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Magnetoresistance through an interplay between the Kondo effect and the Anderson localization is investigated in the weakly localized regime. The anomalous resistivity in the order of J 3 , which is in proportion to T d /2-2 in the absence of magnetic fields, is seen to be suppressed, once the Zeeman energy exceeds the thermal energy; J , T and d are an exchange interaction constant, temperature and dimensionality, respectively.
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Ohkawa et al. (1984) studied this question.
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