A set of measures noise-connected to the reference measure has the noise map property if every noise-optimal coupling between its members is induced by a map whose displacement lies in the noise tangent space.
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. For the ordered pair is noise-connected 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 §connected, so that the noise Wasserstein distance and the noise-optimal couplings of and are defined. Noise-optimal maps from to , their displacements and uniquely noise-mapped pairs are those of Noise-Optimal Maps and Uniquely Noise-Mapped Pairs, is the identity map of , and is the noise tangent space at .
1. (Noise map property) A set has the noise map property if for all and the ordered pair is uniquely noise-mapped and, denoting a noise-optimal map from to ,
This condition does not depend on the choice of . Indeed, let and be noise-optimal maps from to , the pair being uniquely noise-mapped. The couplings and are both noise-optimal by Noise-Optimal Maps and Uniquely Noise-Mapped Pairs §map, and every noise-optimal coupling of and equals for the map of Noise-Optimal Maps and Uniquely Noise-Mapped Pairs §uniquely-mapped; hence . Writing with and , the function on is with , . Here are Borel by Borel Sets of a Hilbert Space with an Orthonormal Basis: Coordinates, Determination by Finite-Dimensional Projections, and Pairs §product-sigma, is Borel by claim 4 of Borel Measurability and Bounded Integration on a Metric Space, and the pair is Borel by Borel Sets of a Hilbert Space with an Orthonormal Basis: Coordinates, Determination by Finite-Dimensional Projections, and Pairs §pairing; and is continuous, indeed Lipschitz with constant , since for real and, by the triangle inequality of the norm, , so that is Borel by claim 3 of Borel Measurability and Bounded Integration on a Metric Space. Hence the function is Borel by claim 4 of Borel Measurability and Bounded Integration on a Metric Space; likewise , the composite of this function with the Borel map (Borel Sets of a Hilbert Space with an Orthonormal Basis: Coordinates, Determination by Finite-Dimensional Projections, and Pairs §pairing), is Borel by the same claim. The function on is bounded, hence integrable against both measures by claim 6 of Borel Measurability and Bounded Integration on a Metric Space. By the change-of-variables formula its integral against is the integral of the zero function, which is , and its integral against is ; the two are equal. By The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere §vanishing the nonnegative Borel function vanishes for -almost every , that is, for -almost every , so the classes of and of in coincide by The Space of Square-Integrable Maps from a Measure Space into a Hilbert Space with an Orthonormal Basis §classes.
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