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The remarkable similarity between the observed SiC polytypes and the phases in the ANNNI model has suggested that the polytypes are equilibrium phases at high temperatures. Their origin lies in a competition between the nearest ( J 1 ) and next-nearest ( J 2 ) neighbour interactions between SiC double layers. We find, using norm-conserving pseudo-potentials, J 1 = +0.0050 eV and J 2 = -0.0034 eV per SiC pair. The sign of J 2 and the value of the ratio J 1 /| J 2 | are such as to lead to polytypes, thus broadly confirming the correctness of an ANNNI-like mechanism. The origins of J 1 and J 2 are discussed.
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Needs et al. (1987) studied this question.
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