Fix and a finite epsilon-net in . Choose a Borel map with , for example the nearest point with ties broken by index. Its cells give discrete probability measures with masses and . LetThe feasible set is nonempty and compact, so the minimum exists. Pushing any coupling forward by changes its cost by at most , hence . Conversely, lift a discrete coupling by the measureTerms with zero row or column masses vanish. This lift has marginals , and its cost differs by at most . Therefore
Here is the finite linear programming duality proof. Write and consider the convex coneIt is closed and finitely generated. One elementary justification of closedness is to reduce each nonnegative representation to linearly independent generators, eliminating a coefficient along any linear dependence; after choosing a subsequence using the same subset of generators, their independent coordinates have bounded, convergent coefficients whenever the represented vectors converge. For , the point lies outside . Separation from this closed convex cone gives coefficients withIf , summing the middle inequalities against any feasible contradicts the last one. Thus , and , obey with dual objective greater than . The weak inequality already proved gives the reverse bound. Letting proves finite strong duality.
Reduce this discrete dual to a single Lipschitz function. For a feasible pair put . The triangle inequality gives , while and . ConsequentlyConversely, any -Lipschitz vector gives a feasible pair . Adding a constant leaves its objective unchanged, so impose . The resulting feasible set is compact, and its maximum is .
For a maximizing vector, the McShane extension theorem has the following explicit proof in this situation. DefineThe triangle inequality proves that this extension is -Lipschitz, and the discrete Lipschitz condition makes . Thus is a continuous feasible pair. Because ,Letting , together with part i, proves . The infimum defining is also attained: the set of couplings is a closed subset of the compact space of probability measures on , and integrating the continuous cost is continuous for the weak-star topology.
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