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Lattice energy calculations based on the Born model are used to examine the possible structures of defect clusters in non-stoichiometric FeO. The basic cluster is identified as a complex of four cation vacancies and one tetrahedral Fe 3+ ion (or 4:1 cluster) which is formed as a result of a large Coulomb term favouring the occupation of the tetrahedral site when all nearest-neighbour cations are vacant. The aggregation of these 4:1 clusters occurs by vacancy-sharing, and the calculations suggest that the most stable small aggregates are formed by edge- rather than corner-sharing (6:2 or 8:3 clusters). If more extended clusters are formed they are likely to involve corner-sharing, but the binding energy for a cluster closely related to the Fe 3 O 4 structure is larger than that calculated for the Koch-Cohen cluster.
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Catlow et al. (1975) studied this question.
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