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Contact process (mathematics) : ウィキペディア英語版
Contact process (mathematics)

The contact process is a model of an interacting particle system. It is a continuous time Markov process with state space \^S, where S is a finite or countable graph, usually Z{}^d. The process is usually interpreted as a model for the spread of an infection: if the state of the process at a given time is \eta, then a site x in S is "infected" if \eta(x)=1 and healthy if \eta(x)=0. Infected sites become healthy at a constant rate, while healthy sites become infected at a rate proportional to the number infected neighbors. One can generalize the state space to \{0,\ldots, \kappa\}^S, such is called the multitype contact process. It represents a model when more than one type of infection is competing for space.
==Dynamics==

More specifically, the dynamics of the basic contact process is defined by the following transition rates: at site x,
:1\rightarrow0\quad\mbox1,
:0\rightarrow1\quad\mbox\lambda\sum_\eta(y),
where the sum is over all the neighbors in S of x. This means that each site waits an exponential time with the corresponding rate, and then flips (so 0 becomes 1 and vice versa).
For each graph S there exists a critical value \lambda_c for the parameter \lambda so that if \lambda>\lambda_c then the 1's survive (that is, if there is at least one 1 at time zero, then at any time there are ones) with positive probability, while if \lambda<\lambda_c then the process dies out. For contact process on the integer lattice, a major breakthrough came in 1990 when Bezuidenhout and Grimmett showed that the contact process also dies out at the critical value. Their proof makes use of eded|date=June 2012}} came in 1990 when Bezuidenhout and Grimmett showed that the contact process also dies out at the critical value. Their proof makes use of percolation theory.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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