Alphabeta Math
TheoremStatement: AI-adaptedProof: AI-adaptedPipeline-generatedaudited 2026-09-10
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The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

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Skorokhod representation on polish spaces

Statement

Assume AC. If μnμ on a Polish S, there are random elements Yn,Y on ((0,1),B((0,1)),λ) with laws μn,μ and YnY almost surely.

Facts & Assumptions

[F1]

Countable boundary null partitions of a separable metric space: Assume AC. For a separable metric S with Borel probability μ, there are countable refining Borel partitions Pk for k1, all of whose nonempty atoms have diameter at most 2k and μ-null boundary. Together these partitions generate B(S).

[F2]

Interval realization from refining small diameter partitions: Assume AC. Let S be nonempty, complete and separable, and let (Pk) be countable refining Borel partitions with nonempty atoms of diameter at most 2k. Fix orders on each family of children. Every Borel probability σ on S is the law of a measurable Tσ:(0,1)S under Borel Lebesgue probability, obtained by nested interval allocation.

[F3]

Portmanteau theorem: For Borel probabilities μn,μ on a metric space S, the following are equivalent: (i) μnμ; (ii) integrals converge for all bounded uniformly continuous real tests; (iii) lim supnμn(F)μ(F) for every closed F; (iv) lim infnμn(G)μ(G) for every open G; (v) μn(A)μ(A) for every Borel A with μ(A)=0.

Proof

Given: The objects, hypotheses and definitions in the statement. Its conclusions are to be established below.

1.1

Fix a compatible complete metric. F1 supplies countable refining partitions with diameters at most 2^{-k} and μ-null boundaries. Fix the same child orders and representatives for all laws. F2 constructs Yn and Y for these laws on the indicated Borel interval, with exactly their prescribed marginals.

F1F2
1.2

By F3, every fixed atom A satisfies μn(A)->μ(A). The endpoints of its interval are the left endpoint of its parent plus a finite sum of the masses of preceding children, and possibly its own mass. Starting with root endpoints 0,1 and inducting over each finite address proves convergence of both endpoints for every fixed atom interval.

F3
2.1

Remove the countable union of all endpoint sets for μ and for every μn; each is null by the realization lemma. For a remaining u and any fixed level k, u lies strictly between the endpoints of its μ interval. Step 1.2 and induction along its finite ancestral address imply that for all sufficiently large n, u lies in the same atom interval for μn. The limits Yn(u),Y(u) lie in the closure of that atom by the realization construction. Its closure still has diameter at most 2^{-k}, so d(Yn(u),Y(u))2k for all such n. Letting k increase proves the asserted almost-sure convergence.

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