Stochastic homogenization for variationalsolutions of Hamilton–Jacobi equations

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 $$\left\{ \begin{aligned} \frac{\partial v}{\partial t}(x)+{\overline H}\left (\frac{\partial v }{\partial x}(x) \right )=0 &\\ v (0,x)=f(x)& \end{aligned} \right.$$

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Publication Details

Journal
Analysis & PDE
Published
2025-03-27
DOI
https://doi.org/10.2140/apde.2025.18.805
Citations
1
Primary Topic
Geometric Analysis and Curvature Flows
Type
article
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article

Stochastic homogenization for variationalsolutions of Hamilton–Jacobi equations

Claude Viterbo
1 citations
Analysis & PDE
Geometric Analysis and Curvature Flows
article

Stochastic homogenization for variationalsolutions of Hamilton–Jacobi equations

Claude Viterbo
article en
1 citations

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 $$\left\{ \begin{aligned} \frac{\partial v}{\partial t}(x)+{\overline H}\left (\frac{\partial v }{\partial x}(x) \right )=0 &\\ v (0,x)=f(x)& \end{aligned} \right.$$

Analysis & PDEVol. 18(4)
Centre National de la Recherche Scientifique (FR), Université Paris Sciences et Lettres (FR), Université Paris-Saclay (FR), École Normale Supérieure - PSL (FR), Laboratoire de Mathématiques d'Orsay (FR), Département de mathématiques et applications (FR)
Openalex Percentile: Top 100%
Geometric Analysis and Curvature Flows
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