On the sector condition and homogenization of diffusions with a Gaussian drift (original) (raw)

Infinite interacting diffusion particles I: Equilibrium process and its scaling limit

Forum Mathematicum, 2000

A stochastic dynamics (X(t)) t≥0 of a classical continuous system is a stochastic process which takes values in the space Γ of all locally finite subsets (configurations) in R d and which has a Gibbs measure µ as an invariant measure. We assume that µ corresponds to a symmetric pair potential φ(x − y). An important class of stochastic dynamics of a classical continuous system is formed by diffusions. Till now, only one type of such dynamics-the so-called gradient stochastic dynamics, or interacting Brownian particles-has been investigated. By using the theory of Dirichlet forms from [27], we construct and investigate a new type of stochastic dynamics, which we call infinite interacting diffusion particles. We introduce a Dirichlet form E Γ µ on L 2 (Γ; µ), and under general conditions on the potential φ, prove its closability. For a potential φ having a "weak" singularity at zero, we also write down an explicit form of the generator of E Γ µ on the set of smooth cylinder functions. We then show that, for any Dirichlet form E Γ µ , there exists a diffusion process that is properly associated with it. Finally, in a way parallel to [17], we study a scaling limit of interacting diffusions in terms of convergence of the corresponding Dirichlet forms, and we also show that these scaled processes are tight in C([0, ∞), D ′ ), where D ′ is the dual space of D:=C ∞ 0 (R d ).

On homogenization of time-dependent random flows

Probability Theory and Related Fields, 2001

We study a diffusion with a random, time dependent drift. We prove the invariance principle when the spectral measure of the drift satisfies a certain integrability condition. This result generalizes the results of [13, 7]. ‫ޒ‬ d V(t, x; ω) • ∇ x ϕ(x) dx = 0 P − a.s., with P the underlying probability measure. In order to guarantee the existence of the solution of (1.1) we will also assume that V(t, x; ω) is (P −a.s.) locally Lipschitz in x. We are interested in proving an invariance principle for x(t), i.e. the convergence in distribution of the process εx(ε −2 t) to a Brownian motion with a certain co-variance matrix, sometimes referred to as the effective diffusivity, D ≥ 2I. This problem has been widely studied under various conditions on the random flow. Typically the flow is assumed to be the divergence of a stationary random anti-symmetric matrix valued field H(t, x; ω) = {H p,q (t, x; ω)}-the so-called stream matrix: V(t, x; ω) = ∇ x • H(t, x; ω) .

Comparison of interacting diffusions and an application to their ergodic theory

Probability Theory and Related Fields, 1996

A general comparison argument for expectations of certain multitime functionals of infinite systems of linearly interacting diffusions differing in the diffusion coefficient is derived. As an application we prove clustering occurs in the case when the symmetrized interaction kernel is recurrent, and the components take values in an interval bounded on one side. The technique also gives an alternative proof of clustering in the case of compact intervals. Classification (1991): 60K35, 60J60, 60J15 is one-sided bounded. We show that clustering is universal in the diffusion coefficient. This had been conjectured in Cox, Greven and Shiga [CGS95a] (see also Shiga [Shi92]). On the way, we obtain a new proof, in the case where the state space of a component is compact, based on the interacting Fisher-Wright diffusion where a well-known duality is available.

Steady states, fluctuation-dissipation theorems and homogenization for diffusions in a random environment with finite range of dependence

2016

Prolongating our previous paper on the Einstein relation, we study the motion of a particle diffusing in a random reversible environment when subject to a small external forcing. In order to describe the long time behavior of the particle, we introduce the notions of steady state and weak steady state. We establish the continuity of weak steady states for an ergodic and uniformly elliptic environment. When the environment has finite range of dependence, we prove the existence of the steady state and weak steady state and compute its derivative at a vanishing force. Thus we obtain a complete "Fluctuation- Dissipation Theorem" in this context as well as the continuity of the effective variance.

Diffusive and Super-Diffusive Limits for Random Walks and Diffusions with Long Memory

Proceedings of the International Congress of Mathematicians (ICM 2018), 2019

We survey recent results of normal and anomalous diffusion of two types of random motions with long memory in BbbRd{\Bbb R}^dBbbRd or BbbZd{\Bbb Z}^dBbbZd. The first class consists of random walks on BbbZd{\Bbb Z}^dBbbZd in divergence-free random drift field, modelling the motion of a particle suspended in time-stationary incompressible turbulent flow. The second class consists of self-repelling random diffusions, where the diffusing particle is pushed by the negative gradient of its own occupation time measure towards regions less visited in the past. We establish normal diffusion (with square-root-of-time scaling and Gaussian limiting distribution) in three and more dimensions and typically anomalously fast diffusion in low dimensions (typically, one and two). Results are quoted from various papers published between 2012-2018, with some hints to the main ideas of the proofs. No technical details are presented here.

Measure-Valued Diffusions and Continual Systems of Interacting Particles in a Random Medium

Ukrainian Mathematical Journal, 2005

UDC 519.21 We consider continual systems of stochastic equations describing the motion of a family of interacting particles whose mass can vary in time in a random medium. It is assumed that the motion of every particle depends not only on its location at given time but also on the distribution of the total mass of particles. We prove a theorem on unique existence, continuous dependence on the distribution of the initial mass, and the Markov property. Moreover, under certain technical conditions, one can obtain the measure-valued diffusions introduced by Skorokhod as the distributions of the mass of such systems of particles.

Steady States, Fluctuation–Dissipation Theorems and Homogenization for Reversible Diffusions in a Random Environment

Archive for Rational Mechanics and Analysis

Prolongating our previous paper on the Einstein relation, we study the motion of a particle diffusing in a random reversible environment when subject to a small external forcing. In order to describe the long time behavior of the particle, we introduce the notions of steady state and weak steady state. We establish the continuity of weak steady states for an ergodic and uniformly elliptic environment. When the environment has finite range of dependence, we prove the existence of the steady state and weak steady state and compute its derivative at a vanishing force. Thus we obtain a complete 'Fluctuation-Dissipation Theorem' in this context as well as the continuity of the effective variance.

A note on the asymptotic variance of drift accelerated diffusions

Statistics & Probability Letters

We prove that the asymptotic variance of a drift accelerated diffusion converges to zero uniformly if and only if there are no H 1-elements in the kernel of the drift generating operator. Our proof is based on spectral analysis in the first order Sobolev space of mean zero functions.