2012
DOI: 10.1007/s00440-012-0453-0
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Matchings on infinite graphs

Abstract: Elek and Lippner (2010) showed that the convergence of a sequence of bounded-degree graphs implies the existence of a limit for the proportion of vertices covered by a maximum matching. We provide a characterization of the limiting parameter via a local recursion defined directly on the limit of the graph sequence. Interestingly, the recursion may admit multiple solutions, implying non-trivial long-range dependencies between the covered vertices. We overcome this lack of correlation decay by introducing a per… Show more

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Cited by 40 publications
(82 citation statements)
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“…Analytic continuation techniques are used in order to extend results from "large" x to all positive x. Our results extend those of Bordenave, Lelarge, Salez [10] which are valid for graphs with bounded degree, and are generalised to arbitrary degree only for x → 0 (this is called the maximum matching problem and it is not treated in this paper, see instead [11] for its first solution in the Erdős-Rényi case and [12,13] for other generalisations). A complete theoretical physics picture of the monomer-dimer model (matching problem) on sparse random graphs was given by Zdeborová and Mézard in [14], where several quantities were computed including the pressure of the model, using the so called replica-symmetric version of the cavity method.…”
Section: Introductionsupporting
confidence: 65%
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“…Analytic continuation techniques are used in order to extend results from "large" x to all positive x. Our results extend those of Bordenave, Lelarge, Salez [10] which are valid for graphs with bounded degree, and are generalised to arbitrary degree only for x → 0 (this is called the maximum matching problem and it is not treated in this paper, see instead [11] for its first solution in the Erdős-Rényi case and [12,13] for other generalisations). A complete theoretical physics picture of the monomer-dimer model (matching problem) on sparse random graphs was given by Zdeborová and Mézard in [14], where several quantities were computed including the pressure of the model, using the so called replica-symmetric version of the cavity method.…”
Section: Introductionsupporting
confidence: 65%
“…This lemma already appeared in [10] and in particular point ii can be seen also as a consequence of theorem 4.2 in [2].…”
Section: Definitions and General Properties Of The Monomerdimer Modelmentioning
confidence: 65%
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“…This quickly leads to a proof of Theorem 1 (Section 7). In spirit, the role of the perturbative parameter ε > 0 is comparable to that of the temperature in [10], although no Gibbs-Boltzmann measure is involved in the present work.…”
Section: Proof Ingredients and Related Workmentioning
confidence: 99%