We present a band theory for the internal energy of binary alloys which undergo order-disorder transformations. The general method involves the self-consistent solution of a tight-binding Hartree Hamiltonian in the presence of both long- and short-range-order correlations through the use of an extended cluster-Bethe-lattice method. A complete scheme for the derivation of the alloy thermodynamics is obtained by coupling the electronic theory to the cluster-variation combinatorial theory for the alloy configurational entropy. The theory is applied to the study of the CuAu order-disorder transition and comparisons are made to existing data and Ising models.
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Kittler et al. (1978) studied this question.
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