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Discontinuous transition in 2D Potts: I. Order-Disorder Interface convergence

Moritz Dober, Alexander Glazman, Sébastien Ott

TL;DR

This work proves that the order-disorder interface in the planar $q$-state Potts model with $q>4$ converges to a Brownian bridge under diffusive scaling, in the Dobrushin boundary setup. The authors engineer a novel chain of graphical couplings linking FK-percolation, the six-vertex model, and the Ashkin–Teller random-cluster representation, and develop an Ornstein–Zernike renewal framework for long ATRC clusters. Exponential mixing and renewal structure enable a precise OZ description, which is then transferred to the FK-percolation and Potts interfaces, establishing the scaling limit and fluctuations. A companion paper addresses the order-order Dobrushin case and the emergence of a wetting layer, completing the scaling-branch picture for discontinuous two-dimensional phase transitions and their interface geometry.

Abstract

It is known that the planar q-state Potts model undergoes a discontinuous phase transition when q > 4 and there are exactly q + 1 extremal Gibbs measures at the transition point: q ordered (monochromatic) measures and one disordered (free). We focus on the Potts model under the Dobrushin order-disorder boundary conditions on a finite $N\times N$ part of the square grid. Our main result is that this interface is a well defined object, has $\sqrt{N}$ fluctuations, and converges to a Brownian bridge under diffusive scaling. The same holds also for the corresponding FK-percolation model for all q > 4. Our proofs rely on a coupling between FK-percolation, the six-vertex model, and the random-cluster representation of an Ashkin-Teller model (ATRC), and on a detailed study of the latter. The coupling relates the interface in FK-percolation to a long subcritical cluster in the ATRC model. For this cluster, we develop a ``renewal picture'' à la Ornstein-Zernike. This is based on fine mixing properties of the ATRC model that we establish using the link to the six-vertex model and its height function. Along the way, we derive various properties of the Ashkin-Teller model, such as Ornstein-Zernike asymptotics for its two-point function. In a companion work, we provide a detailed study of the Potts model under order-order Dobrushin conditions. We show emergence of a free layer of width $\sqrt{N}$ between the two ordered phases (wetting) and establish convergence of its boundaries to two Brownian bridges conditioned not to intersect.

Discontinuous transition in 2D Potts: I. Order-Disorder Interface convergence

TL;DR

This work proves that the order-disorder interface in the planar -state Potts model with converges to a Brownian bridge under diffusive scaling, in the Dobrushin boundary setup. The authors engineer a novel chain of graphical couplings linking FK-percolation, the six-vertex model, and the Ashkin–Teller random-cluster representation, and develop an Ornstein–Zernike renewal framework for long ATRC clusters. Exponential mixing and renewal structure enable a precise OZ description, which is then transferred to the FK-percolation and Potts interfaces, establishing the scaling limit and fluctuations. A companion paper addresses the order-order Dobrushin case and the emergence of a wetting layer, completing the scaling-branch picture for discontinuous two-dimensional phase transitions and their interface geometry.

Abstract

It is known that the planar q-state Potts model undergoes a discontinuous phase transition when q > 4 and there are exactly q + 1 extremal Gibbs measures at the transition point: q ordered (monochromatic) measures and one disordered (free). We focus on the Potts model under the Dobrushin order-disorder boundary conditions on a finite part of the square grid. Our main result is that this interface is a well defined object, has fluctuations, and converges to a Brownian bridge under diffusive scaling. The same holds also for the corresponding FK-percolation model for all q > 4. Our proofs rely on a coupling between FK-percolation, the six-vertex model, and the random-cluster representation of an Ashkin-Teller model (ATRC), and on a detailed study of the latter. The coupling relates the interface in FK-percolation to a long subcritical cluster in the ATRC model. For this cluster, we develop a ``renewal picture'' à la Ornstein-Zernike. This is based on fine mixing properties of the ATRC model that we establish using the link to the six-vertex model and its height function. Along the way, we derive various properties of the Ashkin-Teller model, such as Ornstein-Zernike asymptotics for its two-point function. In a companion work, we provide a detailed study of the Potts model under order-order Dobrushin conditions. We show emergence of a free layer of width between the two ordered phases (wetting) and establish convergence of its boundaries to two Brownian bridges conditioned not to intersect.

Paper Structure

This paper contains 50 sections, 47 theorems, 285 equations, 29 figures, 1 algorithm.

Key Result

Theorem 1

Let $q>4$ be integer and take $T=T_c(q)$. For $n\in\mathbb{N}$, sample $\Gamma_{\mathtt{Potts}}^{\pm,n}$ and $\tilde{\Gamma}_{\mathtt{Potts}}^{\pm,n}$ from $\mathtt{Potts}_{\Lambda_n;T_c(q),q}^{1/\mathrm{f}}$ as described above. Then, as $n$ tends to infinity,

Figures (29)

  • Figure 1: Sample of a 600x600 Potts model with 25 colours at $T_c(25)$ with Dobrushin boundary conditions. Left: order-disorder interface; upper part has blue b.c., bottom has white b.c. (no colour favoured), colours are: blue for the first and interpolate between yellow and red for colours 2 to 25. Right: colours are: blue for the first, red for the second, and interpolate between yellow and orange for colours 3 to 25.
  • Figure 2: Left: wired-free Dobrushin boundary condition. Right: the graph $G_{2}$.
  • Figure 3: Left: Tile associated to a mid-edge. Right: Tile centred at the middle of a horizontal primal edge (solid black) or its associated vertical dual edge (dashed black), with its two possible local loop configurations.
  • Figure 4: Dobrushin boundary condition for the six-vertex height function.
  • Figure 5: Left: the sets $\Lambda_{2,2}$ (solid) and $\Lambda'_{2,2}$ (hollow). Right: the inner tiles $A^\mathrm{i}_{2,2}$ (white) and the boundary tiles $\partial A_{2,2}$ (grey).
  • ...and 24 more figures

Theorems & Definitions (108)

  • Theorem 1
  • Theorem 2
  • Proposition 1.1
  • Theorem 3
  • Lemma 3.1: PfiVel97
  • Proposition 3.2
  • Theorem 4
  • Corollary 3.3
  • Theorem 5
  • proof
  • ...and 98 more