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December 2010 Diffusion limit for many particles in a periodic stochastic acceleration field
Yves Elskens, Etienne Pardoux
Ann. Appl. Probab. 20(6): 2022-2039 (December 2010). DOI: 10.1214/09-AAP671

Abstract

The one-dimensional motion of any number ${\mathcal{N}}$ of particles in the field of many independent waves (with strong spatial correlation) is formulated as a second-order system of stochastic differential equations, driven by two Wiener processes. In the limit of vanishing particle mass ${\mathfrak{m}}\to0$, or, equivalently, of large noise intensity, we show that the momenta of all ${\mathcal{N}}$ particles converge weakly to ${\mathcal{N}}$ independent Brownian motions, and this convergence holds even if the noise is periodic. This justifies the usual application of the diffusion equation to a family of particles in a unique stochastic force field. The proof rests on the ergodic properties of the relative velocity of two particles in the scaling limit.

Citation

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Yves Elskens. Etienne Pardoux. "Diffusion limit for many particles in a periodic stochastic acceleration field." Ann. Appl. Probab. 20 (6) 2022 - 2039, December 2010. https://doi.org/10.1214/09-AAP671

Information

Published: December 2010
First available in Project Euclid: 19 October 2010

zbMATH: 1215.82048
MathSciNet: MR2759727
Digital Object Identifier: 10.1214/09-AAP671

Subjects:
Primary: 34F05 , 60H10 , 82C05 , 82D10
Secondary: 60J70 , 60K40

Keywords: Fokker–Planck equation , Hamiltonian chaos , propagation of chaos , Quasilinear diffusion , stochastic acceleration , wave-particle interaction , weak plasma turbulence

Rights: Copyright © 2010 Institute of Mathematical Statistics

Vol.20 • No. 6 • December 2010
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