Emery's analysis of n-component "spin" systems is extended and simplified for the limits n=0,-2,-4,. Restrictions on the spin-weighting function implied by an interpretation of the n→0 limit as a random system are pointed out. Fully explicit relations are also derived for the interpretation of the n→0 correlation function in terms of self-avoiding and, more generally, weighted self-interacting lattice walks.
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Jasnow et al. (1976) studied this question.
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