The conductance of a disordered system of finite volume Lᵈ (d spatial dimensions) is calculated by making use of a recently developed self-consistent theory. Scaling equations are derived for the dimensionless conductance g and the scaling function β(g(L))=dlng/dlnL is explicitly calculated for arbitrary dimension d. It is shown that the theory obeys scaling in the sense of Wegner, Thouless, and Abrahams et al.
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Vollhardt et al. (1982) studied this question.
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