Abstract
We provide a convincing numerical demonstration of the first-order nature of the transition in the three-state ferromagnetic Potts model in three dimensions by combining Monte Carlo simulations of the bulk free-energy barrier between the ordered and disordered states with finite-size scaling. From the histogram of internal energy and the number of clusters we extrapolate in q, the number of states, and find ${\mathit{q}}_{\mathit{c}}$=2.45\ifmmode\pm\else\textpm\fi{}0.1. We also find that the free-energy barrier \ensuremath{\Delta}F(q,L)\ensuremath{\sim}(q-${\mathit{q}}_{\mathit{c}}$${)}^{2}$${\mathit{L}}^{2.3}$ and conclude that there is no essential singularity in the correlation length or latent heat in contrast to two dimensions.
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