A single-band model is used to study the electronic structure of disordered binary alloys. Functional-derivative techniques are used to generate an expansion for the electron self-energy that is free of all "multiple-occupancy" corrections. This analysis reveals that the relevant small parameter for the coherent-potential approximation (CPA) is Z^-1, where Z is the number of nearest neighbors. In addition to being exact to first order in the concentration x and third order in the impurity potential δ, the CPA retains just those contributions of higher order in x and δ that are independent of Z^-1. Various methods have been suggested to calculate corrections to the CPA due to two-atom clusters. While all of these are exact to order x² and δ⁵, we argue that a proper generalization of the CPA must also be correct to higher orders in Z^-1. The appropriate equations are derived and shown to imply the existence of satellite levels on either side of the impurity subband. A formalism is developed to examine the departure from the usual assumption of complete compositional disorder. To order x², the single-band Hamiltonian is found to imply the existence of short-range order in the alloy. The influence of this short-range order on the density of states is discussed and is shown to modify the clustering effects previously evaluated.
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Schwartz et al. (1972) studied this question.
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