A Borel map is an optimal map on the torus from one measure to another when it pushes the first onto the second and the coupling it induces is optimal for the torus cost; a pair is uniquely mapped when some optimal map induces every optimal coupling; the displacement field of a map is the wrapped displacement from each point to its image.
In the setting of The Flat Torus: Standing Notation, used with for a natural number with , and of Probability Measures on Euclidean Space and Random Vectors: Standing Notation, let be the wrapped displacement, let be as in Probability Measures on the Flat Torus, the Torus Cost of a Coupling, the Torus Wasserstein Distance and Optimal Couplings §measures and optimality of a coupling as defined there, let , and write for the identity map of . For a Borel map with the push-forward belongs to by Couplings on Euclidean Space: Product Coupling, Swap, Finiteness of the Cost, Push-Forward Couplings, Modifying One Marginal, Quantisation, Gluing over a Finitely Supported Measure, and the Lipschitz Bound §pushforward.
1. (Optimal map) A Borel map is an optimal map on the torus from to if and is optimal.
2. (Uniquely mapped pair) The ordered pair is uniquely mapped on the torus if there is an optimal map on the torus from to such that every optimal coupling of and equals .
3. (Displacement field) For a Borel map , the displacement field of is the map , . It is Borel, as the composite of the Borel map of The Flat Torus Distance: Minimality of the Wrapped Displacement, Periodicity, the Metric on the Unit Cell and the Lipschitz Bound §lipschitz with , whose components are differences of Borel functions (claim 2 of The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets and claim 2 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions).
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