Geometric spanners with applications in wireless networks

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dc.contributor.authorSchindelhauer, Christianko
dc.contributor.authorVolbert, Klausko
dc.contributor.authorZiegler, Martinko
dc.date.accessioned2016-04-12T07:52:09Z-
dc.date.available2016-04-12T07:52:09Z-
dc.date.created2015-09-17-
dc.date.created2015-09-17-
dc.date.issued2007-04-
dc.identifier.citationCOMPUTATIONAL GEOMETRY-THEORY AND APPLICATIONS, v.36, no.3, pp.197 - 214-
dc.identifier.issn0925-7721-
dc.identifier.urihttp://hdl.handle.net/10203/203398-
dc.description.abstractIn this paper we investigate the relations between spanners, weak spanners, and power spanners in R-D for any dimension D and apply our results to topology control in wireless networks. For c is an element of R, a c-spanner is a subgraph of the complete Euclidean graph satisfying the condition that between any two vertices there exists a path of length at most c-times their Euclidean distance. Based on this ability to approximate the complete Euclidean graph, sparse spanners have found many applications, e.g., in FPTAS, geometric searching, and radio networks. In a weak c-spanner, this path may be arbitrarily long, but must remain within a disk or sphere of radius c-times the Euclidean distance between the vertices. Finally in a c-power spanner, the total energy consumed on Such a path, where the energy is given by the sum of the squares of the edge lengths on this path, must be at most c-times the square of the Euclidean distance of the direct edge or communication link. While it is known that any c-spanner is also both a weak C-1-spanner and a C-2-power spanner for appropriate C-1, C-2 depending only on c but not on the graph under consideration, we show that the converse is not true: there exists a family of c(1)-power spanners that are not weak C-spanners and also a family of weak c(2)-spanners that are not C-spanners for any fixed C. However a main result of this paper reveals that any weak c-spanner is also a C-power spanner for an appropriate constant C. We further generalize the latter notion by considering (c, delta)-power spanners where the sum of the delta th powers of the lengths has to be bounded, so (c, 2)-power spanners coincide with the usual power spanners and (c, I)-power spanners are classical spanners. Interestingly, these (c, delta)-power spanners form a strict hierarchy where the above results still hold for any delta >= D some even hold for delta > 1 while counter-examples exist for delta < D. We show that every self-similar curve of fractal dimension D-f >= delta is not a (C, delta)-power spanner for any fixed C, in general. Finally, we consider the sparsified Yao-graph (SparsY-graph or YY) that is a well-known sparse topology for wireless networks. We prove that all SparsY-graphs are weak c-spanners for a constant c and hence they allow us to approximate energy-optimal wireless networks by a constant factor. (c) 2006 Elsevier B.V. All rights reserved.-
dc.languageEnglish-
dc.publisherELSEVIER SCIENCE BV-
dc.subjectAD HOC NETWORKS-
dc.titleGeometric spanners with applications in wireless networks-
dc.typeArticle-
dc.identifier.wosid000244221700004-
dc.identifier.scopusid2-s2.0-84867970573-
dc.type.rimsART-
dc.citation.volume36-
dc.citation.issue3-
dc.citation.beginningpage197-
dc.citation.endingpage214-
dc.citation.publicationnameCOMPUTATIONAL GEOMETRY-THEORY AND APPLICATIONS-
dc.identifier.doi10.1016/j.comgeo.2006.02.001-
dc.contributor.localauthorZiegler, Martin-
dc.contributor.nonIdAuthorSchindelhauer, Christian-
dc.contributor.nonIdAuthorVolbert, Klaus-
dc.type.journalArticleArticle; Proceedings Paper-
dc.subject.keywordPlusAD HOC NETWORKS-
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