Exact solution of the classical dimer model on a triangular lattice: Monomer-monomer correlations

TL;DR

This paper derives an exact asymptotic formula for monomer-monomer correlations in the classical dimer model on a triangular lattice, revealing a phase transition at a critical weight value and providing explicit formulas for key parameters.

Contribution

It extends the Borodin-Okounkov-Case-Geronimo formula to block Toeplitz determinants and analyzes Fredholm determinants to obtain precise asymptotics for the model.

Findings

Identifies critical point at t=1/2 separating different decay behaviors.

Provides explicit formulas for correlation decay parameters.

Shows exponential decay of correlations with different oscillatory behavior in subcritical and supercritical regimes.

Abstract

We obtain an asymptotic formula, as $n\to\infty$, for the monomer-monomer correlation function $K_2(x,y)$ in the classical dimer model on a triangular lattice, with the horizontal and vertical weights $w_h=w_v=1$ and the diagonal weight $w_d=t>0$, where $x$ and $y$ are sites $n$ spaces apart in adjacent rows. We find that $t_c=\frac{1}{2}$ is a critical value of $t$. We prove that in the subcritical case, $0<t<\frac{1}{2}$, as $n\to\infty$, $K_2(x,y)=K_2(\infty)\left[1-\frac{e^{-n/\xi}}{n}\,\Big(C_1+C_2(-1)^n+\mathcal O(n^{-1})\Big)\right]$, with explicit formulae for $K_2(\infty)$, $\xi$, $C_1$, and $C_2$. In the supercritical case, $\frac{1}{2} < t < 1$, we prove that as $n\to\infty$, $K_2(x,y)=K_2(\infty)\Bigg[1- \frac{e^{-n/\xi}}{n}\, \Big(C_1\cos(\omega n+\varphi_1)+C_2(-1)^n\cos(\omega n+\varphi_2)+ C_3+C_4(-1)^n$ $+\mathcal O(n^{-1})\Big)\Bigg]$, with explicit formulae for $K_2(\infty)$, $\xi$, $\omega$, and $C_1$, $C_2$, $C_3$, $C_4$, $\varphi_1$, $\varphi_2$. The proof is based on an extension of the Borodin-Okounkov-Case-Geronimo formula to block Toeplitz determinants and on an asymptotic analysis of the Fredholm determinants in hand.