TheoremBase

Well-Posedness of the Lifted Ornstein-Uhlenbeck Hamilton-Jacobi Equation Relative to a Diagonal Gaussian Measure: Comparison, Existence and Uniqueness of a Bounded Viscosity Solution

For a bounded, Wasserstein-uniformly continuous running cost and control cost theta in (0,1], the lifted Ornstein-Uhlenbeck Hamilton-Jacobi equation relative to a diagonal Gaussian satisfies comparison and has exactly one bounded viscosity solution on the finite-entropy measures, bounded by the sup of the cost over the discount.

Statement

In the settings of The Real Numbers: Standing Notation and Background and The Intrinsic Calculus on the Wasserstein Space: Standing Notation, let cc be a variance vector, let a∈Ra\in\mathbb{R} be positive, and let (D,DΣ,E,Σ)(\mathcal{D},\mathcal{D}_{\Sigma},\mathcal{E},\Sigma) be the Gaussian free-energy pair with variances cc and temperature aa. Let λ0,θ∈R\lambda_{0},\theta\in\mathbb{R} satisfy 0<λ00<\lambda_{0} and 0<θ≤10<\theta\le1, and let g:P2(Rd)→Rg:\mathcal{P}_{2}(\mathbb{R}^{d})\to\mathbb{R} be bounded and uniformly continuous from (P2(Rd),W2)(\mathcal{P}_{2}(\mathbb{R}^{d}),W_{2}) to R\mathbb{R} with the metric of The Absolute Value Metric on the Real Line; fix C∈RC\in\mathbb{R} with ∣g(μ)∣≤C|g(\mu)|\le C for every μ∈P2(Rd)\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}), where ∣s∣|s| is the absolute value. Viscosity subsolutions, supersolutions and solutions are those of the lifted Ornstein-Uhlenbeck Hamilton-Jacobi equation with discount λ0\lambda_{0}, control cost θ\theta and running cost gg.

1. (Comparison) Let u:D→Ru:\mathcal{D}\to\mathbb{R} be a viscosity subsolution and v:D→Rv:\mathcal{D}\to\mathbb{R} a viscosity supersolution, and let b,b′∈Rb,b'\in\mathbb{R} satisfy u(μ)≤bu(\mu)\le b and b′≤v(μ)b'\le v(\mu) for every μ∈D\mu\in\mathcal{D}. Then u(μ)≤v(μ)u(\mu)\le v(\mu) for every μ∈D\mu\in\mathcal{D}.

2. (Existence) There is a viscosity solution u:D→Ru:\mathcal{D}\to\mathbb{R} with, λ0−1\lambda_{0}^{-1} denoting the multiplicative inverse of λ0\lambda_{0},

−λ0−1C≤u(μ)≤λ0−1Cfor every μ∈D.-\lambda_{0}^{-1}C\le u(\mu)\le\lambda_{0}^{-1}C\qquad\text{for every }\mu\in\mathcal{D}.

3. (Uniqueness) Let u,u′:D→Ru,u':\mathcal{D}\to\mathbb{R} be viscosity solutions, each bounded. Then u(μ)=u′(μ)u(\mu)=u'(\mu) for every μ∈D\mu\in\mathcal{D}.

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