TheoremBase

Equation Operators on the Wasserstein Space with Momentum-Continuous Shifts

An equation operator on the Wasserstein space has momentum-continuous shifts if, at each weight delta in (0,1) and each level R, its two delta-shifts are uniformly continuous in the vector-field argument over data bounded by R with score bounded by R.

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}) and 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 for each positive δ∈R\delta\in\mathbb{R}. For ν∈DΣ\nu\in\mathcal{D}_{\Sigma} the score Σ(ν)\Sigma(\nu) lies in TνT_{\nu}, hence in the real Hilbert space L2(ν;Rd)L^{2}(\nu;\mathbb{R}^{d}) of Square-Integrable Vector Fields Against a Probability Measure on Euclidean Space, and Test Functions: Standing Notation §l2mu, by Penalty Pairs on the Wasserstein Space: the Penalty, Its Score, and Their Domains §pair; for q,q′∈L2(ν;Rd)q,q'\in L^{2}(\nu;\mathbb{R}^{d}) the difference q−q′q-q' is taken in that space; ∥⋅∥\lVert\cdot\rVert is the norm on S(d)\mathcal{S}(d) of Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation §matrices; and ∣s∣|s| is the absolute value of s∈Rs\in\mathbb{R}. In this definition the letter rr denotes a real number; the dimension written rr in Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation is not used.

(Momentum-continuous shifts) The operator FF has momentum-continuous shifts relative to the penalty pair if for all δ,R,η∈R\delta,R,\eta\in\mathbb{R} with 0<δ<10<\delta<1, 0<R0<R and 0<η0<\eta there is a positive ρ∈R\rho\in\mathbb{R} such that

∣Fδ−(ν,r,q,Y)−Fδ−(ν,r,q′,Y)∣<ηand∣Fδ+(ν,r,q,Y)−Fδ+(ν,r,q′,Y)∣<η\bigl|F^{-}_{\delta}(\nu,r,q,Y)-F^{-}_{\delta}(\nu,r,q',Y)\bigr|<\eta\qquad\text{and}\qquad\bigl|F^{+}_{\delta}(\nu,r,q,Y)-F^{+}_{\delta}(\nu,r,q',Y)\bigr|<\eta

for every ν∈DΣ\nu\in\mathcal{D}_{\Sigma} with ∥Σ(ν)∥ν≤R\lVert\Sigma(\nu)\rVert_{\nu}\le R, every r∈Rr\in\mathbb{R} with ∣r∣≤R|r|\le R, all q,q′∈L2(ν;Rd)q,q'\in L^{2}(\nu;\mathbb{R}^{d}) with ∥q∥ν≤R\lVert q\rVert_{\nu}\le R, ∥q′∥ν≤R\lVert q'\rVert_{\nu}\le R and ∥q−q′∥ν<ρ\lVert q-q'\rVert_{\nu}<\rho, and every Y∈S(d)Y\in\mathcal{S}(d) with ∥Y∥≤R\lVert Y\rVert\le R.

Citations

Loading…

Dependencies

Loading…

Related

0 relations

Curated associations between results. These are editable and subjective — they do not replace the dependency graph, which is derived from the references in the text.

No relations recorded yet.

Comments

Log in to comment.

Loading…