Abstract
For a pair potential \(\Phi \) in a general underlying space X satisfying some natural and sufficiently general conditions in the sense of Penrose (J Math Phys 4:1312, 1963) and Poghosyan and Ueltschi (J Math Phys 50:053509, 2009) together with a locally finite measure \(\varrho \) on X we define by means of the so-called Ursell kernel a function r which is shown to be the correlation function of a unique process \(\mathrm{G}\), the limiting Gibbs process for \((\Phi ,\varrho )\) with empty boundary conditions. This process is exhibited as a Gibbs process in the sense of Dobrushin, Lanford and Ruelle for a class of pair potentials, which contains classical stable and hard-core potentials that are called Penrose potentials here. Particularly, a class of positive potentials is included. Finally, for some class of Penrose potentials, we show that \(\mathrm{G}\) is the unique Gibbs process for \(\Phi \). We use the classical method of Kirkwood–Salsburg equations. A decisive role is played by a generalization of Ruelle’s estimate for correlation functions.
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Notes
This explains the choice of our title.
This notion is weaker than Penrose-stability and stronger than the classical notion of stability.
i.e., Dobrushin, Lanford and Ruelle.
Usually Radon measures are considered on locally compact and second countable Hausdorff topological spaces.
This can be realized by the \(1-1\) correspondence \(\mu \leftrightarrow \kappa =\sum _{x\in \mu ^*}\sum _{i=1}^{\mu \{x\}}\varepsilon _{(x,i)}\) between \(\mu \in {\mathscr {M}}^{\cdot \cdot }(X)\) and \(\kappa \in \mathscr {M}^{\cdot }(X\times \mathbb {N})\).
This notion will play a role in the definition of \(\mathscr {P}\)-stability and in the proof of Lemma 14.
Also called factorial moment measure.
The definition of this regularity condition can be found at the beginning of Sect. 10.
Thus, we realize Minlos’ program on limiting Gibbs processes from [22] by means of methods from point process theory which had been developed later.
Although the function \(g+\Phi _x\) is not an element of U we speak, in an abuse of language, of the Laplace transform evaluated in \(g+\Phi _x\).
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Acknowledgements
We thank one of the referees for his valuable remarks which lead to substantial improvements of this paper. S.P. is grateful to Prof. Sylvie Roelly for her hospitality at Potsdam University. H.Z. thanks Sylvie Roelly and Alexander Zass for illuminating discussions on the uniqueness problem.
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Communicated by Christian Maes.
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In memoriam Jean Ginibre.
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Poghosyan, S., Zessin, H. Penrose-Stable Interactions in Classical Statistical Mechanics. Ann. Henri Poincaré 23, 739–771 (2022). https://doi.org/10.1007/s00023-021-01098-1
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DOI: https://doi.org/10.1007/s00023-021-01098-1