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A Cellular Representation of the Potts Lattice Higgs Model

Summer Eldridge, Malin P. Forsström, Benjamin Schweinhart

Abstract

The $i$-dimensional Potts lattice Higgs model is a random assignment of spins in $\mathbb{Z}_q$ to the $i$-dimensional cells of a cell complex induced by a Hamiltonian with a Potts interaction on the $(i+1)$-cells and an additional term playing the role of an external field. We develop a representation of this model as a pair of dependent plaquette percolations, and prove that Wilson line expectations can be expressed in terms of the probability of a topological event. As an application, we prove the existence of a phase transition for the Marcu--Fredenhagen ratio in the Potts lattice Higgs model on $\mathbb{Z}^d$ when $i=1.$

A Cellular Representation of the Potts Lattice Higgs Model

Abstract

The -dimensional Potts lattice Higgs model is a random assignment of spins in to the -dimensional cells of a cell complex induced by a Hamiltonian with a Potts interaction on the -cells and an additional term playing the role of an external field. We develop a representation of this model as a pair of dependent plaquette percolations, and prove that Wilson line expectations can be expressed in terms of the probability of a topological event. As an application, we prove the existence of a phase transition for the Marcu--Fredenhagen ratio in the Potts lattice Higgs model on when
Paper Structure (20 sections, 27 theorems, 146 equations, 5 figures)

This paper contains 20 sections, 27 theorems, 146 equations, 5 figures.

Key Result

Theorem 5

Let $X$ be a finite cell complex, $q$ be a prime integer, and $\beta_2,\beta_1\geq 0.$ If $p_2=1-e^{-{\beta_2}},$$p_1=1-e^{-{\beta_1}}$, $k_2=\frac{p_2}{1-p_2}=e^{\beta_2}-1,$ and $k_1=\frac{p_1}{1-p_1}=e^{\beta_1}-1$, then there is a coupling $\kappa=\kappa_{k_2,k_1,q,i,X}$, ${\kappa \colon C^i(X;\ which satisfies the following.

Figures (5)

  • Figure 1: Two illustrations of the event $V_{\gamma}.$ On the left, $P_2$ is depicted by the collection of light blue squares and $P_1$ by the orange bonds. The events $V_{\gamma_1}$ and $V_{\gamma_2}$ both occur, where $\gamma_1$ and $\gamma_2$ are the loop and path shown in dark gray. On the right, $P_2$ is shown by the blue surface and $P_1$ by the orange line segment. $\gamma$ is depicted in black. Here, $V_{\gamma}$ occurs when homology is taken with coefficients in $\mathbb{Z}_2$ but the plaquettes in the orange surface cannot be compatibly oriented to yield a null-homology when coefficients are taken in a field of odd characteristic. The figure on the right was adapted from Figure 1 of duncan2025sharp which was in turn inspired by Figure 1 of aizenman1983sharp.
  • Figure 2: In the figures above, we draw the paths and surfaces used in the definitions of the Marcu--Fredenhagen ratio for $i = 1$ and $i = 2$ respectively.
  • Figure 3: Conjectured limiting behavior of $R\left( \beta_2,\beta_1,n \right)$. We will not address the difference between the Confinement phase and the Higgs phase here. We propose to rigorously establish the diagram in the blue regions.
  • Figure 4: A cell complex with six vertices, seven edges, and one face.
  • Figure :

Theorems & Definitions (61)

  • Definition 1: Potts lattice Higgs Model
  • Definition 2: Percolation Subcomplex
  • Definition 3
  • Definition 4: Coupled Plaquette Percolation (CPP)
  • Theorem 5
  • Definition 6: $V_\gamma$ and $W_\gamma$
  • Theorem 7
  • Definition 8: The Marcu--Fredenhagen ratio for $i = 1$
  • Definition 9: The topological Marcu--Fredenhagen ratio
  • Theorem 10
  • ...and 51 more