English

Strong diffusion approximation in averaging with dynamical systems fast motion

Probability 2022-04-26 v3 Dynamical Systems

Abstract

The paper deals with the fast-slow motions setups in the continuous time dX(t)dt=1εB(Xε(t),ξ(t/ε2))+b(Xε(t),ξ(t/ε2)),t[0,T]\frac {dX^(t)}{dt}=\frac 1\varepsilon B(X^\varepsilon(t),\xi(t/\varepsilon^2))+b(X^\varepsilon(t),\,\xi(t/\varepsilon^2)),\, t\in [0,T] and the discrete time Xε((n+1)ε2)=Xε(nε2)+εB(Xε(nε2),ξ(n))+ε2b(Xε(nε2),ξ(n))X^\varepsilon((n+1)\varepsilon^2)=X^\varepsilon(n\varepsilon^2)+\varepsilon B(X^\varepsilon(n\varepsilon^2),\xi(n)) +\varepsilon^2 b(X^\varepsilon(n\varepsilon^2),\xi(n)), n=0,1,...,[T/ε2]n=0,1,...,[T/\varepsilon^2] where Σ\Sigma and bb are smooth vector functions and ξ\xi is a stationary vector stochastic process such that Eξ(0)=0E\xi(0)=0 for all xRdx\in\mathbb{R}^d. Unlike \cite{Ki20} the assumptions imposed on the process ξ\xi allow applications to a wide class of observables gg in the dynamical systems setup so that ξ\xi can be taken in the form ξ(t)=g(Ftξ(0))\xi(t)=g(F^t\xi(0)) or ξ(n)=g(Fnξ(0))\xi(n)=g(F^n\xi(0)) where FF is either a flow or a diffeomorphism with some hyperbolicity and gg is a vector function. In this paper we show that both XεX^\varepsilon and a family of diffusions Ξε\Xi^\varepsilon can be redefined on a common sufficiently rich probability space so that Esup0tTXε(t)Ξε(t)pCεδ,p1E\sup_{0\leq t\leq T}|X^\varepsilon(t)-\Xi^\varepsilon(t)|^{p}\leq C\varepsilon^\delta,\, p\geq 1 for some C,δ>0C,\delta>0 and all ε>0\varepsilon>0, where all Ξε,ε>0\Xi^\varepsilon,\, \varepsilon>0 have the same diffusion coefficients but underlying Brownian motions may change with ε\varepsilon.

Keywords

Cite

@article{arxiv.2105.01940,
  title  = {Strong diffusion approximation in averaging with dynamical systems fast motion},
  author = {Yuri Kifer},
  journal= {arXiv preprint arXiv:2105.01940},
  year   = {2022}
}

Comments

30 pages. arXiv admin note: text overlap with arXiv:2011.07907

R2 v1 2026-06-24T01:47:41.753Z