2022
DOI: 10.1002/jgt.22901
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Hamiltonicity of graphs perturbed by a random geometric graph

Abstract: We study Hamiltonicity in graphs obtained as the union of a deterministic n-vertex graph H with linear degrees and a d-dimensional random geometric graph G n r ( , ) d , for any ≥ d 1. We obtain an asymptotically optimal bound on the minimum r for which a.a.s. ∪ H G n r ( , ) d is Hamiltonian. Our proof provides a linear time algorithm to find a Hamilton cycle in such graphs.

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Cited by 5 publications
(4 citation statements)
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“…We believe it would be interesting to study graphs perturbed by a random graph with a fixed degree sequence as well. Very recently, the first author has also considered Hamiltonicity of graphs perturbed by a random geometric graph [18]. Of course, this study should also be extended to other graph properties.…”
Section: Concluding Remarks and Open Problemsmentioning
confidence: 99%
“…We believe it would be interesting to study graphs perturbed by a random graph with a fixed degree sequence as well. Very recently, the first author has also considered Hamiltonicity of graphs perturbed by a random geometric graph [18]. Of course, this study should also be extended to other graph properties.…”
Section: Concluding Remarks and Open Problemsmentioning
confidence: 99%
“…The study of the emergence of various spanning configurations in randomly perturbed (hyper)graphs dates back to the work of Bohman et al [12], and received significant attention in recent years, see for example, [5,911,14,15,17,27,28,3032] to name just a few. In most results in this area, the random perturbation is the binomial random graph 𝔾false(n,pfalse) (or the, essentially equivalent, Erdős‐Rényi random graph 𝔾false(n,mfalse)); however, quite recently other distributions have been considered, such as random geometric graphs [19] and random regular graphs [16]. In the context of rainbow spanning configurations, the emergence of rainbow Hamilton cycles in uniformly colored randomly perturbed graphs was studied by Anastos and Frieze [4] as well as by the first two authors [1].…”
Section: Introductionmentioning
confidence: 99%
“…At this point, one may consider an auxiliary path which visits every cell once and construct a Hamilton cycle by traversing the cells twice following the path (forwards and then backwards), incorporating the vertices into the cycle while doing so. Technical variations of this idea have been used to obtain many results about Hamilton cycles in random geometric graphs [4,5,18,19,20,23,26,37,40,48].…”
Section: B ( ) Hmentioning
confidence: 99%
“…Therefore, when considering this problem, we must really consider all possible values of . Second, all known results about Hamiltonicity in ( , ) exploit the fact that these graphs are locally dense, meaning that vertices which are (geometrically) close form very large cliques [4,5,18,19,20,23,26,37,40,48]. This is not the case in the local resilience setting, where the adversary may delete all cliques.…”
mentioning
confidence: 99%