Math 2.0

Probability theory and stochastic processes Special processes Example

Voter model

Example

Let d≥1d \ge 1. The voter model on ℤd\Z^d is the spin system on {0,1}ℤd\set{0, 1}^{\Z^d} with flip rates c(x,η)=12d #{y∈ℤd:∣y−x∣=1, η(y)≠η(x)}.c(x, \eta) = \frac{1}{2d} \, \#\set{y \in \Z^d : \abs{y - x} = 1, \ \eta(y) \ne \eta(x)}. Here η(x)\eta(x) is the opinion of the voter at site xx. At rate 11, each voter picks one of its 2d2d neighbours uniformly at random and adopts that neighbour's opinion. The rates lie in [0,1][0, 1] and depend on 2d+12d + 1 sites, so it is an interacting particle system.

Remarks

The two constant configurations, all 00 and all 11, are absorbing. The model is dual to a system of coalescing random walks. Tracing back whose opinion a voter holds gives a random walk path, and two such paths merge when they meet. Because of this duality, the long-time behaviour depends on whether simple random walk on ℤd\Z^d is recurrent, which by Pólya's recurrence theorem holds exactly for d≤2d \le 2. Started from independent opinions with density ρ∈(0,1)\rho \in (0, 1), for d≤2d \le 2 any two sites tend to agree, P(ηt(x)≠ηt(y))→0P(\eta_t(x) \ne \eta_t(y)) \to 0 as t→∞t \to \infty. For d≥3d \ge 3 there is a one-parameter family of invariant measures in which both opinions keep a positive density.

Further reading

  1. Web https://en.wikipedia.org/wiki/Voter_model
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MSC60K35, 82C22
Instance ofInteracting particle system
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Changed2 November 2026

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