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Couplings of Two Borel Probability Measures on a Hilbert Space and Their Quadratic Cost

Defines couplings of two Borel probability measures on a Hilbert space and the quadratic cost of a coupling.

Statement

In the setting of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation, let μ,ν∈P(X)\mu,\nu\in\mathcal{P}(X), and let π1,π2:X×X→X\pi_{1},\pi_{2}:X\times X\to X be the coordinate maps of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §pairs, which are Borel by Borel Sets of a Hilbert Space with an Orthonormal Basis: Coordinates, Determination by Finite-Dimensional Projections, and Pairs §product-sigma. In this definition and its dependents the letter II denotes the quadratic cost below, not the identity form of Real Hilbert Spaces: Standing Notation and Background §forms.

1. (Coupling) A coupling of μ\mu and ν\nu is a π∈P(X×X)\pi\in\mathcal{P}(X\times X) with (π1)#π=μ(\pi_{1})_{\#}\pi=\mu and (π2)#π=ν(\pi_{2})_{\#}\pi=\nu. The set of couplings of μ\mu and ν\nu is denoted Π(μ,ν)\Pi(\mu,\nu).

2. (Quadratic cost) The quadratic cost of π∈Π(μ,ν)\pi\in\Pi(\mu,\nu) is

I(π)=∫X×X∣π1(z)−π2(z)∣2 π(dz)∈[0,∞],I(\pi)=\int_{X\times X}|\pi_{1}(z)-\pi_{2}(z)|^{2}\,\pi(dz)\in[0,\infty],

the integral of a nonnegative function that is continuous on (X×X,d)(X\times X,d), hence Borel by claims 2 and 3 of Borel Measurability and Bounded Integration on a Metric Space: the maps π1,π2\pi_{1},\pi_{2} are linear with ∣πiz∣≤∣z∣|\pi_{i}z|\le|z| by Properties of the Product of Two Real Inner Product Spaces §coordinates, so z↦π1(z)−π2(z)z\mapsto\pi_{1}(z)-\pi_{2}(z) is Lipschitz with constant 22, and x↦∣x∣2x\mapsto|x|^{2} is continuous on XX as recorded in The Second Moment of a Borel Probability Measure on a Hilbert Space and the Probability Measures with Finite Second Moment.

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