TheoremBase

The Structure Estimate at a Maximiser of the Wasserstein-Doubled Difference

For a bounded-above viscosity subsolution and a bounded-below viscosity supersolution on the penalty domain, a nonnegative supremum of the Wasserstein-doubled difference of their delta-envelopes is attained at a pair in the score domain at which the properness constant times the supremum is bounded by the two moduli of the structure condition.

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 Wasserstein-coercive penalty pair on P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}) with closed score along couplings, whose penalty domain D\mathcal{D} has the map property. Let FF be a second-order equation operator over DΣ\mathcal{D}_{\Sigma}, with δ\delta-shifts Fδ−F^{-}_{\delta} and Fδ+F^{+}_{\delta} relative to that pair, that satisfies the shift-coercivity condition and the shift-semicontinuity condition. We write α2\tfrac{\alpha}{2} for the product of α∈R\alpha\in\mathbb{R} with the multiplicative inverse of 22 (claim 8 of Elementary Order Arithmetic in an Ordered Field) and α−1\alpha^{-1} for the multiplicative inverse of a positive α∈R\alpha\in\mathbb{R}; ∣s∣|s| is the absolute value of s∈Rs\in\mathbb{R}.

Let u,v:D→Ru,v:\mathcal{D}\to\mathbb{R} and b,b′∈Rb,b'\in\mathbb{R} satisfy u(σ)≤bu(\sigma)\le b and b′≤v(σ)b'\le v(\sigma) for every σ∈D\sigma\in\mathcal{D}; by The Delta-Envelopes of Bounded Functions and Their Monotonicity in the Weight, for a Wasserstein-Closed Penalty Pair (i), uu has penalty-subordinate growth from above and vv from below. Assume that uu is a viscosity subsolution of FF and that vv is a viscosity supersolution of FF, both relative to the penalty pair. For positive δ∈R\delta\in\mathbb{R} the δ\delta-envelopes uδ−u^{-}_{\delta} of uu and vδ+v^{+}_{\delta} of vv, functions on D\mathcal{D}, are then defined. Fix e0∈Re_{0}\in\mathbb{R} with e0≤E(σ)e_{0}\le\mathcal{E}(\sigma) for every σ∈D\sigma\in\mathcal{D}, as provided by Basic Properties of a Wasserstein-Coercive Penalty Pair (ii).

Let δ,α∈R\delta,\alpha\in\mathbb{R} satisfy 0<δ<10<\delta<1 and 1<α1<\alpha, let Ψδ,α:D×D→R\Psi_{\delta,\alpha}:\mathcal{D}\times\mathcal{D}\to\mathbb{R} be the function with value

Ψδ,α(μ,ν)=uδ−(μ)−vδ+(ν)−α2 W2(μ,ν)2\Psi_{\delta,\alpha}(\mu,\nu)=u^{-}_{\delta}(\mu)-v^{+}_{\delta}(\nu)-\tfrac{\alpha}{2}\,W_{2}(\mu,\nu)^{2}

at (μ,ν)(\mu,\nu), and let M(δ,α)M(\delta,\alpha) be the supremum of its values, a real number by Existence, Penalty Bounds and Monotonicity of the Maximum of the Wasserstein-Doubled Difference of Bounded Functions (i). Assume 0≤M(δ,α)0\le M(\delta,\alpha). Let B,R∈RB,R\in\mathbb{R} satisfy

∣b∣+∣b′∣+∣e0∣≤B,0<2B≤R.|b|+|b'|+|e_{0}|\le B,\qquad 0<2B\le R.

Let λ\lambda be a properness constant for FF at RR, and let (ω1,ω2)(\omega_{1},\omega_{2}) be a second-order structure pair for FF at RR.

(The structure estimate at a maximising pair) Then there is (ρ∗,σ∗)∈DΣ×DΣ(\rho^{*},\sigma^{*})\in\mathcal{D}_{\Sigma}\times\mathcal{D}_{\Sigma} with Ψδ,α(ρ∗,σ∗)=M(δ,α)\Psi_{\delta,\alpha}(\rho^{*},\sigma^{*})=M(\delta,\alpha) and

λ M(δ,α) ≤ ω1(α W2(ρ∗,σ∗)2+α−1)+ω2(δ (∣E(ρ∗)∣+∣E(σ∗)∣+1), α).\lambda\,M(\delta,\alpha)\ \le\ \omega_{1}\bigl(\alpha\,W_{2}(\rho^{*},\sigma^{*})^{2}+\alpha^{-1}\bigr)+\omega_{2}\bigl(\delta\,(|\mathcal{E}(\rho^{*})|+|\mathcal{E}(\sigma^{*})|+1),\ \alpha\bigr).

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