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Takeover times for a simple model of network infection
We study a stochastic model of infection spreading on a network. At each time step a node is chosen at random, along with one of its neighbors. If the node is infected and the neighbor is susceptible, the neighbor becomes infected. How many time steps [Formula: see text] does it take to completely i...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Physical Society
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7217517/ https://www.ncbi.nlm.nih.gov/pubmed/29347209 http://dx.doi.org/10.1103/PhysRevE.96.012313 |
Sumario: | We study a stochastic model of infection spreading on a network. At each time step a node is chosen at random, along with one of its neighbors. If the node is infected and the neighbor is susceptible, the neighbor becomes infected. How many time steps [Formula: see text] does it take to completely infect a network of [Formula: see text] nodes, starting from a single infected node? An analogy to the classic “coupon collector” problem of probability theory reveals that the takeover time [Formula: see text] is dominated by extremal behavior, either when there are only a few infected nodes near the start of the process or a few susceptible nodes near the end. We show that for [Formula: see text] , the takeover time [Formula: see text] is distributed as a Gumbel distribution for the star graph, as the convolution of two Gumbel distributions for a complete graph and an Erdős-Rényi random graph, as a normal for a one-dimensional ring and a two-dimensional lattice, and as a family of intermediate skewed distributions for [Formula: see text]-dimensional lattices with [Formula: see text] (these distributions approach the convolution of two Gumbel distributions as [Formula: see text] approaches infinity). Connections to evolutionary dynamics, cancer, incubation periods of infectious diseases, first-passage percolation, and other spreading phenomena in biology and physics are discussed. |
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