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The resistivity of a dilute alloy due to localized spin fluctuations (LSF) occurring on the impurity orbitals is given by a universal function of the temperature. The resistivity is finite at T=0, then decreases with temperature as T 2 , T, lnT and T -1 successively. The T 2 and T behaviour are in good agreement with the experimental data on AIMn. The T 2 and lnT laws are expected by comparison between LSF and the Kondo effect.
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Rivier et al. (1972) studied this question.
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