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Massive Scaling Limit of the Ising Model: Subcritical Analysis and Isomonodromy

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arxiv 1811.06636 v2 pith:HXYVSHRU submitted 2018-11-16 math.PR math-phmath.MP

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We study the spin n-point functions of the planar Ising model on a simply connected domain \Omega discretised by the square lattice \delta\mathbb{Z}^{2} under near-critical scaling limit. While the scaling limit on the full-plane \mathbb{C} has been analysed in terms of a fermionic field theory, the limit in general \Omega has not been studied. We will show that, in a massive scaling limit wherein the inverse temperature is scaled \beta\sim\beta_{c}-m_{0}\delta for a constant m_{0}<0, the renormalised spin correlations converge to a continuous quantity determined by a boundary value problem set in \Omega. In the case of \Omega=\mathbb{C} and n=2, this result reproduces the celebrated formula of [WMTB76] involving the Painlev\'e III transcendent. To this end, we generalise the comprehensive discrete complex analytic framework used in the critical setting to the massive setting, which results in a perturbation of the usual notions of analyticity and harmonicity.

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Cited by 3 Pith papers

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  1. The near critical random bond ising model via embedding deformation

    math.PR 2025-09 conditional novelty 8.0 of 10

    A new embedding-deformation method proves conformal invariance of the near-critical random bond Ising model for coupling fluctuations up to n^-1/3, far beyond the deterministic n^-1 window.

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    Fractional vertex-operator correlations of the massless sine-Gordon model at β = 4π are shown to equal Palmer's tau functions of massive twisted Dirac operators, giving a proof of the Lukyanov-Zamolodchikov one-point formula.

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    Centered random bond disorder preserves criticality in planar FK-percolation over windows much larger than the deterministic critical window, with the strongest case being Bernoulli percolation where disorder is asymp...

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