The q-state, d-dimensional Potts models exhibit a variety of phase-transition behaviour in the limit d to 1 + , q to infinity , and l identical to (d-1) in q finite. The regions l<1, 1<l<2, and 2<l are distinguished, respectively, by no transition, second-order transitions (with a new changeover phenomenon at l=ln 4), and first-order transitions. The latter are due to the condensation of effective vacancies. Critical and tricritical exponent values are given.
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Berker et al. (1980) studied this question.
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