In the setting of Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation , let μ , ρ , ν ∈ P 2 ( R d ) \mu,\rho,\nu\in\mathcal{P}_{2}(\mathbb{R}^{d}) μ , ρ , ν ∈ P 2 ( R d ) , let π 12 ∈ Π ( μ , ρ ) \pi_{12}\in\Pi(\mu,\rho) π 12 ∈ Π ( μ , ρ ) and π 23 ∈ Π ( ρ , ν ) \pi_{23}\in\Pi(\rho,\nu) π 23 ∈ Π ( ρ , ν ) be couplings , with M 2 M_{2} M 2 the second moment and I I I the quadratic cost fixed there, and let q 1 , q 2 , q 3 : R 3 d → R d \mathrm{q}_{1},\mathrm{q}_{2},\mathrm{q}_{3}:\mathbb{R}^{3d}\to\mathbb{R}^{d} q 1 , q 2 , q 3 : R 3 d → R d be the coordinate maps of the threefold product , which are Borel, as are the pairings ( q 1 , q 2 ) (\mathrm{q}_{1},\mathrm{q}_{2}) ( q 1 , q 2 ) , ( q 2 , q 3 ) (\mathrm{q}_{2},\mathrm{q}_{3}) ( q 2 , q 3 ) and ( q 1 , q 3 ) (\mathrm{q}_{1},\mathrm{q}_{3}) ( q 1 , q 3 ) . For σ ∈ P ( R 3 d ) \sigma\in\mathcal{P}(\mathbb{R}^{3d}) σ ∈ P ( R 3 d ) , L 2 ( σ ; R d ) L^{2}(\sigma;\mathbb{R}^{d}) L 2 ( σ ; R d ) is the space of square-integrable vector fields against σ \sigma σ , read with 3 d 3d 3 d in place of q q q and d d d in place of r r r , with its inner product ⟨ ⋅ , ⋅ ⟩ σ \langle\cdot,\cdot\rangle_{\sigma} ⟨ ⋅ , ⋅ ⟩ σ and norm ∥ ⋅ ∥ σ \lVert\cdot\rVert_{\sigma} ∥ ⋅ ∥ σ ; the class of a Borel map R 3 d → R d \mathbb{R}^{3d}\to\mathbb{R}^{d} R 3 d → R d that is square-integrable against σ \sigma σ 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 σ ∈ P ( R 3 d ) \sigma\in\mathcal{P}(\mathbb{R}^{3d}) σ ∈ P ( R 3 d ) with
( q 1 , q 2 ) # σ = π 12 , ( q 2 , q 3 ) # σ = π 23 ; (\mathrm{q}_{1},\mathrm{q}_{2})_{\#}\sigma=\pi_{12},\qquad(\mathrm{q}_{2},\mathrm{q}_{3})_{\#}\sigma=\pi_{23}; ( q 1 , q 2 ) # σ = π 12 , ( q 2 , q 3 ) # σ = π 23 ;
such a σ \sigma σ is called a gluing of π 12 \pi_{12} π 12 and π 23 \pi_{23} π 23 .
2. (The coordinate fields of a gluing) ¶ Let σ \sigma σ be a gluing of π 12 \pi_{12} π 12 and π 23 \pi_{23} π 23 . Then the classes of q 1 \mathrm{q}_{1} q 1 , q 2 \mathrm{q}_{2} q 2 and q 3 \mathrm{q}_{3} q 3 belong to L 2 ( σ ; R d ) L^{2}(\sigma;\mathbb{R}^{d}) L 2 ( σ ; R d ) , with
∥ q 1 ∥ σ 2 = M 2 ( μ ) , ∥ q 2 ∥ σ 2 = M 2 ( ρ ) , ∥ q 3 ∥ σ 2 = M 2 ( 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), ∥ q 1 ∥ σ 2 = M 2 ( μ ) , ∥ q 2 ∥ σ 2 = M 2 ( ρ ) , ∥ q 3 ∥ σ 2 = M 2 ( ν ) ,
∥ q 1 − q 2 ∥ σ 2 = I ( π 12 ) , ∥ q 2 − q 3 ∥ σ 2 = I ( π 23 ) . \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}). ∥ q 1 − q 2 ∥ σ 2 = I ( π 12 ) , ∥ q 2 − q 3 ∥ σ 2 = I ( π 23 ) .
3. (The composite coupling) ¶ Let σ \sigma σ be a gluing of π 12 \pi_{12} π 12 and π 23 \pi_{23} π 23 . Then ( q 1 , q 3 ) # σ (\mathrm{q}_{1},\mathrm{q}_{3})_{\#}\sigma ( q 1 , q 3 ) # σ belongs to Π ( μ , ν ) \Pi(\mu,\nu) Π ( μ , ν ) ,
∥ q 1 − q 3 ∥ σ 2 = I ( ( q 1 , q 3 ) # σ ) , \lVert\mathrm{q}_{1}-\mathrm{q}_{3}\rVert_{\sigma}^{2}=I\bigl((\mathrm{q}_{1},\mathrm{q}_{3})_{\#}\sigma\bigr), ∥ q 1 − q 3 ∥ σ 2 = I ( ( q 1 , q 3 ) # σ ) ,
and
I ( ( q 1 , q 3 ) # σ ) ≤ I ( π 12 ) + I ( π 23 ) . \sqrt{I\bigl((\mathrm{q}_{1},\mathrm{q}_{3})_{\#}\sigma\bigr)}\le\sqrt{I(\pi_{12})}+\sqrt{I(\pi_{23})}. I ( ( q 1 , q 3 ) # σ ) ≤ I ( π 12 ) + I ( π 23 ) .