TheoremBase

Well-Posedness of the Hamilton-Jacobi Equation with the Free-Field Score Drift for Laws of Distributions on the Torus: Comparison, Existence and Uniqueness of a Bounded Viscosity Solution

For laws of distributions on the torus with finite entropy relative to the free field, and a bounded running cost uniformly continuous for the Wasserstein distance with L2L^2 cost, the Hamilton-Jacobi equation with the free-field score drift has comparison and exactly one bounded viscosity solution.

Statement

In the setting of The Free Field on the Torus as the Gaussian Reference Measure, with Square-Integrable White Noise: Standing Notation, let (D,DΣ,E,Σ)(\mathcal{D},\mathcal{D}_{\Sigma},\mathcal{E},\Sigma) be the Gaussian entropy pair with temperature 11, whose hypothesis holds with the constant 11 by White Noise in the Square-Integrable Space and the Free Field on the Torus as Noise Weights and a Variance Sequence on a Negative Sobolev Space §ratio; thus D\mathcal{D} is the set of Borel probability measures on X=H−m(Tn)X=H^{-m}(\mathbb{T}^{n}) of finite relative entropy with respect to the free field γc\gamma_{c}, by The Gaussian Entropy Pair on the Noise Wasserstein Space: Relative Entropy and the Noise Score Field §penalty-domain. WaW_{a} is the noise Wasserstein distance, whose cost ∣y−x∣a2|y-x|_{a}^{2} equals ∥U∥L22\lVert U\rVert_{L^{2}}^{2} when y−x=U^y-x=\hat{U} with U∈L2(Tn)U\in L^{2}(\mathbb{T}^{n}), by White Noise in the Square-Integrable Space and the Free Field on the Torus as Noise Weights and a Variance Sequence on a Negative Sobolev Space §noise-space, and (Pρa,Wa)(\mathcal{P}^{a}_{\rho},W_{a}) is the metric space 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, which contains D\mathcal{D}. 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 (Pρa,Wa)(\mathcal{P}^{a}_{\rho},W_{a}) 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 the free field with temperature 11 (so that its score term is 1⋅⟨Zνa,q⟩ν=⟨Zνa,q⟩ν1\cdot\langle Z^{a}_{\nu},q\rangle_{\nu}=\langle Z^{a}_{\nu},q\rangle_{\nu}), discount λ0\lambda_{0}, control cost θ\theta and running cost gg,

λ0 r+θ2 ∥q∥ν2+⟨Zνa,q⟩ν=g(ν),\lambda_{0}\,r+\frac{\theta}{2}\,\lVert q\rVert_{\nu}^{2}+\langle Z^{a}_{\nu},q\rangle_{\nu}=g(\nu),

an equation in (ν,r,q)(\nu,r,q) read as in that clause, with ZνaZ^{a}_{\nu} the noise score field of ν∈DΣ\nu\in\mathcal{D}_{\Sigma}.

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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