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Equations for the free energies of mono- and bi-layer superstructures of III-V ternary alloy systems were derived as functions of the order parameter ϕ (random atom arrangement when ϕ = 0 and a complete ordered arrangement when ϕ = 1). It was assumed in the analysis that mixing enthalpy was a strain energy caused by mixing. By minimizing the free energy, we obtained the value of ϕ at the equilibrium state. The values are larger than zero for monolayer superstructures on (100) and (110) surfaces below certain temperatures. For monolayer superstructures on a (111) surface, the stable states are at ϕ = 0, i.e., random arrangements at all temperatures. Bilayer superstructures are less stable than monolayer superstructures of the corresponding surface orientation.
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Ichimura et al. (1986) studied this question.
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