Abstract
We analyze the properties of theq-state ferromagnetic Potts model for realq. The nature of the phase transition at the critical point is first-order forq≠2, and second-order forq=2. The random-bond percolation limitq→1, and its second-order-like transition, are not related to the previous behaviour since they arise from non-stable phases of the system. It is suggested that this property characterizes the model on high-dimensional lattices, too.
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di Liberto, F., Monroy, G. & Peruggi, F. The potts model on bethe lattices. Z. Physik B - Condensed Matter 66, 379–385 (1987). https://doi.org/10.1007/BF01305430
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DOI: https://doi.org/10.1007/BF01305430