TheoremBase

Viscosity Sub- and Supersolutions on the Torus Wasserstein Space are Entropy-Penalised Viscosity Sub- and Supersolutions

If the Hamiltonian is continuous along couplings and satisfies the score-perturbation bound, every upper semicontinuous viscosity subsolution is an entropy-penalised viscosity subsolution, and likewise for lower semicontinuous supersolutions. The proof regularises the test function and the entropy with the heat semigroup.

Statement

In the setting of The Discounted Hamilton-Jacobi-Bellman Equation with Idiosyncratic Noise on the Torus Wasserstein Space: Standing Notation, consider the equation (E)(\mathrm{E}) of The Discounted Hamilton-Jacobi-Bellman Equation with Idiosyncratic Noise on the Torus Wasserstein Space §laplacian-form, and assume that the Hamiltonian HH is continuous along couplings and satisfies the score-perturbation bound. Semicontinuity refers to the metric space (P(Td),WT)(\mathcal{P}(\mathbb{T}^{d}),W_{\mathbb{T}}).

1. (Subsolutions) Every upper semicontinuous viscosity subsolution of (E)(\mathrm{E}) is an entropy-penalised viscosity subsolution of (E)(\mathrm{E}).

2. (Supersolutions) Every lower semicontinuous viscosity supersolution of (E)(\mathrm{E}) is an entropy-penalised viscosity supersolution of (E)(\mathrm{E}).

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