In metals and alloys containing localized magnetic moments, an important contribution to the electrical resistivity can be associated with disorder of the atomic spin system. This contribution is ascribed to a scalar interaction between the spins of the conduction electrons and the atomic spins. Assuming a simple form for this interaction, the experimental and theoretical situation concerning the spin-disorder resistivity is reviewed for pure metals, dilute alloys, and concentrated binary alloys.
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Arnold J. den Dekker (1965) studied this question.
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