Abstract

We continue our study of intermittency for the parabolic Anderson model $\partial u/\partial t = \kappa\Delta u + \xi u$ in a space-time random medium $\xi$, where $\kappa$ is a positive diffusion constant, $\Delta$ is the lattice Laplacian on $\mathbb{Z}^d$, $d \geq 1$, and $\xi$ is a simple symmetric exclusion process on $\mathbb{Z}^d$ in Bernoulli equilibrium. This model describes the evolution of a reactant $u$ under the influence of a catalyst $\xi$. <br /><br /> In Gärtner, den Hollander and Maillard [3] we investigated the behavior of the annealed Lyapunov exponents, i.e., the exponential growth rates as $t\to\infty$ of the successive moments of the solution $u$. This led to an almost complete picture of intermittency as a function of $d$ and $\kappa$. In the present paper we finish our study by focussing on the asymptotics of the Lyaponov exponents as $\kappa\to\infty$ in the critical dimension $d=3$, which was left open in Gärtner, den Hollander and Maillard [3] and which is the most challenging. We show that, interestingly, this asymptotics is characterized not only by a Green term, as in $d\geq 4$, but also by a polaron term. The presence of the latter implies intermittency of all orders above a finite threshold for $\kappa$.

Highlights

  • Introduction and main resultIn this paper we consider the parabolic Anderson model (PAM) on d, d ≥ 1,∂ u = κ∆u + ξu on d × [0, ∞), u∂(t·, 0) = 1 on d, (1.1)where κ is a positive diffusion constant, ∆ is the lattice Laplacian acting on u as ∆u(x, t) =[u( y, t) − u(x, t)] y∈ d y−x =1 (1.2)( · is the Euclidian norm), and ξ =t≥0, ξt = {ξt (x) : x ∈ d }, (1.3)is a space-time random field that drives the evolution

  • Where κ is a positive diffusion constant, ∆ is the lattice Laplacian acting on u as

  • If ξ is given by an infinite particle system dynamics, the solution u of the PAM may be interpreted as the concentration of a diffusing reactant under the influence of a catalyst performing such a dynamics

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Summary

Introduction and main result

Where κ is a positive diffusion constant, ∆ is the lattice Laplacian acting on u as. is a space-time random field that drives the evolution. If ξ is given by an infinite particle system dynamics, the solution u of the PAM may be interpreted as the concentration of a diffusing reactant under the influence of a catalyst performing such a dynamics. In Gärtner, den Hollander and Maillard [3] we studied the PAM for ξ Symmetric Exclusion (SE), and developed an almost complete qualitative picture. We restrict to Simple Symmetric Exclusion (SSE), i.e., (ξt )t≥0 is the Markov dynamics on Ω = {0, 1} 3 (0 = vacancy, 1 = particle) with generator L acting on cylinder functions f : Ω → as. (See Liggett [7], Chapter VIII.) Let η and η denote probability and expectation for ξ given ξ0 = η ∈ Ω. The probability measures νρ, ρ ∈ (0, 1), are the only extremal equilibria of the SSE dynamics.

Lyapunov exponents
Intermittency
Outline
Separation of the Green term and the polaron term
Key objects
Key propositions
Preparatory lemmas
Reduction to the original measure
Rayleigh-Ritz formula
Reduced key propositions
Choice of test function
Freezing
R log EX0 exp
Defreezing
Spectral bound
Reduction to a spectral bound
Two further lemmas
Small-time cut out
Two key propositions
Considering
Full Text
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