Connecting the Random Connection Model

preprint2015arXivOpen access

Abstract

Consider the random graph G(Pn,r)G({\mathcal P}_{n},r) whose vertex set Pn{\mathcal P}_{n} is a Poisson point process of intensity nn on (−12,12]d(- \frac{1}{2}, \frac{1}{2}]^d, d≥2d \geq 2. Any two vertices Xi,Xj∈PnX_i,X_j \in {\mathcal P}_{n} are connected by an edge with probability g(d(Xi,Xj)r)g\left( \frac{d(X_i,X_j)}{r} \right), independently of all other edges, and independent of the other points of Pn{\mathcal P}_{n}. dd is the toroidal metric, r>0r > 0 and g:[0,∞)→[0,1]g:[0,\infty) \to [0,1] is non-increasing and α=∫Rdg(∣x∣)dx<∞α= \int_{\mathbb{R}^d} g(|x|) dx < \infty. Under suitable conditions on gg, almost surely, the critical parameter dnd_n for which G(Pn,⋅)G({\mathcal P}_{n}, \cdot) does not have any isolated nodes satisfies lim⁡n→∞αndndlog⁡n=1\lim_{n \to \infty} \frac{αn d_n^d}{\log n} = 1. Let β=inf⁡{x>0:xg(αxθ)>1}β= \inf\{x > 0: x g\left( \fracα{x θ} \right) > 1 \}, and θθ be the volume of the unit ball in Rd\mathbb{R}^d. Then for all γ>βγ> β, G(Pn,(γlog⁡nαn)1d)G\left({\mathcal P}_{n}, \left( \frac{γ\log n}{αn} \right)^{\frac{1}{d}}\right) is connected with probability approaching one as n→∞n \to \infty. The bound can be seen to be tight for the usual random geometric graph obtained by setting g=1[0,1]g = 1_{[0,1]}. We also prove some useful results on the asymptotic behaviour of the length of the edges and the degree distribution in the {\it connectivity regime}.

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