paper

Marginal dimensions of the Potts model with invisible states

arXiv:1512.03635 · doi:10.1088/1751-8113/49/25/255001

Abstract

We reconsider the mean-field Potts model with interacting and non-interacting (invisible) states. The model was recently introduced to explain discrepancies between theoretical predictions and experimental observations of phase transitions in some systems where the -symmetry is spontaneously broken. We analyse the marginal dimensions of the model, i.e., the value of at which the order of the phase transition changes. In the case, we determine that value to be ; there is a second-order phase transition there when and a first-order one at . We also analyse the region and show that the change from second to first order there is manifest through a new mechanism involving {\emph{two}} marginal values of . The limit gives bond percolation and some intermediary values also have known physical realisations. Above the lower value , the order parameters exhibit discontinuities at temperature below a critical value . But, provided is small enough, this discontinuity does not appear at the phase transition, which is continuous and takes place at . The larger value marks the point at which the phase transition at changes from second to first order. Thus, for , the transition at remains second order while the order parameter has a discontinuity at . As increases further, increases, bringing the discontinuity closer to . Finally, when exceeds coincides with and the phase transition becomes first order. This new mechanism indicates how the discontinuity characteristic of first order phase transitions emerges.

15 pages, 7 figures, 2 tables

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