TheoremBase

Brenier's Theorem: Optimal Couplings out of an Absolutely Continuous Measure are Induced by a Unique Map

When the first measure is absolutely continuous, every optimal coupling is induced by a Borel map which is the gradient of a convex function almost everywhere; the optimal coupling and the map are unique.

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 and let μ,ν\mu,\nu belong to the set P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}) of probability measures with finite second moment, whose second moments are written M2(μ)M_{2}(\mu) and M2(ν)M_{2}(\nu). Let Π(μ,ν)\Pi(\mu,\nu) be the set of their couplings, and let optimality of a coupling be as defined there.

Write id\mathrm{id} for the identity map of Rd\mathbb{R}^{d}, which is Borel, being continuous. For a Borel map T:Rd→RdT:\mathbb{R}^{d}\to\mathbb{R}^{d} the pairing (id,T)(\mathrm{id},T) is Borel by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets (ii), so the push-forward (id,T)#μ(\mathrm{id},T)_{\#}\mu of Probability Measures on Euclidean Space and Random Vectors: Standing Notation (iv) is defined, and it belongs to Π(μ,T#μ)\Pi(\mu,T_{\#}\mu) by Couplings on Euclidean Space: Product Coupling, Swap, Finiteness of the Cost, Push-Forward Couplings, Modifying One Marginal, Quantisation, Gluing over a Finitely Supported Measure, and the Lipschitz Bound (iv). For Borel maps S,S′:Rd→RdS,S':\mathbb{R}^{d}\to\mathbb{R}^{d} the function x↦∥S(x)−S′(x)∥2x\mapsto\lVert S(x)-S'(x)\rVert^{2} is Borel by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets (iv) and vanishes exactly where SS and S′S' agree, by claim 2 of Properties of the Euclidean Norm on Rn\mathbb{R}^n: Square, Distance, Vanishing, Coordinate Bounds, Homogeneity, Triangle Inequalities and Expansion of a Square together with the metric axioms of Rn\mathbb{R}^n with the Euclidean Distance Is a Complete Metric Space with Coordinatewise Convergence and claims 1 and 3 of Zero Products and Elementary Identities in a Field; hence {x∈Rd:S(x)≠S′(x)}\{x\in\mathbb{R}^{d}:S(x)\ne S'(x)\}, the preimage of the Borel set R∖{0}\mathbb{R}\setminus\{0\} under that function, belongs to B(Rd)\mathcal{B}(\mathbb{R}^{d}).

Assume that μ\mu is absolutely continuous. Then the following hold.

1. (Every optimal coupling is induced by a map) Let π∈Π(μ,ν)\pi\in\Pi(\mu,\nu) be optimal. Then there is a Borel map T:Rd→RdT:\mathbb{R}^{d}\to\mathbb{R}^{d} with π=(id,T)#μ\pi=(\mathrm{id},T)_{\#}\mu, and every Borel map TT with π=(id,T)#μ\pi=(\mathrm{id},T)_{\#}\mu satisfies T#μ=νT_{\#}\mu=\nu and

∫Rd∥T(x)∥2 μ(dx)=M2(ν)<∞.\int_{\mathbb{R}^{d}}\lVert T(x)\rVert^{2}\,\mu(dx)=M_{2}(\nu)<\infty .

2. (The map is the subgradient of a convex potential) Let π∈Π(μ,ν)\pi\in\Pi(\mu,\nu) be optimal. Then there is a Borel map T:Rd→RdT:\mathbb{R}^{d}\to\mathbb{R}^{d} with π=(id,T)#μ\pi=(\mathrm{id},T)_{\#}\mu for which there are an open convex set G⊆RdG\subseteq\mathbb{R}^{d}, which belongs to B(Rd)\mathcal{B}(\mathbb{R}^{d}) by Product Measures and Lebesgue Measure on ℝⁿ: Standing Notation and Background (iv) and satisfies μ(G)=1\mu(G)=1, a function ϕ:G→R\phi:G\to\mathbb{R} that is convex on GG, and a set D∈B(Rd)D\in\mathcal{B}(\mathbb{R}^{d}) with D⊆GD\subseteq G and μ(D)=1\mu(D)=1, such that ϕ\phi is differentiable at every point of DD and its subdifferential relative to GG satisfies

∂Gϕ(x)={T(x)}for every x∈D.\partial_{G}\phi(x)=\{T(x)\}\qquad\text{for every }x\in D .

3. (Uniqueness of the optimal coupling) If π\pi and π′\pi' are optimal couplings of μ\mu and ν\nu, then π=π′\pi=\pi'.

4. (Uniqueness of the map) If TT and T′T' are Borel maps from Rd\mathbb{R}^{d} to Rd\mathbb{R}^{d} such that (id,T)#μ(\mathrm{id},T)_{\#}\mu and (id,T′)#μ(\mathrm{id},T')_{\#}\mu are optimal couplings of μ\mu and ν\nu, then

μ({x∈Rd: T(x)≠T′(x)})=0.\mu\bigl(\{x\in\mathbb{R}^{d}:\ T(x)\ne T'(x)\}\bigr)=0 .

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