Abstract
The steady magnetic susceptibility of dilute substitutional alloys, in the absence of spin-orbit coupling is discussed. Band characteristics of the host are retained. A general expression for the Fourier transformed susceptibility tensor is given which may in principle be expanded in powers of the impurity potential. The zero-order term gives the perfect crystal susceptibility previously derived by Hebborn and Sondheimer. The first-order term is very complicated by a 'rigid band' model allows the impurity shift to be expressed in terms of the known pure crystal result.

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