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Entropy-Penalised Viscosity Subsolutions, Supersolutions and Solutions of the Discounted Hamilton-Jacobi-Bellman Equation on the Torus Wasserstein Space

Sub- and supersolutions tested at strict extrema of the function minus an intrinsic test function and a small multiple of the entropy. The extremal measure must have finite Fisher information, and the score form of the equation must hold there up to a tolerance proportional to the multiple.

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 its score form (Eξ)(\mathrm{E}_{\xi}) of The Discounted Hamilton-Jacobi-Bellman Equation with Idiosyncratic Noise on the Torus Wasserstein Space §score-form, and let u:P(Td)→Ru:\mathcal{P}(\mathbb{T}^{d})\to\mathbb{R}. For an intrinsic test function φ\varphi on Pac(Td)\mathcal{P}^{\mathrm{ac}}(\mathbb{T}^{d}) and μ∈PEnt(Td)\mu\in\mathcal{P}^{\mathrm{Ent}}(\mathbb{T}^{d}) the gradient ∇φ(μ)\nabla\varphi(\mu) is defined, μ\mu being absolutely continuous by The Entropy of Measures on the Torus: Nonnegativity, Absolute Continuity and Closed Sublevel Sets §nonnegative.

1. (Subsolution) uu is an entropy-penalised viscosity subsolution of (E)(\mathrm{E}) if there are a real number δ0>0\delta_{0}>0 and a nondecreasing function c:[0,∞)→[0,∞)c:[0,\infty)\to[0,\infty) with the following property. For every intrinsic test function φ\varphi on Pac(Td)\mathcal{P}^{\mathrm{ac}}(\mathbb{T}^{d}), every real δ\delta with 0<δ≤δ00<\delta\le\delta_{0}, and every μ∈PEnt(Td)\mu\in\mathcal{P}^{\mathrm{Ent}}(\mathbb{T}^{d}) such that

u(ν)−φ(ν)−δ Ent(ν)<u(μ)−φ(μ)−δ Ent(μ)for every ν∈PEnt(Td) with ν≠μ,u(\nu)-\varphi(\nu)-\delta\,\mathrm{Ent}(\nu)<u(\mu)-\varphi(\mu)-\delta\,\mathrm{Ent}(\mu)\qquad\text{for every }\nu\in\mathcal{P}^{\mathrm{Ent}}(\mathbb{T}^{d})\text{ with }\nu\ne\mu,

one has μ∈PI(Td)\mu\in\mathcal{P}^{\mathcal{I}}(\mathbb{T}^{d}) and

ρ u(μ)+H(μ,∇φ(μ))+σ22 ⟨∇φ(μ),ξμ⟩μ≤δ c(∥∇φ(μ)∥μ).\rho\,u(\mu)+H\bigl(\mu,\nabla\varphi(\mu)\bigr)+\frac{\sigma^{2}}{2}\,\bigl\langle\nabla\varphi(\mu),\xi_{\mu}\bigr\rangle_{\mu}\le\delta\,c\bigl(\lVert\nabla\varphi(\mu)\rVert_{\mu}\bigr).

2. (Supersolution) uu is an entropy-penalised viscosity supersolution of (E)(\mathrm{E}) if there are a real number δ0>0\delta_{0}>0 and a nondecreasing function c:[0,∞)→[0,∞)c:[0,\infty)\to[0,\infty) with the following property. For every intrinsic test function φ\varphi on Pac(Td)\mathcal{P}^{\mathrm{ac}}(\mathbb{T}^{d}), every real δ\delta with 0<δ≤δ00<\delta\le\delta_{0}, and every μ∈PEnt(Td)\mu\in\mathcal{P}^{\mathrm{Ent}}(\mathbb{T}^{d}) such that

u(ν)−φ(ν)+δ Ent(ν)>u(μ)−φ(μ)+δ Ent(μ)for every ν∈PEnt(Td) with ν≠μ,u(\nu)-\varphi(\nu)+\delta\,\mathrm{Ent}(\nu)>u(\mu)-\varphi(\mu)+\delta\,\mathrm{Ent}(\mu)\qquad\text{for every }\nu\in\mathcal{P}^{\mathrm{Ent}}(\mathbb{T}^{d})\text{ with }\nu\ne\mu,

one has μ∈PI(Td)\mu\in\mathcal{P}^{\mathcal{I}}(\mathbb{T}^{d}) and

ρ u(μ)+H(μ,∇φ(μ))+σ22 ⟨∇φ(μ),ξμ⟩μ≥−δ c(∥∇φ(μ)∥μ).\rho\,u(\mu)+H\bigl(\mu,\nabla\varphi(\mu)\bigr)+\frac{\sigma^{2}}{2}\,\bigl\langle\nabla\varphi(\mu),\xi_{\mu}\bigr\rangle_{\mu}\ge-\delta\,c\bigl(\lVert\nabla\varphi(\mu)\rVert_{\mu}\bigr).

3. (Solution) uu is an entropy-penalised viscosity solution of (E)(\mathrm{E}) if it is both an entropy-penalised viscosity subsolution and an entropy-penalised viscosity supersolution of (E)(\mathrm{E}).

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