{ "id": "1611.05728", "version": "v1", "published": "2016-11-17T15:11:00.000Z", "updated": "2016-11-17T15:11:00.000Z", "title": "Component structure of the configuration model: barely supercritical case", "authors": [ "Remco van der Hofstad", "Svante Janson", "Malwina Luczak" ], "comment": "46 pages", "categories": [ "math.PR" ], "abstract": "We study near-critical behavior in the configuration model. Let $D_n$ be the degree of a random vertex. We let $\\nu_n={\\mathbb E} [D_n(D_n-1)]/{\\mathbb E}[D_n]$ and, assuming that $\\nu_n \\to 1$ as $n \\to \\infty$, we write $\\varepsilon_n=\\nu_n-1$. We call the setting where $\\varepsilon_n n^{1/3}/({\\mathbb E}[D_n^3])^{2/3} \\to \\infty$ the {\\it barely supercritical} regime. We further assume that the variance of $D_n$ is uniformly bounded as $n \\to \\infty$. Let $D_n^*$ denote the size-biased version of $D_n$. We prove that there is a unique giant component of size $n \\rho_n {\\mathbb E} D_n (1+o(1))$, where $\\rho_n$ denotes the survival probability of a branching process with offspring distribution $D_n^*-1$. This extends earlier results of Janson and Luczak~\\cite{JanLuc07}, as well as those of Janson, Luczak, Windridge and House~\\cite{SJ300} to the case where the third moment of $D_n$ is unbounded, filling the gap in the literature. We further study the size of the largest component in the \\emph{critical} regime, where $\\varepsilon_n = O(n^{-1/3} ({\\mathbb E} D_n^3)^{2/3})$, extending and complementing results of Hatami and Molloy~\\cite{HatamiMolloy}.", "revisions": [ { "version": "v1", "updated": "2016-11-17T15:11:00.000Z" } ], "analyses": { "subjects": [ "05C80", "60C05" ], "keywords": [ "configuration model", "barely supercritical case", "component structure", "extends earlier results", "unique giant component" ], "note": { "typesetting": "TeX", "pages": 46, "language": "en", "license": "arXiv", "status": "editable" } } }