1993
DOI: 10.1007/bf01192132
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Large deviations and the maximum entropy principle for marked point random fields

Abstract: Summary.We establish large deviation principles for the stationary and the individual empirical fields of Poisson, and certain interacting, random fields of marked point particles in IR~. The underlying topologies are induced by a class of not necessarily bounded local functions, and thus finer than the usual weak topologies. Our methods yield further that the limiting behaviour of conditional Poisson distributions, as well as certain distributions of Gibbsian type, is governed by the maximum entropy principle… Show more

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Cited by 71 publications
(149 citation statements)
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“…[10]. In this paper we study large deviations from the ergodic theorem (1.2) when P is Gibbsian relative to a suitable pair interaction q~.…”
Section: Introductionmentioning
confidence: 99%
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“…[10]. In this paper we study large deviations from the ergodic theorem (1.2) when P is Gibbsian relative to a suitable pair interaction q~.…”
Section: Introductionmentioning
confidence: 99%
“…A configuration of particles (without multiple occupancies) is de-scribed by a locally finite subset co of R d, i.e., a set co C R d having finite intersection with every bounded set. We write f2 for the set of all such configurations co. ~2 is equipped with the a-algebra 9 c generated by the counting variables Ne:co--+ card(co N B) for Bore1 subsets B of R d. It is well-known [10,13] that 5 c is the Borel a-algebra for a natural Polish topology on Q. The translation group 0 = (OX)xERd acting on (~,S) is defined by 0xco = {y -x :y E co},co c f~,x c R a.…”
Section: Introductionmentioning
confidence: 99%
“…The following lemma, for which the proof is almost the same as the one given in [4], ensures that (μ n ) and (μ n ) are asymptotically equivalent for the topology τ W .…”
Section: Existence Of Quermass-interaction Processesmentioning
confidence: 81%
“…Let us remark that Assumption 2.1 of [4] with the function ψ : R → 1 + R 2 is exactly our assumption (H). So, it plays a fundamental role at this part of the proof of Theorem 2.1.…”
Section: Proposition 32 ([4 Proposition 26]) For Every a > 0 Thmentioning
confidence: 99%
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