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The structure of networks that evolve under a combination of growth, via node addition and random attachment, and contraction, via random node deletion (2209.10027v2)

Published 20 Sep 2022 in cond-mat.stat-mech and cond-mat.dis-nn

Abstract: We present analytical results for the emerging structure of networks that evolve via a combination of growth (by node addition and random attachment) and contraction (by random node deletion). To this end we consider a network model in which at each time step a node addition and random attachment step takes place with probability $P_{add}$ and a random node deletion step takes place with probability $P_{del}=1-P_{add}$. The balance between the growth and contraction processes is captured by the parameter $\eta=P_{add}-P_{del}$. The case of pure network growth is described by $\eta=1$. In case that $0<\eta<1$ the rate of node addition exceeds the rate of node deletion and the overall process is of network growth. In the opposite case, where $-1<\eta<0$, the overall process is of network contraction, while in the special case of $\eta=0$ the expected size of the network remains fixed, apart from fluctuations. Using the master equation we obtain a closed form expression for the time dependent degree distribution $P_t(k)$. The degree distribution $P_t(k)$ includes a term that depends on the initial degree distribution $P_0(k)$, which decays as time evolves, and an asymptotic distribution $P_{st}(k)$. In the case of pure network growth ($\eta=1$) the asymptotic distribution $P_{st}(k)$ follows an exponential distribution, while for $-1<\eta<1$ it consists of a sum of Poisson-like terms and exhibits a Poisson-like tail. In the case of overall network growth ($0 < \eta < 1$) the degree distribution $P_t(k)$ eventually converges to $P_{st}(k)$. In the case of overall network contraction ($-1 < \eta < 0$) we identify two different regimes. For $-1/3 < \eta < 0$ the degree distribution $P_t(k)$ quickly converges towards $P_{st}(k)$. In contrast, for $-1 < \eta < -1/3$ the convergence of $P_t(k)$ is initially very slow and it gets closer to $P_{st}(k)$ only shortly before the network vanishes.

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