If the source measure on the flat torus is absolutely continuous, the pair is uniquely mapped on the torus; almost every displacement of an optimal map is the unique shortest one and is given by the subgradient of a convex function whose difference from half the squared norm is periodic and Lipschitz; and when the target is also absolutely continuous, the reverse optimal map inverts the forward one and reverses its displacement.
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 as in Probability Measures on the Flat Torus, the Torus Cost of a Coupling, the Torus Wasserstein Distance and Optimal Couplings §measures and the half-open unit cell; let optimal maps on the torus, uniquely mapped pairs on the torus and the displacement field of a Borel map be as defined there, and let regular points of be as defined there. Let and assume that is absolutely continuous. For Borel the set belongs to , as in the preamble of Brenier's Theorem: Optimal Couplings out of an Absolutely Continuous Measure are Induced by a Unique Map. Then the following hold.
1. (Unique optimal map) The pair is uniquely mapped on the torus, and it has an optimal map on the torus with values in . If and are optimal maps on the torus from to , then .
2. (Periodic potential) Let be an optimal map on the torus from to . There are a -periodic function , Lipschitz with constant , such that is convex on , and a set with , such that for every : is differentiable at , the point is regular, and the subdifferential of is
3. (Inverse map) Assume moreover that is absolutely continuous, let be an optimal map on the torus from to and one from to . Then there is a set with such that and for every .
Loading…
No relations recorded yet.