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Viscosity Sub- and Supersolutions of the Hamilton-Jacobi-Bellman Equation on Unitary Laws

Viscosity sub- and supersolutions are bounded semicontinuous functions on unitary laws satisfying the equation's inequalities at relative extrema against C1C^1 test functions on the gauge space.

Statement

In the setting of Unitary Laws with Free Unitary Noise: Standing Data, with the conventions of Unitary Laws with Free Unitary Noise: Standing Data §spaces and the test functions F∈C1(Ed)F\in C^{1}(E_{d}), the maps F∘ιdF\circ\iota_{d} and the gradients DFDF of Unitary Laws with Free Unitary Noise: Standing Data §test-functions, let H:Ld×Ed→RH:\mathcal{L}_{d}\times E_{d}\to\mathbb{R} be a map, the Hamiltonian, let ρ,β\rho,\beta be the constants, ff the source and Θ^λ\widehat{\Theta}\lambda the noise direction, and let The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation be the Hamilton–Jacobi–Bellman equation with this Hamiltonian HH. The notions below are relative to HH; we speak of viscosity sub- and supersolutions of The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation with Hamiltonian HH. Upper and lower semicontinuity, local maxima and local minima refer to the metric space (Ld,dL)(\mathcal{L}_{d},d_{\mathcal{L}}), relative to Ld\mathcal{L}_{d}.

1. (Subsolutions) A map u:Ld→Ru:\mathcal{L}_{d}\to\mathbb{R} is a viscosity subsolution of The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation if it is bounded and upper semicontinuous on Ld\mathcal{L}_{d} and, for every F∈C1(Ed)F\in C^{1}(E_{d}) and every λ∈Ld\lambda\in\mathcal{L}_{d} at which u−F∘ιdu-F\circ\iota_{d} has a local maximum relative to Ld\mathcal{L}_{d},

ρ u(λ)+H(λ,DF(ιd(λ)))−β22⟨DF(ιd(λ)),Θ^λ⟩d≤f(λ).\rho\,u(\lambda)+H\bigl(\lambda,DF(\iota_{d}(\lambda))\bigr)-\frac{\beta^{2}}{2}\bigl\langle DF(\iota_{d}(\lambda)),\widehat{\Theta}\lambda\bigr\rangle_{d}\le f(\lambda).

2. (Supersolutions) A map v:Ld→Rv:\mathcal{L}_{d}\to\mathbb{R} is a viscosity supersolution of The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation if it is bounded and lower semicontinuous on Ld\mathcal{L}_{d} and, for every F∈C1(Ed)F\in C^{1}(E_{d}) and every λ∈Ld\lambda\in\mathcal{L}_{d} at which v−F∘ιdv-F\circ\iota_{d} has a local minimum relative to Ld\mathcal{L}_{d},

ρ v(λ)+H(λ,DF(ιd(λ)))−β22⟨DF(ιd(λ)),Θ^λ⟩d≥f(λ).\rho\,v(\lambda)+H\bigl(\lambda,DF(\iota_{d}(\lambda))\bigr)-\frac{\beta^{2}}{2}\bigl\langle DF(\iota_{d}(\lambda)),\widehat{\Theta}\lambda\bigr\rangle_{d}\ge f(\lambda).

3. (Solutions) A viscosity solution of The Discounted Hamilton-Jacobi-Bellman Equation on Unitary Laws with Free Unitary Noise §equation is a map Ld→R\mathcal{L}_{d}\to\mathbb{R} that is both a viscosity subsolution and a viscosity supersolution.

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