattering matrix is solved exactly in the strongly correlated limit and is compared with solutions for the s-d exchange model and for the Anderson model. The expression for the resistivity differs qualitatively from those for the s-d exchange and Anderson models and can be associated with the anomaly observed in Rh-Fe alloy.
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