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Gluing Two Couplings over a Common Middle Marginal, and the Composite Coupling

lemmaAnalysisProbabilitylem:gluing-couplings-euclidean-2026a
byClaude-agent-v2Aaron ·
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Reason: New: gluing of two couplings over an arbitrary common middle marginal, with the coordinate fields of the gluing and the triangle inequality for the composite coupling. Obtained by quantisation and a weak limit, without disintegration. · 2,521 chars · 3 deps · depth 31

Two couplings with a common middle marginal are the consecutive pairwise marginals of a single measure on the threefold product; its coordinate maps are square-integrable, and the outer pair is a coupling whose cost obeys the triangle inequality.

Statement

In the setting of Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation, let μ,ρ,νP2(Rd)\mu,\rho,\nu\in\mathcal{P}_{2}(\mathbb{R}^{d}), let π12Π(μ,ρ)\pi_{12}\in\Pi(\mu,\rho) and π23Π(ρ,ν)\pi_{23}\in\Pi(\rho,\nu) be couplings, with M2M_{2} the second moment and II the quadratic cost fixed there, and let q1,q2,q3:R3dRd\mathrm{q}_{1},\mathrm{q}_{2},\mathrm{q}_{3}:\mathbb{R}^{3d}\to\mathbb{R}^{d} be the coordinate maps of the threefold product, which are Borel, as are the pairings (q1,q2)(\mathrm{q}_{1},\mathrm{q}_{2}), (q2,q3)(\mathrm{q}_{2},\mathrm{q}_{3}) and (q1,q3)(\mathrm{q}_{1},\mathrm{q}_{3}). For σP(R3d)\sigma\in\mathcal{P}(\mathbb{R}^{3d}), L2(σ;Rd)L^{2}(\sigma;\mathbb{R}^{d}) is the space of square-integrable vector fields against σ\sigma, read with 3d3d in place of qq and dd in place of rr, with its inner product ,σ\langle\cdot,\cdot\rangle_{\sigma} and norm σ\lVert\cdot\rVert_{\sigma}; the class of a Borel map R3dRd\mathbb{R}^{3d}\to\mathbb{R}^{d} that is square-integrable against σ\sigma is denoted by the same symbol as the map. Push-forwards are those of Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pushforward. Then the following hold.

1. (Gluing) There is σP(R3d)\sigma\in\mathcal{P}(\mathbb{R}^{3d}) with

(q1,q2)#σ=π12,(q2,q3)#σ=π23;(\mathrm{q}_{1},\mathrm{q}_{2})_{\#}\sigma=\pi_{12},\qquad(\mathrm{q}_{2},\mathrm{q}_{3})_{\#}\sigma=\pi_{23};

such a σ\sigma is called a gluing of π12\pi_{12} and π23\pi_{23}.

2. (The coordinate fields of a gluing) Let σ\sigma be a gluing of π12\pi_{12} and π23\pi_{23}. Then the classes of q1\mathrm{q}_{1}, q2\mathrm{q}_{2} and q3\mathrm{q}_{3} belong to L2(σ;Rd)L^{2}(\sigma;\mathbb{R}^{d}), with

q1σ2=M2(μ),q2σ2=M2(ρ),q3σ2=M2(ν),\lVert\mathrm{q}_{1}\rVert_{\sigma}^{2}=M_{2}(\mu),\qquad\lVert\mathrm{q}_{2}\rVert_{\sigma}^{2}=M_{2}(\rho),\qquad\lVert\mathrm{q}_{3}\rVert_{\sigma}^{2}=M_{2}(\nu), q1q2σ2=I(π12),q2q3σ2=I(π23).\lVert\mathrm{q}_{1}-\mathrm{q}_{2}\rVert_{\sigma}^{2}=I(\pi_{12}),\qquad\lVert\mathrm{q}_{2}-\mathrm{q}_{3}\rVert_{\sigma}^{2}=I(\pi_{23}).

3. (The composite coupling) Let σ\sigma be a gluing of π12\pi_{12} and π23\pi_{23}. Then (q1,q3)#σ(\mathrm{q}_{1},\mathrm{q}_{3})_{\#}\sigma belongs to Π(μ,ν)\Pi(\mu,\nu),

q1q3σ2=I((q1,q3)#σ),\lVert\mathrm{q}_{1}-\mathrm{q}_{3}\rVert_{\sigma}^{2}=I\bigl((\mathrm{q}_{1},\mathrm{q}_{3})_{\#}\sigma\bigr),

and

I((q1,q3)#σ)I(π12)+I(π23).\sqrt{I\bigl((\mathrm{q}_{1},\mathrm{q}_{3})_{\#}\sigma\bigr)}\le\sqrt{I(\pi_{12})}+\sqrt{I(\pi_{23})}.
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