2022
DOI: 10.2140/pmp.2022.3.707
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The genus-zero five-vertex model

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Cited by 4 publications
(6 citation statements)
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“…In fact, we observe that the surface tension σ has the same structure as the general large r five-vertex model (see theorem 3.2 b of [14]): the boundary values of √ det H σ are equal to π in the corners (0, 0) and (−1, 0) and 4π in the corner (−1/2, 1/2), and the extension inside is dictated by the harmonicity of κ 1/2 (z). The behaviors at these two types of corners are referred to as ferroelectric and anti-ferroelectric phases in [6].…”
Section: Four-vertex Model Versus Lozenge Tilingsmentioning
confidence: 59%
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“…In fact, we observe that the surface tension σ has the same structure as the general large r five-vertex model (see theorem 3.2 b of [14]): the boundary values of √ det H σ are equal to π in the corners (0, 0) and (−1, 0) and 4π in the corner (−1/2, 1/2), and the extension inside is dictated by the harmonicity of κ 1/2 (z). The behaviors at these two types of corners are referred to as ferroelectric and anti-ferroelectric phases in [6].…”
Section: Four-vertex Model Versus Lozenge Tilingsmentioning
confidence: 59%
“…parameterizes the tangent lines to the arctic curve as u runs over R, see [14]. The roots of s u therefore correspond to the horizontal sides of R, the roots of t u correspond to the vertical lines of R, and the roots of c u are the tangent lines through the origin.…”
Section: Domino Limit Shapesmentioning
confidence: 99%
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“…For recent progresses in relation to nonperiodic graphs, see [20], and reference therein. Concerning models that cannot be expressed in terms of free fermions, the variational principle has been solved only for the five-vertex model [21][22][23], and for some particular cases of the stochastic six-vertex model [24,25].…”
Section: Introductionmentioning
confidence: 99%