The formalism of the previous paper is applied to calculate surface states on two very simple models of a solid, in order to show the type of Green functions needed in practical applications of the theory. The first model is that of Shockley states in the gap of a nearly-free-electron band structure in one dimension. In the second model a band of surface states is split off from a single band in three dimensions.
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Garcı́a-Moliner et al. (1969) studied this question.
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