Physics – Condensed Matter – Disordered Systems and Neural Networks
Scientific paper
2009-01-28
Physics
Condensed Matter
Disordered Systems and Neural Networks
10 pages 5 figures; corrected metadata only
Scientific paper
We introduce a model for dynamic networks, where the links or the strengths of the links change over time. We solve the model by mapping dynamic networks to the problem of directed percolation, where the direction corresponds to the evolution of the network in time. We show that the dynamic network undergoes a percolation phase transition at a critical concentration $p_c$, which decreases with the rate $r$ at which the network links are changed. The behavior near criticality is universal and independent of $r$. We find fundamental network laws are changed. (i) For Erd\H{o}s-R\'{e}nyi networks we find that the size of the giant component at criticality scales with the network size $N$ for all values of $r$, rather than as $N^{2/3}$. (ii) In the presence of a broad distribution of disorder, the optimal path length between two nodes in a dynamic network scales as $N^{1/2}$, compared to $N^{1/3}$ in a static network.
Cohen Reuven
Dickison Mark
Havlin Shlomo
Parshani Roni
Stanley Eugene H.
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