TheoremBase

The Optimal Map as a Square-Integrable Vector Field: Integrability, Transport Cost and Uniqueness of the Class

A Borel map transporting one measure to another is square-integrable against the source; for an optimal map the squared norm of its displacement is the squared Wasserstein distance; and for a uniquely mapped pair all optimal maps define the same square-integrable class.

Statement

In the setting of Square-Integrable Vector Fields Against a Probability Measure on Euclidean Space, and Test Functions: Standing Notation, let μ,ν∈P2(Rd)\mu,\nu\in\mathcal{P}_{2}(\mathbb{R}^{d}), with the second moment M2M_{2} and the Wasserstein distance W2W_{2}, and let L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) be the space of square-integrable vector fields against μ\mu, with norm ∥⋅∥μ\lVert\cdot\rVert_{\mu}. Let id:Rd→Rd\mathrm{id}:\mathbb{R}^{d}\to\mathbb{R}^{d} be the identity map, whose class belongs to L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) by Basic Properties of the Tangent Space: Closed Subspace, the Identity Map Belongs to It, Second-Moment Limits, and Representation of Bounded Functionals on Gradients (ii) and is again written id\mathrm{id}. Push-forwards are those of Probability Measures on Euclidean Space and Random Vectors: Standing Notation (iv), Π(μ,ν)\Pi(\mu,\nu) is the set of couplings of μ\mu and ν\nu, and for a∈Rda\in\mathbb{R}^{d} the translation τa\tau_{a} of Rd\mathbb{R}^{d} is that fixed there, a Borel map. Then the following hold.

1. (Push-forward by a Borel map, and square-integrability) Let S:Rd→RdS:\mathbb{R}^{d}\to\mathbb{R}^{d} be Borel and write ∥S∥2\lVert S\rVert^{2} for the map x↦∥S(x)∥2x\mapsto\lVert S(x)\rVert^{2}, which is Borel and nonnegative by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets (iv). Then

M2(S#μ)=∫Rd∥S∥2 dμM_{2}(S_{\#}\mu)=\int_{\mathbb{R}^{d}}\lVert S\rVert^{2}\,d\mu

in [0,∞][0,\infty]. Consequently, if ∫Rd∥S∥2 dμ<∞\int_{\mathbb{R}^{d}}\lVert S\rVert^{2}\,d\mu<\infty, then S#μ∈P2(Rd)S_{\#}\mu\in\mathcal{P}_{2}(\mathbb{R}^{d}), the class of SS belongs to L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) and is again written SS, and id−S∈L2(μ;Rd)\mathrm{id}-S\in L^{2}(\mu;\mathbb{R}^{d}); and if S#μ=νS_{\#}\mu=\nu, then ∫Rd∥S∥2 dμ=M2(ν)<∞\int_{\mathbb{R}^{d}}\lVert S\rVert^{2}\,d\mu=M_{2}(\nu)<\infty, so the same conclusions hold. In particular, for every a∈Rda\in\mathbb{R}^{d} the translate (τa)#μ(\tau_{a})_{\#}\mu belongs to P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}), with

M2((τa)#μ)≤2 M2(μ)+2 ∥a∥2.M_{2}\bigl((\tau_{a})_{\#}\mu\bigr)\le2\,M_{2}(\mu)+2\,\lVert a\rVert^{2}.

2. (The transport cost of an optimal map) Let TT be an optimal map from μ\mu to ν\nu. Then

∥id−T∥μ2=W2(μ,ν)2.\lVert\mathrm{id}-T\rVert_{\mu}^{2}=W_{2}(\mu,\nu)^{2}.

3. (Uniqueness of the class) Suppose that the ordered pair (μ,ν)(\mu,\nu) is uniquely mapped, and let TT and T′T' be optimal maps from μ\mu to ν\nu. Then the classes of TT and of T′T' in L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}) are equal; consequently so are the classes of id−T\mathrm{id}-T and of id−T′\mathrm{id}-T'.

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