Sharp phase transition for the continuum Widom-Rowlinson model

TL;DR

This paper demonstrates a sharp phase transition in the continuum Widom-Rowlinson model, linking percolation thresholds with liquid-gas phase transitions and establishing conditions for uniqueness and non-uniqueness of Gibbs states.

Contribution

It establishes a precise connection between percolation thresholds and phase transition boundaries in the Widom-Rowlinson model, partially confirming a long-standing conjecture.

Findings

Existence of exponential decay in subcritical phase for any positive inverse temperature

Linear lower bound of connectivity in supercritical phase

Non-uniqueness of Gibbs states occurs if and only if activity equals inverse temperature for large 2

Abstract

The Widom-Rowlinson model (or the Area-interaction model) is a Gibbs point process in $\mathbb{R}^d$ with the formal Hamiltonian $H(\omega)=\text{Volume}(\cup_{x\in\omega} B_1(x))$, where $\omega$ is a locally finite configuration of points and $B_1(x)$ denotes the unit closed ball centred at $x$. The model is tuned by two parameters: the activity $z>0$ and the inverse temperature $\beta\ge 0$. We investigate the phase transition of the model in the point of view of percolation theory and the liquid-gas transition. First, considering the graph connecting points with distance smaller than $2r>0$, we show that for any $\beta>0$, there exists $0<\tilde{z}^a(\beta, r)<+\infty$ such that an exponential decay of connectivity at distance $n$ occurs in the subcritical phase and a linear lower bound of the connection at infinity holds in the supercritical case. Secondly we study a standard liquid-gas phase transition related to the uniqueness/non-uniqueness of Gibbs states depending on the parameters $z,\beta$. Old results claim that a non-uniqueness regime occurs for $z=\beta$ large enough and it is conjectured that the uniqueness should hold outside such an half line ($z=\beta\ge \beta_c>0$). We solve partially this conjecture by showing that for $\beta$ large enough the non-uniqueness holds if and only if $z=\beta$. We show also that this critical value $z=\beta$ corresponds to the percolation threshold $ \tilde{z}^a(\beta, r)=\beta$ for $\beta$ large enough, providing a straight connection between these two notions of phase transition.