TheoremBase

Lifted Optimal Maps between Rescaled Heads Converge Strongly to the Noise-Optimal Displacement

For a uniquely noise-mapped pair, the optimal Euclidean maps between the rescaled heads, lifted back to the Hilbert space, have cost at most the squared noise Wasserstein distance and converge strongly to the displacement of the noise-optimal map.

Statement

In the setting of Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation, let Pρa\mathcal{P}^{a}_{\rho} be the set of The Measures Noise-Connected to the Reference Measure §space and WaW_{a} the noise Wasserstein distance. For n∈Nn\in\mathbb{N}, the rescaled head map rnr_{n} and the lift Λn\Lambda_{n} are those of Lifting Euclidean Tangent Fields of the Rescaled Head to Noise Tangent Fields on a Hilbert Space, and for λ∈P(X)\lambda\in\mathcal{P}(X) we write λ~n=(rn)#λ\tilde{\lambda}_{n}=(r_{n})_{\#}\lambda. On Rn\mathbb{R}^{n}, the set P2(Rn)\mathcal{P}_{2}(\mathbb{R}^{n}) of The Second Moment of a Probability Measure on Euclidean Space and the Probability Measures with Finite Second Moment §space, the quadratic Wasserstein distance W2W_{2}, optimal couplings and the spaces L2(λ;Rn)L^{2}(\lambda;\mathbb{R}^{n}) of Square-Integrable Vector Fields Against a Probability Measure on Euclidean Space, and Test Functions: Standing Notation §l2mu are read with nn in place of the dimension written dd there, in the settings named there. Let μ,ν∈Pρa\mu,\nu\in\mathcal{P}^{a}_{\rho} be such that the ordered pair (μ,ν)(\mu,\nu) is uniquely noise-mapped, and let TT be a noise-optimal map from μ\mu to ν\nu, with displacement T−id∈L2(μ;Xa)T-\mathrm{id}\in L^{2}(\mu;X^{a}), the space of Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §fields with norm ∥⋅∥μ\lVert\cdot\rVert_{\mu}. Then μ,ν∈P2(X)\mu,\nu\in\mathcal{P}_{2}(X) by The Noise Wasserstein Distance is a Metric on the Measures Noise-Connected to the Reference Measure: Existence of Noise-Optimal Couplings, Comparison with the Quadratic Wasserstein Distance and Lower Semicontinuity §moments, so μ~n,ν~n∈P2(Rn)\tilde{\mu}_{n},\tilde{\nu}_{n}\in\mathcal{P}_{2}(\mathbb{R}^{n}) by Lifting Euclidean Tangent Fields of the Rescaled Head to Noise Tangent Fields on a Hilbert Space §head. For every n∈Nn\in\mathbb{N} let Sn:Rn→RnS_{n}:\mathbb{R}^{n}\to\mathbb{R}^{n} be a Borel map such that (id,Sn)#μ~n(\mathrm{id},S_{n})_{\#}\tilde{\mu}_{n} is an optimal coupling of μ~n\tilde{\mu}_{n} and ν~n\tilde{\nu}_{n}; write Sn−idS_{n}-\mathrm{id} for the map u↦Sn(u)−uu\mapsto S_{n}(u)-u.

1. (Head cost) For every n∈Nn\in\mathbb{N}, ∫Rn∥Sn(u)−u∥2 μ~n(du)=W2(μ~n,ν~n)2≤Wa(μ,ν)2\int_{\mathbb{R}^{n}}\lVert S_{n}(u)-u\rVert^{2}\,\tilde{\mu}_{n}(du)=W_{2}(\tilde{\mu}_{n},\tilde{\nu}_{n})^{2}\le W_{a}(\mu,\nu)^{2}.

2. (The lift) For every n∈Nn\in\mathbb{N}, the lift Λn(Sn−id)∈L2(μ;Xa)\Lambda_{n}(S_{n}-\mathrm{id})\in L^{2}(\mu;X^{a}) of Lifting Euclidean Tangent Fields of the Rescaled Head to Noise Tangent Fields on a Hilbert Space §lift is defined, and ∥Λn(Sn−id)∥μ≤Wa(μ,ν)\lVert\Lambda_{n}(S_{n}-\mathrm{id})\rVert_{\mu}\le W_{a}(\mu,\nu).

3. (Strong convergence) ∥Λn(Sn−id)−(T−id)∥μ→0\lVert\Lambda_{n}(S_{n}-\mathrm{id})-(T-\mathrm{id})\rVert_{\mu}\to0 as n→∞n\to\infty.

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