SPEEDING UP NON-MARKOVIAN FIRST-PASSAGE PERCOLATION WITH A FEW EXTRA EDGES

被引:1
作者
Medvedev, Alexey [1 ,2 ]
Pete, Gabor [3 ,4 ]
机构
[1] Univ Namur, Namur Inst Complex Networks naXys, Rempart Vierge 8, B-5000 Namur, Belgium
[2] Catholic Univ Louvain, Louvain La Neuve, Belgium
[3] Alfred Renyi Inst Math, Realtanoda U 13-15, H-1053 Budapest, Hungary
[4] Budapest Univ Technol & Econ, Budapest, Hungary
基金
欧洲研究理事会;
关键词
Temporal network; near-critical random graph; Galton-Watson tree; Erdos-Renyi graph; Polya urn process; spreading phenomena; SI model; first-passage percolation; bursty time series; non-Markovian process; 1ST PASSAGE PERCOLATION; CRITICAL RANDOM GRAPHS; TREES;
D O I
10.1017/apr.2018.39
中图分类号
O21 [概率论与数理统计]; C8 [统计学];
学科分类号
020208 ; 070103 ; 0714 ;
摘要
One model of real-life spreading processes is that of first-passage percolation (also called the SI model) on random graphs. Social interactions often follow bursty patterns, which are usually modelled with independent and identically distributed heavy-tailed passage times on edges. On the other hand, random graphs are often locally tree-like, and spreading on trees with leaves might be very slow due to bottleneck edges with huge passage times. Here we consider the SI model with passage times following a power-law distribution P(xi > t) similar to t(-alpha) with infinite mean. For any finite connected graph G with a root s, we find the largest number of vertices kappa(G , s) that are infected in finite expected time, and prove that for every k <= kappa (G, s), the expected time to infect k vertices is at most O(k(1/alpha)). Then we show that adding a single edge from s to a random vertex in a random tree T typically increases kappa(T , s) from a bounded variable to a fraction of the size of T, thus severely accelerating the process. We examine this acceleration effect on some natural models of random graphs: critical Galton-Watson trees conditioned to be large, uniform spanning trees of the complete graph, and on the largest cluster of near-critical Erdos-Renyi graphs. In particular, at the upper end of the critical window, the process is already much faster than exactly at criticality.
引用
收藏
页码:858 / 886
页数:29
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