2016
DOI: 10.1007/s10955-015-1433-4
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Representation and Poly-time Approximation for Pressure of $$\mathbb {Z}^2$$ Lattice Models in the Non-uniqueness Region

Abstract: ABSTRACT. We develop a new pressure representation theorem for nearest-neighbour Gibbs interactions and apply this to obtain the existence of efficient algorithms for approximating the pressure in the 2-dimensional ferromagnetic Potts, multi-type WidomRowlinson and hard-core models. For Potts, our results apply to every inverse temperature but the critical. For Widom-Rowlinson and hard-core, they apply to certain subsets of both the subcritical and supercritical regions. The main novelty of our work is in the … Show more

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Cited by 25 publications
(8 citation statements)
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“…Date: 6/29/2018. 1 results apply to a wide class of statistical mechanics models, including the ferromagnetic Potts and hard-core models. The following theorem is representative of our results.…”
Section: Introductionmentioning
confidence: 89%
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“…Date: 6/29/2018. 1 results apply to a wide class of statistical mechanics models, including the ferromagnetic Potts and hard-core models. The following theorem is representative of our results.…”
Section: Introductionmentioning
confidence: 89%
“…where Z(G, z) is the polymer partition function defined in (1). Under the conditions for which we obtain an FPTAS for Z(G, z) we obtain an efficient sampling algorithm.…”
Section: 1mentioning
confidence: 99%
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“…Analogues of the Kolmogorov-Sinai entropy in higher dimensions for Markov random fields, in which again conditioning on a measure in a restricted number of directions, or on lexicographic pasts, takes place, also have been considered, for example in [1,57]. Existence of such entropies turns out to be a weaker property than continuity.…”
Section: Entropiesmentioning
confidence: 99%
“…Proof. By adapting [1,Theorem 7.3] to the context of Gibbs (Z 2 , H, Φ)-specifications π, we know that if π is such that Q(π) < p c (Z 2 ), then π satisfies exponential SSM, where p c (Z 2 ) denotes the critical probability for Bernoulli site percolation on Z 2 and Q(π) is defined as Given q ∈ N, consider the graph H q as shown in Figure 11. The graph H q consists of a complete graph K q+1 and two other extra vertices a and b both adjacent to every vertex in the complete graph.…”
Section: Examplesmentioning
confidence: 99%