2010
DOI: 10.1239/aap/1269611141
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Sentry Selection in Wireless Networks

Abstract: Let P be a Poisson process of intensity one in the infinite plane R 2 . We surround each point x of P by the open disc of radius r centred at x. Now let S n be a fixed disc of area n, and let C r (S n ) be the set of discs which intersect S n . Write E k r for the event that C r (S n ) is a k-cover of S n , and F k r for the event that C r (S n ) may be partitioned into k disjoint single covers of S n . We prove thatlog n , and that this result is best possible. We also give improved estimates for P(E k r ). F… Show more

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Cited by 10 publications
(10 citation statements)
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“…The proof of Theorem 2, which is rather complicated, is given in [5]. The same paper also contains a short proof of Theorem 1.…”
Section: Theoretical Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…The proof of Theorem 2, which is rather complicated, is given in [5]. The same paper also contains a short proof of Theorem 1.…”
Section: Theoretical Resultsmentioning
confidence: 99%
“…These facts point us towards the investigation of non-2-partitionable 2-covers with half-planes. In [5], the following theorem is proved. C 3 s and C 5 s are the configurations which occur with probability Θ(1/ log n) and make Theorem 2 best possible for k = 2.…”
Section: Obstructions To Partitionabilitymentioning
confidence: 99%
“…If the distance of i from pq is c i /t then the heights of D p and D q above m 0 are asymptotically t 3 Figure 1) is entirely contained in R ∪ R . Therefore, s will not be covered by A λ , since, by construction, V ⊂ R ∪ R is free of black points; all black discs will be stopped by p, q, r, or another red point before they cover s .…”
Section: Good Configurationsmentioning
confidence: 99%
“…For instance, writing πr 2 = log n + log log n + t, Svante Janson proved in 1986 [7] that as n → ∞, coverage occurs with probability asymptotically exp(−e −t ). One approach to this result [2], [3] uses the fact that the obstructions to coverage are small uncovered regions, which essentially form their own Poisson process, of intensity e −t /n. Although these uncovered regions may be of different shapes, they are all roughly the same size.…”
Section: Introductionmentioning
confidence: 99%
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