TheoremBase

The Wasserstein Distance and the Mean-Square Distance of Random Vectors

The law map from L2(OmegaL^2(Omega;Rd)R^d) to P2(Rd)P_2(R^d) is well defined and contracts the Wasserstein distance below the L2L^2 distance; on a rich probability space it is surjective and the Wasserstein distance is the infimum of the L2L^2 distance over random vectors with the prescribed laws.

Statement

In the setting of Probability Measures on Euclidean Space and Random Vectors: Standing Notation, let d∈Nd\in\mathbb{N} satisfy 1≤d1\le d. Let L2(Ω;Rd)L^{2}(\Omega;\mathbb{R}^{d}) be the space of classes of square-integrable random vectors, with its norm ∥⋅∥L2\lVert\cdot\rVert_{L^{2}}, the law L(X)\mathcal{L}(X) of a class and the notational convention fixed there; let P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}) be the set of probability measures with finite second moment and W2W_{2} the quadratic Wasserstein distance. Then the following hold.

1. (The law map) The map Λ:L2(Ω;Rd)→P2(Rd)\Lambda:L^{2}(\Omega;\mathbb{R}^{d})\to\mathcal{P}_{2}(\mathbb{R}^{d}), Λ(X)=L(X)\Lambda(X)=\mathcal{L}(X), is well defined, by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations (ii).

2. (The Wasserstein distance is dominated by the mean-square distance) For all X,Y∈L2(Ω;Rd)X,Y\in L^{2}(\Omega;\mathbb{R}^{d}),

W2(L(X),L(Y))≤∥X−Y∥L2.W_{2}\bigl(\mathcal{L}(X),\mathcal{L}(Y)\bigr)\le\lVert X-Y\rVert_{L^{2}} .

3. (Surjectivity on a rich space) If (Ω,F,P)(\Omega,\mathcal{F},P) is rich, then for every μ∈P2(Rd)\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}) there is X∈L2(Ω;Rd)X\in L^{2}(\Omega;\mathbb{R}^{d}) with L(X)=μ\mathcal{L}(X)=\mu; that is, Λ\Lambda is surjective.

4. (The distance as an infimum over random vectors) If (Ω,F,P)(\Omega,\mathcal{F},P) is rich, then for all μ,ν∈P2(Rd)\mu,\nu\in\mathcal{P}_{2}(\mathbb{R}^{d}) the set D(μ,ν)={∥X−Y∥L2:X,Y∈L2(Ω;Rd), L(X)=μ, L(Y)=ν}D(\mu,\nu)=\{\lVert X-Y\rVert_{L^{2}}:X,Y\in L^{2}(\Omega;\mathbb{R}^{d}),\ \mathcal{L}(X)=\mu,\ \mathcal{L}(Y)=\nu\} is a nonempty set of real numbers bounded below by W2(μ,ν)W_{2}(\mu,\nu), hence has a greatest lower bound inf⁡D(μ,ν)\inf D(\mu,\nu) by Existence of the Infimum of a Nonempty Subset of R\mathbb{R} Bounded Below, and

W2(μ,ν)=inf⁡D(μ,ν).W_{2}(\mu,\nu)=\inf D(\mu,\nu).

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