Abstract

The order-disorder phase transition at the surface at ${A}_{3}B$-type alloys has been studied using the Bragg-Williams theory. A simple electronic theory for the order-disorder transition at the surface is also presented. In agreement with experiments for ${\mathrm{Cu}}_{3}$Au one finds that the order parameter and in particular the discontinuity in the order parameter at the transition temperature ${T}_{c}$ is strongly reduced for the first three atomic surface layers. We study also the effect of surface segregation on the order-disorder transition at the surface. One finds that due to segregation the order parameter can disappear at the surface at temperatures below ${T}_{c}$. Also, atomic ordering may suppress segregation.

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