Marić's selection principle for the Fleming–Viot random walk

Let pp and qq be the right- and left-jump rates, respectively, with q>pq>p, and let ρN\rho^N be the equilibrium density of the Fleming–Viot process driven by the nearest-neighbor random walk on N{\mathbb N}, absorbed at the origin. Let ν0\nu_0 denote the minimal quasi-stationary distribution of the random walk. Marić's selection principle. As NN tends to infinity, the equilibrium density converges to the minimal quasi-stationary distribution:

ρNν0.\rho^N \to \nu_0.

This conjecture asserts that the Fleming–Viot system selects the minimal quasi-stationary distribution among the infinitely many quasi-stationary distributions of the random walk. Ergodicity of the Fleming–Viot process for q>pq>p is known, while the stated large-particle-number convergence is presented in the source as a conjecture supported by heuristic arguments and simulations.

Sources & referencesView supporting material

Primary source

Nevena Maric, “Fleming-Viot particle system driven by a random walk on N”, arXiv:1405.0094 (2014).

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