This paper studies the intermediate time behaviour of a small random perturbation of a periodic cellular flow. Our main result shows that on time scales shorter than the diffusive time scale, the limiting behaviour of trajectories that start close enough to cell boundaries is a fractional kinetic process: A Brownian motion time changed by the local time of an independent Brownian motion. Our proof uses the Freidlin-Wentzell framework, and the key step is to establish an analogous averaging principle on shorter time scales.As a consequence of our main theorem, we obtain a homogenization result for the associated advection diffusion equation. We show that on intermediate time scales the effective equation is a fractional time PDE that arises in modelling anomalous diffusion.
The effective short time and long time behaviour of tracer particlesThis section contains a brief review of results concerning the effective behaviour of tracer particles on long time scales and short time scales. Its main purpose is to place our results in the broader context of existing literature, and the familiar reader can skip directly to Section 3.
Homogenization: Effective behaviour on long time scalesWell known homogenization results show that on time scales much larger than the diffusive time scale 1/ε, the effective behaviour ofX is that of a Brownian motion with an enhanced diffusion coefficient. Explicitly, consider the rescaled processZ =Z ε,δ , defined bỹwhere for clarity we suppress the dependence ofX andZ on the parameters ε and δ. Freidlin [Fre64] (see also [Oll94, BLP78, PS08]) proved that for fixed ε we havẽ