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The Critical Spin Field of the Planar XY Model

OpenAI · October 5, 2026

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Abstract

Using the companion critical Bessel-height and pin-limit theorems, we prove that at the mass-defined critical inverse temperature of the nearest-neighbor XY model on the square lattice, the spin field on a square with boundary angles fixed to zero converges along the full sequence to the full-variance imaginary exponential of a zero-Dirichlet Gaussian free field with stiffness $2/\pi$. The normalization uses the exact center magnetization and the lattice Green-function factor. Convergence holds in law in $H^{-3}_{\mathrm{loc}}((-1,1)^2)$; all mixed moments and joint laws of fields smeared against smooth compactly supported test functions in $(-1,1)^2$ converge as well.

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Cite

@misc{OAI:The-Critical-Spin-Field-of-the-Planar-XY-Model-October-5-2026,
  author = {{OpenAI}},
  title = {{The Critical Spin Field of the Planar XY Model}},
  howpublished = {OpenAI Math Release preprint \href{https://github.com/openai/math/blob/main/preprints/The-Critical-Spin-Field-of-the-Planar-XY-Model-October-5-2026/paper.pdf}{OAI:The-Critical-Spin-Field-of-the-Planar-XY-Model-October-5-2026}},
  year = {2026}
}

Family 216: Critical and near-critical XY scaling and BKT universality

For the square-lattice nearest-neighbor cosine XY model, proves critical axis correlations $C_{\beta_c}(r)\sim Ar^{-1/4}(\log r)^{1/8}$ and the Berezinskii–Kosterlitz–Thouless essential singularity $\sqrt{\beta_c-\beta}\log\xi(\beta)\to B$, with $A,B\gt 0$ after the free-box thermodynamic limit. For finite square-symmetric interactions containing nearest neighbors, discrete Gaussian heights converge to Gaussian fields throughout the rough phase, including its threshold, along geometric torus sizes. Critical center-magnetization and spin-field conclusions retain their stated height, renormalization, and field-input assumptions.

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