Alphabeta Math
ExampleConstruction: AI-adaptedVerification: AI-adaptedPipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-09
How statement and proof provenance work

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.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Weighted counting in dimension zero

Example

A Hausdorff second-countable zero-manifold M is countable and discrete. For any weights w(p)[0,] its density measure is μw(A)=pAw(p)(AM). Finite positive weights give a Radon measure. On N={0,1,}, weights 2k1 give total mass one, while weights one give infinite total mass.

Facts & Assumptions

Given: Assume ACω. Manifolds are Hausdorff, second countable and smooth, with boundary allowed; n=0 is allowed unless excluded. Densities are pointwise Borel, 0=0, and λ0(R0)=1. Zero-dimensional weighted counting with two explicit total-mass series.

[F1]

Pointwise Borel nonnegative densities: A zero-dimensional chart is a singleton with coordinate mass one and determinant one.

[F2]

Intrinsic density measure and its chart restriction: The chart restriction of the density measure is its coefficient integral.

[F3]

Positive smooth densities give Radon volume: Positive finite smooth densities define Radon measures.

Verification

1.1

Each point has an open singleton chart, so M is discrete and every subset is Borel. Fix a countable base (Bj). For each p the base contains {p}; assigning the least such index injects M into N. Thus M is countable without selecting a chart for each point. Singleton indicators form a locally finite smooth partition in dimension zero.

F1given
2.1

The singleton chart integral is μw({p})=w(p)λ0(R0)=w(p). Countable additivity on the disjoint singleton decomposition of any A gives μw(A)=pAw(p). The empty sum is zero; zero or infinite weights cause no cancellation.

F1F2step 1.1
3.1

A compact subset of a discrete space is finite, since its singleton cover has a finite subcover. Every scalar function here is smooth in local zero-dimensional coordinates. Thus finite positive weights satisfy the positive smooth density theorem and give a Radon measure; directly, compact masses are finite sums, and every set is open and approximated in measure by its finite subsets.

F3step 1.1step 2.1
4.1

For M=N and w(k)=2k1, the partial sum through k=N1 is 12N, which tends to one. For w(k)=1 the same partial sum is N, hence the total mass is infinite. In the one-point case the formula gives precisely its weight.

step 2.1step 3.1

Depends on

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Sources