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Stochastic homogenization and effective Hamiltonians of HJ equations in one space dimension: The double-well case

Analysis of PDEs · Submitted 15 Jul 2020

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Under the extra condition that $G$ is a double-well function (i.e., it has precisely two local minima), we give a new and fully constructive proof of homogenization which yields a formula for the effective Hamiltonian $\overline H$.

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arXiv ID2007.07854 (version 1)
Pith IDUV56Q2JG, Pith's permanent record of this paper and its review
CitationAtilla Yilmaz. "Stochastic homogenization and effective Hamiltonians of HJ equations in one space dimension: The double-well case." arXiv:2007.07854 (2020). https://pith.science/paper/UV56Q2JG
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Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,542 input tokens.

What the abstract itself states, as probabilities: claims first 0.08 · states limitation 0.47 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.20 · compares with prior results 0.91 · mentions code or data availability 0.02.

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arXiv listing abstract v1. Results and the main claim are underlined; .

We consider Hamilton-Jacobi equations in one space dimension with Hamiltonians of the form $H(p,x,\omega) = G(p) + \beta V(x,\omega)$, where $V(\cdot,\omega)$ is a stationary and ergodic potential of unit amplitude. The homogenization of such equations is established in a 2016 paper of Armstrong, Tran and Yu for all continuous and coercive $G$. Under the extra condition that $G$ is a double-well function (i.e., it has precisely two local minima), we give a new and fully constructive proof of homogenization which yields a formula for the effective Hamiltonian $\overline H$. We use this formula to provide a complete list of the heights at which the graph of $\overline H$ has a flat piece. We illustrate our results by analyzing basic classes of examples, highlight some corollaries that clarify the dependence of $\overline H$ on $G$, $\beta$ and the law of $V(\cdot,\omega)$, and discuss a generalization to even-symmetric triple-well Hamiltonians.

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 We consider Hamilton-Jacobi equations in one space dimension with Hamiltonians of the form $H(p,x,\omega) = G(p) + \beta V(x,\omega)$, where $V(\cdot,\omega)$ is a stationary and ergodic potential of unit amplitude. background 0.95 0.30 0.03 asserted 0.89
s1 The homogenization of such equations is established in a 2016 paper of Armstrong, Tran and Yu for all continuous and coercive $G$. background 1.00 0.03 0.05 asserted 1.00
s2 Under the extra condition that $G$ is a double-well function (i.e., it has precisely two local minima), we give a new and fully constructive proof of homogenization which yields a formula for the effective Hamiltonian $\overline H$. contribution 0.99 0.96 0.76 asserted 1.00
s3 We use this formula to provide a complete list of the heights at which the graph of $\overline H$ has a flat piece. result 0.86 0.95 0.22 asserted 1.00
s4 We illustrate our results by analyzing basic classes of examples, highlight some corollaries that clarify the dependence of $\overline H$ on $G$, $\beta$ and the law of $V(\cdot,\omega)$, and discuss a generalization to even-symmetric triple-well Hamiltonians. contribution 0.92 0.93 0.09 asserted 0.99

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Original abstract

We consider Hamilton-Jacobi equations in one space dimension with Hamiltonians of the form $H(p,x,\omega) = G(p) + \beta V(x,\omega)$, where $V(\cdot,\omega)$ is a stationary and ergodic potential of unit amplitude. The homogenization of such equations is established in a 2016 paper of Armstrong, Tran and Yu for all continuous and coercive $G$. Under the extra condition that $G$ is a double-well function (i.e., it has precisely two local minima), we give a new and fully constructive proof of homogenization which yields a formula for the effective Hamiltonian $\overline H$. We use this formula to provide a complete list of the heights at which the graph of $\overline H$ has a flat piece. We illustrate our results by analyzing basic classes of examples, highlight some corollaries that clarify the dependence of $\overline H$ on $G$, $\beta$ and the law of $V(\cdot,\omega)$, and discuss a generalization to even-symmetric triple-well Hamiltonians.

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  • When $H$ is not assumed to be convex (non-convex case), only very specific frameworks were treated: for level-set convex Hamiltonians [ref] , when the law of $H$ is invariant by rotation [ref] , in one-dimension [ref] , when the law of $H$ satisfies a finite range condition and $H$ is positively homogenous or star-shaped [ref] .

    Percolation games · Stochastic homogenization · 0.91

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