Continuous and discontinuous phase transitions in hypergraph processes

dc.creatorDarling, R. W. R.
dc.creatorLevin, D. A.
dc.creatorNorris, J. R.
dc.date2003-12-24
dc.date2004-03-02
dc.date.accessioned2026-07-07T05:04:11Z
dc.date.available2026-07-07T05:04:11Z
dc.descriptionLet V denote a set of N vertices. To construct a "hypergraph process", create a new hyperedge at each event time of a Poisson process; the cardinality K of this hyperedge is random, with arbitrary probability generating function r(x), except that we assume P(K=1) +P(K=2) > 0. Given K=k, the k vertices appearing in the new hyperedge are selected uniformly at random from V. Hyperedges of cardinality 1 are called patches, and serve as a way of selecting root vertices. Identifiable vertices are those which are reachable from these root vertices, in a strong sense which generalizes the notion of graph component. Hyperedges are also called identifiable if all of their vertices are identifiable. We use "fluid limit" scaling: hyperedges arrive at rate N, and we study structures of size O(1) and O(N). After division by N, numbers of identifiable vertices and reducible hyperedges exhibit phase transitions, which may be continuous or discontinuous depending on the shape of the structure function -log(1 - x)/r'(x), for x in (0,1). Both the case P(K=1) > 0 and the case P(K=1) = 0 < P(K=2) are considered; for the latter, a single extraneous patch is added to mark the root vertex.
dc.description25 pages, 2 figures. Revised version. To appear in Random Structures & Algorithms
dc.identifierhttps://arxiv.org/abs/math/0312451
dc.identifierhttp://arxiv.org/abs/math/0312451
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/69704
dc.subjectProbability
dc.subjectCombinatorics
dc.subject05C80;60F17;05C85
dc.titleContinuous and discontinuous phase transitions in hypergraph processes
dc.typetext

Files

Collections