\pdfoutput=1 \documentclass[11pt]{article} \usepackage[margin=1in]{geometry} \usepackage[T1]{fontenc} \usepackage{lmodern,microtype} \usepackage{amsmath,amssymb,amsthm} \usepackage{xcolor} \usepackage{xurl} \usepackage[colorlinks=true,linkcolor=blue!50!black,citecolor=blue!50!black,urlcolor=blue!50!black,bookmarksnumbered=true]{hyperref} \usepackage{bookmark} \usepackage{tikz} \usetikzlibrary{arrows.meta,calc} \hypersetup{pdftitle={Closing the identification step in the GFF limit: Uniqueness of the zero-slope six-vertex phase for -1 <= Delta < 1/2},pdfauthor={Yan Ru Pei},pdfkeywords={six-vertex model, height function, gradient Gibbs measures, uniqueness, cluster swapping, Gaussian free field}} \newtheorem{theorem}{Theorem}[section] \newtheorem{proposition}[theorem]{Proposition} \newtheorem{lemma}[theorem]{Lemma} \newtheorem{corollary}[theorem]{Corollary} \theoremstyle{definition} \newtheorem{definition}[theorem]{Definition} \theoremstyle{remark} \newtheorem{remark}[theorem]{Remark} \numberwithin{equation}{section} \newcommand{\Z}{\mathbb Z} \newcommand{\R}{\mathbb R} \newcommand{\E}{\mathbb E} \newcommand{\Pp}{\mathbb P} \newcommand{\MM}{\mathbb M} \newcommand{\Diag}{\mathfrak D} \newcommand{\ind}[1]{\mathbf 1\{#1\}} \newcommand{\SFE}{\operatorname{SFE}} \newcommand{\ICI}{I_{\mathrm{CI}}} \newcommand{\dd}{\mathrm d} \newcommand{\om}{\bar\omega} \newcommand{\Om}{\bar\Omega} \newcommand{\gb}{\bar\gamma} \newcommand{\mub}{\bar\mu} \newcommand{\rhob}{\bar\rho} \newcommand{\Psh}{\Pp^{\sharp}} \newcommand{\Lr}{\Lambda} \newcommand{\dist}{\operatorname{dist}} \newcommand{\Ebar}{\mathcal E} \newcommand{\ID}{\textup{(ID)}} \makeatletter \def\Xint#1{\mathchoice {\XXint\displaystyle\textstyle{#1}}% {\XXint\textstyle\scriptstyle{#1}}% {\XXint\scriptstyle\scriptscriptstyle{#1}}% {\XXint\scriptscriptstyle\scriptscriptstyle{#1}}% \!\int} \def\XXint#1#2#3{{\setbox0=\hbox{$#1{#2#3}{\int}$}% \vcenter{\hbox{$#2#3$}}\kern-.5\wd0}} \makeatother \newcommand{\avint}{\Xint-} \title{Closing the identification step in the GFF limit:\\ Uniqueness of the zero-slope six-vertex phase for $-1\le\Delta<\frac12$} \author{Yan Ru Pei\\[0.3em]\small\href{mailto:yanrpei@gmail.com}{\texttt{yanrpei@gmail.com}}} \date{November 2026\\[0.3em]\small\href{https://doi.org/10.5281/zenodo.24117031}{doi:10.5281/zenodo.24117031}} \begin{document} \maketitle \begin{abstract} For the six-vertex model with $a=b=1$ and $c\in(1,2]$, that is $-1\le\Delta<\frac12$, we prove that the plane measure, the limit of balanced torus measures, is the only translation-ergodic gradient Gibbs measure of slope zero, and hence the unique translation-invariant minimiser of the specific free energy. Both statements had been asserted by reference to Sheffield's uniqueness theory, which is proved for nearest-neighbour potentials; we show that for $c\ne1$ the six-vertex weights, which couple faces across the diagonals of each vertex, are not a nearest-neighbour potential in height coordinates. The proof extends Sheffield's cluster swapping to these diagonal interactions by means of residual energies on the diagonals, shows with the Lanford--Ruelle theorem for subshifts of finite type and a Burton--Keane argument that two distinct ergodic zero-slope phases are gradients of Gibbs measures on heights, and shows from the spin representation in the form given by Duminil-Copin, Kozlowski, Lammers and Manolescu that the plane measure is not. This supplies a step that we found missing in the chain of recent results on the Gaussian free field limit of the six-vertex height function. An unrefereed manuscript of OpenAI states the full-plane limit for every $c\in(0,2]$; for $\sqrt2\le c<2$ it identifies a state built from nearly balanced sectors with the plane measure through the characterisation above. Our result gives that identification, given two properties of the state stated in the manuscript. We also check that the manuscript and the work of Averous, Duminil-Copin, He, Lammers and Manolescu concern the same measure, so that their convergence in domains holds, for $c\in[1,2]$ and with constants depending on $\Delta$, wherever the manuscript's full-plane theorem holds. \end{abstract} \setcounter{tocdepth}{1} \tableofcontents \input{sec1-intro} \input{sec2-gradient} \input{sec3-swaps} \input{sec4-fold} \input{sec5-plane} \input{sec6-proofs} \input{sec7-domains} \appendix \input{appA} \begin{thebibliography}{99} \bibitem{ADHLM} E.~Averous, H.~Duminil-Copin, T.~He, P.~Lammers, and I.~Manolescu. \newblock Conformal invariance of the six-vertex model's height function. \newblock Preprint, \href{https://arxiv.org/abs/2610.07454}{arXiv:2610.07454}, 2026. \bibitem{BGMT} S.~Barbieri, R.~G\'omez, B.~Marcus, and S.~Taati. \newblock Equivalence of relative {G}ibbs and relative equilibrium measures for actions of countable amenable groups. \newblock {\em Nonlinearity}, 33, 2020. \newblock \href{https://arxiv.org/abs/1809.00078}{arXiv:1809.00078}. \bibitem{BurtonKeane} R.~M. Burton and M.~Keane. \newblock Density and uniqueness in percolation. \newblock {\em Comm. Math. Phys.}, 121(3):501--505, 1989. \bibitem{CPST} N.~Chandgotia, R.~Peled, S.~Sheffield, and M.~Tassy. \newblock Delocalization of uniform graph homomorphisms from $\Z^2$ to $\Z$. \newblock {\em Comm. Math. Phys.}, 387(2):621--647, 2021. \newblock \href{https://arxiv.org/abs/1810.10124}{arXiv:1810.10124}. \bibitem{DKLM} H.~Duminil-Copin, K.~K. Kozlowski, P.~Lammers, and I.~Manolescu. \newblock Gaussian free field convergence of the six-vertex model with $-1\le\Delta\le-\frac12$. \newblock Preprint, \href{https://arxiv.org/abs/2603.06268}{arXiv:2603.06268}, 2026. \bibitem{DKMO} H.~Duminil-Copin, A.~Karrila, I.~Manolescu, and M.~Oulamara. \newblock Delocalization of the height function of the six-vertex model. \newblock {\em J. Eur. Math. Soc.}, 26(11):4131--4190, 2024. \newblock \href{https://arxiv.org/abs/2012.13750}{arXiv:2012.13750}. \bibitem{EdwardsSokal} R.~G. Edwards and A.~D. Sokal. \newblock Generalization of the {F}ortuin--{K}asteleyn--{S}wendsen--{W}ang representation and {M}onte {C}arlo algorithm. \newblock {\em Phys. Rev. D}, 38:2009--2012, 1988. \bibitem{Erdos} P.~Erd\H{o}s. \newblock On a lemma of {L}ittlewood and {O}fford. \newblock {\em Bull. Amer. Math. Soc.}, 51:898--902, 1945. \bibitem{FK} C.~M. Fortuin and P.~W. Kasteleyn. \newblock On the random-cluster model. {I}. {I}ntroduction and relation to other models. \newblock {\em Physica}, 57:536--564, 1972. \bibitem{GlazmanLammers} A.~Glazman and P.~Lammers. \newblock Delocalisation and continuity in {2D}: loop {$O(2)$}, six-vertex, and random-cluster models. \newblock {\em Comm. Math. Phys.}, 406(5):108, 2025. \href{https://arxiv.org/abs/2306.01527}{arXiv:2306.01527}. \bibitem{GlazmanPeled} A.~Glazman and R.~Peled. \newblock On the transition between the disordered and antiferroelectric phases of the 6-vertex model. \newblock {\em Electron. J. Probab.}, 28:1--53, 2023. \newblock \href{https://arxiv.org/abs/1909.03436}{arXiv:1909.03436}. \bibitem{LammersTassy} P.~Lammers and M.~Tassy. \newblock Macroscopic behavior of {L}ipschitz random surfaces. \newblock {\em Probab. Math. Phys.}, 5(1):177--267, 2024. \href{https://arxiv.org/abs/2004.15025}{arXiv:2004.15025}; theorem numbers refer to arXiv version~1. \bibitem{Lis} M.~Lis. \newblock On delocalization in the six-vertex model. \newblock {\em Comm. Math. Phys.}, 383(2):1181--1205, 2021. \newblock \href{https://arxiv.org/abs/2004.05337}{arXiv:2004.05337}. \bibitem{Lis22} M.~Lis. \newblock Spins, percolation and height functions. \newblock {\em Electron. J. Probab.}, 2022. \newblock \href{https://arxiv.org/abs/1909.07351}{arXiv:1909.07351}. \bibitem{OAI225} \mbox{OpenAI}. \newblock The {G}aussian free field limit of the balanced six-vertex model with variance multiplier $1/\arcsin(c/2)$. \newblock \mbox{OpenAI} Math Release preprint, September 23, 2026. \newblock \href{https://github.com/openai/math/tree/4eaee87548250b2682affda7d05d947c05554bae/preprints/The-Gaussian-free-field-limit-of-the-balanced-six-vertex-model-with-variance-multiplier-1-over-arcsin-c-over-2-September-23-2026}{\texttt{github.com/openai/math}}, commit \texttt{4eaee87}. \bibitem{Ryan} K.~Ryan. \newblock The spin-1/2 {H}eisenberg {XXZ} chain and the {L}orentz mirror model with loop weight~$2$. \newblock Preprint, \href{https://arxiv.org/abs/2608.21306}{arXiv:2608.21306}, 2026. \bibitem{Sheffield} S.~Sheffield. \newblock Random surfaces. \newblock {\em Ast\'erisque}, 304, 2005. \href{https://arxiv.org/abs/math/0304049}{arXiv:math/0304049}; page and theorem numbers refer to arXiv version~3. \bibitem{vEHL} D.~van Engelenburg, L.~Heeney, and M.~Lis. \newblock Double cluster swapping for spin models: {P}faffian relations and sharpness. \newblock Preprint, \href{https://arxiv.org/abs/2609.01362}{arXiv:2609.01362}, 2026. \end{thebibliography} \end{document}