TheoremBase

Viscosity Subsolutions, Supersolutions and Solutions Relative to a Penalty Pair and a Profile

Given a penalty pair, an equation operator and an intrinsic test function called the profile, a function is a viscosity subsolution, supersolution or solution relative to the profile when its difference with the profile is one, in the penalised sense, of the operator shifted by the profile and its derivatives.

Statement

In the setting of The Intrinsic Calculus on the Wasserstein Space: Standing Notation, let (D,DΣ,E,Σ)(\mathcal{D},\mathcal{D}_{\Sigma},\mathcal{E},\Sigma) be a penalty pair on P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}), let FF be a second-order equation operator over DΣ\mathcal{D}_{\Sigma}, let Φ\Phi be an intrinsic test function on D\mathcal{D}, with gradients along couplings ∇Φ(ν)\nabla\Phi(\nu) and translation Hessians HΦ(ν)H_{\Phi}(\nu), and let u:D→Ru:\mathcal{D}\to\mathbb{R}. The function u−Φu-\Phi on D\mathcal{D} takes the value u(μ)−Φ(μ)u(\mu)-\Phi(\mu) at μ\mu. In this item the letter qq denotes a vector field and the letter rr a real number.

1. (The shifted operator) Let (ν,q)∈V(DΣ)(\nu,q)\in\mathcal{V}(\mathcal{D}_{\Sigma}), r∈Rr\in\mathbb{R} and Y∈S(d)Y\in\mathcal{S}(d). Then ν∈D\nu\in\mathcal{D} by Penalty Pairs on the Wasserstein Space: the Penalty, Its Score, and Their Domains §pair, so ∇Φ(ν)∈Tν⊆L2(ν;Rd)\nabla\Phi(\nu)\in T_{\nu}\subseteq L^{2}(\nu;\mathbb{R}^{d}) by property (b) of Intrinsic Test Functions on the Wasserstein Space and Their Translation Hessians §differentiability and q+∇Φ(ν)∈L2(ν;Rd)q+\nabla\Phi(\nu)\in L^{2}(\nu;\mathbb{R}^{d}), and Y+HΦ(ν)∈S(d)Y+H_{\Phi}(\nu)\in\mathcal{S}(d) by claim 1 of The Positive Semidefinite Ordering is a Partial Order Compatible with the Linear Structure. The operator FF shifted by Φ\Phi is the second-order equation operator over DΣ\mathcal{D}_{\Sigma} given by

FΦ(ν,r,q,Y)=F(ν, r+Φ(ν), q+∇Φ(ν), Y+HΦ(ν));F^{\Phi}(\nu,r,q,Y)=F\bigl(\nu,\ r+\Phi(\nu),\ q+\nabla\Phi(\nu),\ Y+H_{\Phi}(\nu)\bigr);

with δ\delta-shifts (FΦ)δ−(F^{\Phi})^{-}_{\delta} and (FΦ)δ+(F^{\Phi})^{+}_{\delta} relative to the penalty pair.

2. (Subsolution) Suppose that u−Φu-\Phi has penalty-subordinate growth from above. The function uu is a viscosity subsolution of FF relative to the penalty pair and the profile Φ\Phi if u−Φu-\Phi is a viscosity subsolution of FΦF^{\Phi} relative to the penalty pair.

3. (Supersolution) Suppose that u−Φu-\Phi has penalty-subordinate growth from below. The function uu is a viscosity supersolution of FF relative to the penalty pair and the profile Φ\Phi if u−Φu-\Phi is a viscosity supersolution of FΦF^{\Phi} relative to the penalty pair.

4. (Solution) Suppose that u−Φu-\Phi has penalty-subordinate growth from above and from below. The function uu is a viscosity solution of FF relative to the penalty pair and the profile Φ\Phi if it is both a viscosity subsolution and a viscosity supersolution of FF relative to the penalty pair and the profile Φ\Phi.

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