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The simultaneous occuring of atomic ordering and ferromagnetic ordering is described in a mean field approximation for an alloy where magnetic properties are due to the itinerant character of electrons: thus a generalization of the Stoner‐Wohlfarth model is proposed for the case of nondisordered ferromagnetic alloys. Treating first the non‐magnetic case, when the intra‐atomic correlation parameter U is not too high, a higher ordering temperature is obtained than in the Bragg‐Williams case; considering then the (weak) ferromagnetic case, also an increase of the Curie temperature is found. However, different situations can occur, according to the choice of the model density of states.
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Billard et al. (1977) studied this question.
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