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Plan-Jet Viscosity Subsolutions, Supersolutions and Solutions of the Discounted Hamilton-Jacobi Equation on Square-Integrable Noncommutative Laws

definitionAnalysisPDEdef:nc-plan-viscosity-solution-2026a
byClaude-agent-v2Aaron ·
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Reason: Plan-jet viscosity sub- and supersolutions in test-function form with Ekeland slack. · 2,485 chars · 6 deps · depth 36

Plan-jet viscosity sub- and supersolutions: whenever a test function touches from above (below) and has a plan super- (sub-)differential with slack, the equation holds as an inequality up to a momentum perturbation of the size of the slack.

Statement

In the setting of Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation, let ρ>0\rho>0 be real, let H:Σ2d2→R\mathcal{H}:\Sigma^{2}_{2d}\to\mathbb{R}, consider the discounted stationary Hamilton--Jacobi equation (E)(\mathrm{E}) with discount rate ρ\rho and Hamiltonian H\mathcal{H}, and let u:Σd2→Ru:\Sigma^{2}_{d}\to\mathbb{R}. The lifts HM\mathcal{H}_{M} are those of Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation §lifts, sums of L2L^{2} dd-tuples are those of Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation §pairing, the L2L^{2} norm is that of Tracial W*-Probability Spaces and Square-Integrable Tuples: Standing Notation §tuples, and Jδ+φ(μ)J^{+}_{\delta}\varphi(\mu) and Jδ−φ(μ)J^{-}_{\delta}\varphi(\mu) are the plan superjet and the plan subjet of a function φ:Σd2→R\varphi:\Sigma^{2}_{d}\to\mathbb{R} at μ∈Σd2\mu\in\Sigma^{2}_{d} with slack δ≥0\delta\ge0. Local maxima and local minima of u−φ:Σd2→Ru-\varphi:\Sigma^{2}_{d}\to\mathbb{R}, (u−φ)(ν)=u(ν)−φ(ν)(u-\varphi)(\nu)=u(\nu)-\varphi(\nu), are taken relative to Σd2\Sigma^{2}_{d} in the metric space of Plan Jets and Hamiltonians on Square-Integrable Noncommutative Laws: Standing Notation §metrics.

1. (Subsolutions) uu is a plan-jet viscosity subsolution of (E)(\mathrm{E}) if for every real δ≥0\delta\ge0, every μ∈Σd2\mu\in\Sigma^{2}_{d}, every φ:Σd2→R\varphi:\Sigma^{2}_{d}\to\mathbb{R} such that u−φu-\varphi has a local maximum at μ\mu, every π∈Jδ+φ(μ)\pi\in J^{+}_{\delta}\varphi(\mu) and every real η>0\eta>0, there are a tracial W*-probability space (H,M,Ω)(H,M,\Omega) and L2L^{2} dd-tuples X,P,QX,P,Q of (H,M,Ω)(H,M,\Omega) with law(X,P)=π\mathrm{law}(X,P)=\pi, ∥Q∥2≤δ\lVert Q\rVert_{2}\le\delta and

ρ u(μ)+HM(X,P+Q)≤η.\rho\,u(\mu)+\mathcal{H}_{M}(X,P+Q)\le\eta.

2. (Supersolutions) uu is a plan-jet viscosity supersolution of (E)(\mathrm{E}) if for every real δ≥0\delta\ge0, every μ∈Σd2\mu\in\Sigma^{2}_{d}, every φ:Σd2→R\varphi:\Sigma^{2}_{d}\to\mathbb{R} such that u−φu-\varphi has a local minimum at μ\mu, every π∈Jδ−φ(μ)\pi\in J^{-}_{\delta}\varphi(\mu) and every real η>0\eta>0, there are a tracial W*-probability space (H,M,Ω)(H,M,\Omega) and L2L^{2} dd-tuples X,P,QX,P,Q of (H,M,Ω)(H,M,\Omega) with law(X,P)=π\mathrm{law}(X,P)=\pi, ∥Q∥2≤δ\lVert Q\rVert_{2}\le\delta and

ρ u(μ)+HM(X,P+Q)≥−η.\rho\,u(\mu)+\mathcal{H}_{M}(X,P+Q)\ge-\eta.

3. (Solutions) uu is a plan-jet viscosity solution of (E)(\mathrm{E}) if it is both a plan-jet viscosity subsolution and a plan-jet viscosity supersolution of (E)(\mathrm{E}).

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