TheoremBase

A Pair Maximising a Quadratically Penalised Difference of Law-Invariant Functions Within Its Laws Realises an Optimal Coupling

On a rich probability space, if a pair of square-integrable random vectors maximises U(X) - V(Y) - alpha times the squared mean-square distance among pairs with the same laws, U and V law-invariant, then its mean-square distance equals the Wasserstein distance of the laws and the law of the pair is an optimal coupling.

Statement

In the setting of The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation, assume that (Ω,F,P)(\Omega,\mathcal{F},P) is rich. Let L2(Ω;Rd)L^{2}(\Omega;\mathbb{R}^{d}) be the space of classes of square-integrable random vectors, and (P2(Rd),W2)(\mathcal{P}_{2}(\mathbb{R}^{d}),W_{2}) the Wasserstein space, so that L(X)∈P2(Rd)\mathcal{L}(X)\in\mathcal{P}_{2}(\mathbb{R}^{d}) for every X∈L2(Ω;Rd)X\in L^{2}(\Omega;\mathbb{R}^{d}) by The Wasserstein Space and Its Lift to Square-Integrable Random Vectors: Standing Notation (v). Let U,V:L2(Ω;Rd)→RU,V:L^{2}(\Omega;\mathbb{R}^{d})\to\mathbb{R} be law-invariant, let α∈R\alpha\in\mathbb{R} be positive, and let X0,Y0∈L2(Ω;Rd)X_{0},Y_{0}\in L^{2}(\Omega;\mathbb{R}^{d}) satisfy

U(X)−V(Y)−α ∥X−Y∥L22≤U(X0)−V(Y0)−α ∥X0−Y0∥L22U(X)-V(Y)-\alpha\,\lVert X-Y\rVert_{L^{2}}^{2}\le U(X_{0})-V(Y_{0})-\alpha\,\lVert X_{0}-Y_{0}\rVert_{L^{2}}^{2}

for all X,Y∈L2(Ω;Rd)X,Y\in L^{2}(\Omega;\mathbb{R}^{d}) with L(X)=L(X0)\mathcal{L}(X)=\mathcal{L}(X_{0}) and L(Y)=L(Y0)\mathcal{L}(Y)=\mathcal{L}(Y_{0}). Then the following hold.

1. (The penalty is the Wasserstein distance)

∥X0−Y0∥L2=W2(L(X0),L(Y0)).\lVert X_{0}-Y_{0}\rVert_{L^{2}}=W_{2}\bigl(\mathcal{L}(X_{0}),\mathcal{L}(Y_{0})\bigr).

2. (The pair realises an optimal coupling) The law of the pairing (X0,Y0)(X_{0},Y_{0}) of any representatives of X0X_{0} and Y0Y_{0}, a random vector in Rd+d\mathbb{R}^{d+d} by Random Vectors: Coordinates, Functions, Pairs and Almost-Sure Equality (v), is an optimal coupling of L(X0)\mathcal{L}(X_{0}) and L(Y0)\mathcal{L}(Y_{0}).

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