2021
DOI: 10.1016/j.nuclphysb.2021.115365
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Identifying the Huse-Fisher universality class of the three-state chiral Potts model

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Cited by 11 publications
(4 citation statements)
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“…The only difference it that the chiral transition of our model is more extended below the lobe than for the blockade model. Note that, more generally, our results agree with those obtained on classical 2D and quantum 1D versions of the period-3 case 9,14,23,29-36 , for which the existence of a transition line in the chiral universality class is supported both by experiments 6,7 and by recent numerical work 25,27,28,37,38 .…”
supporting
confidence: 90%
See 1 more Smart Citation
“…The only difference it that the chiral transition of our model is more extended below the lobe than for the blockade model. Note that, more generally, our results agree with those obtained on classical 2D and quantum 1D versions of the period-3 case 9,14,23,29-36 , for which the existence of a transition line in the chiral universality class is supported both by experiments 6,7 and by recent numerical work 25,27,28,37,38 .…”
supporting
confidence: 90%
“…It is fixed to z = 1 at the conformal points P and AT, but an accurate estimate of its value away from this point is still beyond state-of-the-art simulations. What one can get quite accurately however is the exponent ν, and the fact that its value is consistent with that of β along the chiral transition is an indication that cross-over effects are negligible for the model of Rydberg chains, contrary to the classical 2D chiral Potts model, where crossover effects lead to an overestimate of ν and a violation of the ν = β criterion close to the Potts point 38 .…”
mentioning
confidence: 93%
“…It is worth noting that the precise Potts point can be located numerically with high precision by following the commensurate line q = 2π/3 in the disordered phase until the period-3 ordered phase is reached. More details can be found in references [42][43][44][45] for more details. Furthermore, we also examined the effect of the interaction cutoff adopted in our simulation on this R b = 2.3 case.…”
Section: Non-conformal Critical Point: Chiral Universility Classmentioning
confidence: 99%
“…, sparking interest in the C-IC transition first proposed in the context of adsorbed monolayers in 1980s and 1990s [38][39][40][41]. The C-IC transition with p ≥ 5 emerges through an intermediate gapless floating phase (Luttinger liquid) with a central charge c = 1, characterized by incommensurate correlations and wave vector q [42][43][44][45][46]. On the one hand, disorderto-floating transitions belong to the Kosterlitz-Thouless (KT) universality class with exponentially diverged correlation lengths.…”
Section: Introductionmentioning
confidence: 99%