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.
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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 is countable and discrete. For any weights its density measure is Finite positive weights give a Radon measure. On , weights give total mass one, while weights one give infinite total mass.
Facts & Assumptions
Given: Assume . Manifolds are Hausdorff, second countable and smooth, with boundary allowed; is allowed unless excluded. Densities are pointwise Borel, , and . Zero-dimensional weighted counting with two explicit total-mass series.
Pointwise Borel nonnegative densities: A zero-dimensional chart is a singleton with coordinate mass one and determinant one.
Intrinsic density measure and its chart restriction: The chart restriction of the density measure is its coefficient integral.
Positive smooth densities give Radon volume: Positive finite smooth densities define Radon measures.
Verification
Each point has an open singleton chart, so M is discrete and every subset is Borel. Fix a countable base . For each the base contains ; assigning the least such index injects M into . Thus M is countable without selecting a chart for each point. Singleton indicators form a locally finite smooth partition in dimension zero.
The singleton chart integral is . Countable additivity on the disjoint singleton decomposition of any A gives . The empty sum is zero; zero or infinite weights cause no cancellation.
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.
For and , the partial sum through is , which tends to one. For the same partial sum is N, hence the total mass is infinite. In the one-point case the formula gives precisely its weight.
Depends on
Used by
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Dependency tree · two levels
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Sources
- Folland, Real Analysis, second edition, §11.4 pp.361–363; Theorems 2.14–2.15 pp.50–51 (standard reference, not scraped)