TheoremBase

Well-Posedness of the Hamilton-Jacobi Equation with Gaussian Score Drift on a Hilbert Space: Comparison, Existence and Uniqueness of a Bounded Viscosity Solution

For a bounded, uniformly continuous running cost, the Hamilton-Jacobi equation with Gaussian score drift on laws of finite relative entropy with respect to a diagonal Gaussian measure satisfies comparison and has exactly one bounded viscosity solution.

Statement

In the setting of A Diagonal Gaussian Reference Measure on the Noise Wasserstein Space, Rescaled Heads and Gaussian Tails: Standing Notation, so that the reference measure is ρ=γc\rho=\gamma_{c}, let β\beta and κ\kappa be positive real numbers with ck≤κ akc_{k}\le\kappa\,a_{k} for every k∈Nk\in\mathbb{N}, and let (D,DΣ,E,Σ)(\mathcal{D},\mathcal{D}_{\Sigma},\mathcal{E},\Sigma) be the Gaussian entropy pair with temperature β\beta, whose hypothesis holds with this κ\kappa; it is a noise penalty pair on Pρa\mathcal{P}^{a}_{\rho} by The Gaussian Entropy Pair is a Noise Penalty Pair, with Nonnegative Penalty and Dense Score Domain §pair, and D\mathcal{D} is the set of measures of finite relative entropy with respect to γc\gamma_{c}, by The Gaussian Entropy Pair on the Noise Wasserstein Space: Relative Entropy and the Noise Score Field §penalty-domain. Let ∣s∣|s| denote the absolute value of s∈Rs\in\mathbb{R}. Let λ0,θ∈R\lambda_{0},\theta\in\mathbb{R} satisfy 0<λ00<\lambda_{0} and 0<θ≤10<\theta\le1, and let g:D→Rg:\mathcal{D}\to\mathbb{R} be bounded and uniformly continuous on D\mathcal{D}, relative to D\mathcal{D} in the metric space (Pρa,Wa)(\mathcal{P}^{a}_{\rho},W_{a}) of The Noise Wasserstein Distance is a Metric on the Measures Noise-Connected to the Reference Measure: Existence of Noise-Optimal Couplings, Comparison with the Quadratic Wasserstein Distance and Lower Semicontinuity §metric and with R\mathbb{R} carrying the metric of The Absolute Value Metric on the Real Line. Fix C∈RC\in\mathbb{R} with 0≤C0\le C and ∣g(μ)∣≤C|g(\mu)|\le C for every μ∈D\mu\in\mathcal{D}; such a CC exists, since if C′C' bounds ∣g∣|g| on D\mathcal{D} as in Bounded Real-Valued Function on a Set, the larger of C′C' and 00 serves. Viscosity subsolutions, supersolutions and solutions are those of the Hamilton-Jacobi equation with Gaussian score drift relative to γc\gamma_{c} with temperature β\beta, discount λ0\lambda_{0}, control cost θ\theta and running cost gg.

1. (Comparison) Let u,v:D→Ru,v:\mathcal{D}\to\mathbb{R} and 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}, let uu be a viscosity subsolution and vv a viscosity supersolution. 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}. Consequently, together with claim 2, the equation has exactly one bounded viscosity solution u:D→Ru:\mathcal{D}\to\mathbb{R}.

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