Stochastic homogenization for variational solutions of Hamilton-Jacobi equations
Claude Viterbo
TL;DR
This work develops a stochastic homogenization framework for variational solutions of Hamilton–Jacobi equations with random Hamiltonians $H(x,p;oldsymbol{ ext ω})$ under an ergodic ${oldsymbol{ ext R}}^n$-action. Using generating functions, spectral invariants, and a $oldsymbol{ ext γ}_c$-topology on non-compact cotangent bundles, the authors establish almost-sure convergence of $u^oldsymbol{ ext ε}$ to a homogenized equation with effective Hamiltonian $oldsymbol{ar H}$, without requiring convexity in $p$. The proof combines non-compact, almost periodic, and coercive regimes through regularization to finite-dimensional tori, ergodic arguments, and a detailed comparison of Hamiltonian flows with their variational solutions. The results unify stochastic and variational approaches, extend viscosity-based homogenization in the convex case, and apply to both non-compact and discrete settings, with extensions to time-dependent and partially homogenized scenarios. Altogether, the paper provides a rigorous pathway from random Hamiltonians to deterministic effective dynamics in a broad, non-convex, variational context.
Abstract
Let $(Ω, μ)$ be a probability space endowed with an ergodic action, $τ$ of $( {\mathbb R} ^n, +)$. Let $H(x,p; ω)=H_ω(x,p)$ be a smooth Hamiltonian on $T^* {\mathbb R} ^n$ parametrized by $ω\in Ω$ and such that $ H(a+x,p;τ_aω)=H(x,p;ω)$. We consider for an initial condition $f\in C^0 ( {\mathbb R}^n)$, the family of variational solutions of the stochastic Hamilton-Jacobi equations $$\left\{ \begin{aligned} \frac{\partial u^{ \varepsilon }}{\partial t}(t,x;ω)+H\left (\frac{x}{ \varepsilon } , \frac{\partial u^\varepsilon }{\partial x}(t,x;ω);ω\right )=0 &\\ u^\varepsilon (0,x;ω)=f(x)& \end{aligned} \right .$$ Under some coercivity assumptions on $p$ -- but without any convexity assumption -- we prove that for a.e. $ω\in Ω$ we have $C^0-\lim u^{\varepsilon}(t,x;ω)=v(t,x)$ where $v$ is the variational solution of the homogenized equation $$\left\{ \begin{aligned} \frac{\partial v}{\partial t}(x)+{\overline H}\left (\frac{\partial v }{\partial x}(x) \right )=0 &\\ v (0,x)=f(x)& \end{aligned} \right.$$
