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.
In the setting of Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation, let be the set of The Measures Noise-Connected to the Reference Measure §space and the noise Wasserstein distance. For , the rescaled head map and the lift are those of Lifting Euclidean Tangent Fields of the Rescaled Head to Noise Tangent Fields on a Hilbert Space, and for we write . On , the set of The Second Moment of a Probability Measure on Euclidean Space and the Probability Measures with Finite Second Moment §space, the quadratic Wasserstein distance , optimal couplings and the spaces of Square-Integrable Vector Fields Against a Probability Measure on Euclidean Space, and Test Functions: Standing Notation §l2mu are read with in place of the dimension written there, in the settings named there. Let be such that the ordered pair is uniquely noise-mapped, and let be a noise-optimal map from to , with displacement , the space of Probability Measures on a Hilbert Space Transported in the Noise Norm: Standing Notation §fields with norm . Then 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 by Lifting Euclidean Tangent Fields of the Rescaled Head to Noise Tangent Fields on a Hilbert Space §head. For every let be a Borel map such that is an optimal coupling of and ; write for the map .
1. (Head cost) For every , .
2. (The lift) For every , the lift of Lifting Euclidean Tangent Fields of the Rescaled Head to Noise Tangent Fields on a Hilbert Space §lift is defined, and .
3. (Strong convergence) as .
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