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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.

An improper flat-prior scale makes a formal evidence arbitrary

Example

Consider one observation Y from the normal location model Y∣θ∼N(θ,σ2) with known σ2>0. For any c>0, the measure Πc(dθ)=c λ(dθ) is an improper flat prior, where λ is Lebesgue measure (Lebesgue measurable sets, the family L(Rn), and the restricted set function λn). The likelihood integral against it is finite but equals c. If two competing models use this same normal-location likelihood, with the same observed y and known variance, but use independent arbitrary constants c1 and c2, their formal evidence ratio is c2/c1, so it has no value determined by the models.

Facts & Assumptions

Given: A normal location likelihood with σ2>0, an observation y∈R, and the sigma-finite prior measure c dθ for c>0.

[A1]

AC is assumed for the library normal-law convention. The Axiom of Choice

[F1]

A proper-model evidence in this pair is defined by integrating a specified likelihood density against a probability prior. Marginal likelihoods, proper model evidence, and Bayes factors

[F2]

The BCS-02 fiberwise normalizer is the likelihood integral against the supplied sigma-finite prior measure; an improper prior has infinite total mass. Evidence normalizer and fiberwise posterior update

[F3]

AC implies Countable Choice. AC implies DC implies countable choice

[F4]

Under Countable Choice, Lebesgue measure is sigma-finite and finite on bounded sets. Lebesgue measure is sigma-finite, and every metrically bounded subset of Rn has finite outer measure

[F6]

For σ>0, the normal location likelihood density is (2πσ2)−1/2exp⁡(−(y−θ)2/(2σ2)). A positive-variance normal law has its location-scale density

Verification

Given: The model and prior measure in the Example.

1.1A1F1F2F3F4F5F6givenalgebra

By [A1, F3, F4], λ is sigma-finite, so Πc=cλ is sigma-finite. By [F5], Πc([−n,n])=2cn for every positive integer n, hence Πc(R)=+∞ and it is improper in the sense of [F2]. By [F6], its formal likelihood integral is ∫Rc2πσ2exp⁡ ⁣(−(y−θ)22σ2)dθ. The substitution z=(y−θ)/σ has absolute Jacobian σ, so this equals c∫R(2π)−1/2e−z2/2 dz=c. This value is positive and finite for every fixed c>0, but Πc(R)=+∞, so it is not an evidence under [F1].

2.1F1F2step 1.1algebra∎

For the two copies of the same normal-location likelihood specified above, with model-specific constants c1,c2>0, the formal ratio is c2/c1 by step 1.1. Rescaling either improper prior changes this ratio arbitrarily while leaving its unnormalized density proportional to Lebesgue measure; hence no generic Bayes factor is defined by these improper priors.

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