Sharp phase transition for the continuum ...
Document type :
Pré-publication ou Document de travail
Title :
Sharp phase transition for the continuum Widom-Rowlinson model
Author(s) :
Dereudre, David [Auteur]
Laboratoire de Mathématiques et leurs Applications de Valenciennes - EA 4015 [LAMAV]
Houdebert, Pierre [Auteur]
Laboratoire Paul Painlevé - UMR 8524 [LPP]
Laboratoire de Mathématiques et leurs Applications de Valenciennes - EA 4015 [LAMAV]
Houdebert, Pierre [Auteur]
Laboratoire Paul Painlevé - UMR 8524 [LPP]
English keyword(s) :
Gibbs point process
DLR equations
Boolean model
contin-uum percolation
random cluster model
Fortuin-Kasteleyn representation
randomised tree algorithm
OSSS inequality
DLR equations
Boolean model
contin-uum percolation
random cluster model
Fortuin-Kasteleyn representation
randomised tree algorithm
OSSS inequality
HAL domain(s) :
Mathématiques [math]/Probabilités [math.PR]
English abstract : [en]
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 ...
Show more >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.Show less >
Show more >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.Show less >
Language :
Anglais
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27 pages, 1 figure
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