Anomalous diffusion by fractal homogenization
Scott Armstrong, Vlad Vicol
TL;DR
The authors construct an explicit deterministic, time-space periodic, incompressible vector field with fractal (multi-scale) structure built from alternating shear flows. Using a fractal (renormalization) homogenization framework, they recursively define scale-dependent correctors and renormalized diffusivities, proving that the effective diffusivity becomes order one on the macroscopic scale. This leads to anomalous dissipation of scalar variance: as κ → 0, the dissipation κ∥∇θ^κ∥^2 remains bounded away from zero for mean-zero initial data. The approach provides a rigorous, scale-by-scale mechanism for anomalous diffusion in a deterministic setting and offers a quantitative homogenization methodology applicable to turbulent-like transport problems.
Abstract
For every $α< \frac13$, we construct an explicit divergence-free vector field $\mathbf{b}(t,x)$ which is periodic in space and time and belongs to $C^0_t C^α_x \cap C^α_t C^0_x$ such that the corresponding scalar advection-diffusion equation $$\partial_t θ^κ+ \mathbf{b} \cdot \nabla θ^κ- κΔθ^κ= 0$$ exhibits anomalous dissipation of scalar variance for arbitrary $H^1$ initial data: $$\limsup_{κ\to 0} \int_0^{1} \int_{\mathbb{T}^d} κ\| \nabla θ^κ(t,x) \|^2 \,dx\,dt >0.$$ The vector field is deterministic and has a fractal structure, with periodic shear flows alternating in time between different directions serving as the base fractal. These shear flows are repeatedly inserted at infinitely many scales in suitable Lagrangian coordinates. Using an argument based on ideas from quantitative homogenization, the corresponding advection-diffusion equation with small $κ$ is progressively renormalized, one scale at a time, starting from the (very small) length scale determined by the molecular diffusivity up to the macroscopic (unit) scale. At each renormalization step, the effective diffusivity is enhanced by the influence of advection on that scale. By iterating this procedure across many scales, the effective diffusivity on the macroscopic scale is shown to be of order one.
