Crash Course on Optimal Transport
summary
Covers Monge vs Kantorovich formulations and shows that Monge maps can be empty while Kantorovich couplings always exist, because Kantorovich turns transport into a linear program with convex marginals. States Kantorovich duality and the simple dual for cost |x−y|: a supremum over 1‑Lipschitz potentials. Proves Brenier (called Wren) for quadratic cost: if mu is absolutely continuous then the optimal coupling is unique and equals a map T = ∇φ with φ convex. Defines p‑Wasserstein, geodesics via linear interpolation and constant‑speed property.
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chapters (10)
- 0:00Introduction
- 3:25Brief overview
- 8:28Cost formulation
- 12:13Applications
- 15:45Definitions
- 20:01Question
- 31:36Structure
- 35:37Optimal Coupling
- 50:04Moment Condition
- 56:14Optimal Transport Map
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