On the transition between the disordered and antiferroelectric phases of the 6-vertex model
arXiv:1909.03436 · doi:10.1214/23-EJP980
Abstract
The symmetric six-vertex model with parameters is expected to exhibit different behavior in the regimes (antiferroelectric), (disordered) and (ferroelectric). In this work, we study the way in which the transition between the regimes and manifests. When , we show that the associated height function is localized and its extremal periodic Gibbs states can be parametrized by the integers in such a way that, in the -th state, the heights and percolate while the connected components of their complement have diameters with exponentially decaying tails. When , the height function is delocalized. The proofs rely on the Baxter-Kelland-Wu coupling between the six-vertex and the random-cluster models and on recent results for the latter. An interpolation between free and wired boundary conditions is introduced by modifying cluster weights. Using triangular lattice contours (-circuits), we describe another coupling for height functions that in particular leads to a novel proof of the delocalization at . Finally, we highlight a spin representation of the six-vertex model and obtain a coupling of it to the Ashkin-Teller model on at its self-dual line . When , we show that each of the two Ising configurations exhibits exponential decay of correlations while their product is ferromagnetically ordered.
v2: Improvements to the exposition, minor enhancements to the main results. Added a short proof for the delocalization of the height function of square-ice via triangular circuits. v3: Minor edits, published version
References in corpus (3)
Cited by in corpus (13)
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- On the duality between height functions and continuous spin models