Alphabeta Math
ExampleConstruction: AI-generatedVerification: AI-generatedPipeline-generatedprecheck pass
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.

Point-null mass under atomic and continuous priors

Example

Let M0 have parameter space Θ0={0} and prior Π0=δ0, and let M1 have parameter space Θ1=[0,1] and uniform prior Π1=λ∣[0,1]. Use the common data space Y={0,1} with counting measure μ, and specify the jointly measurable Bernoulli density on each parameter space by fi(θ,0)=1−θ and fi(θ,1)=θ. Give the models prior weights w0,w1>0 with w0+w1=1. After observing y=0, model M0 has positive posterior probability because it is an explicit model atom with positive prior weight. A single continuous prior on [0,1] instead assigns θ=0 probability zero.

Facts & Assumptions

Given: The two-model setup in the Example and observed value y=0.

[A1]

Countable Choice is assumed for the Lebesgue-volume formula used to compute interval and singleton measures. The Axiom of Countable Choice (ACω)

[F1]

For finitely many models with positive weights and finite positive evidences, posterior model probabilities are proportional to weight times evidence. Finite-model posterior probabilities and Bayes-factor odds

[F2]

Evidence under a proper parameter prior is the integral of the specified likelihood density against that prior. Marginal likelihoods, proper model evidence, and Bayes factors

[F4]

On R, Lebesgue measure λ is the restriction of Lebesgue outer measure to the Lebesgue measurable sets. Lebesgue measurable sets, the family L(Rn), and the restricted set function λn

Verification

Given: The models, weights, and observation in the Example.

1.1A1F1F2F3givenalgebra

By [A1, F3], λ([0,1])=1, so the uniform prior is proper. Under M0, m0(0)=1. Under M1, its density is 1 on [0,1], so m1(0)=∫01(1−θ) dθ=1/2. Both evidences are finite and positive, and [F1] gives Pr⁡(M0∣y=0)=w0/(w0+w1/2)>0.

2.1A1F3F4step 1.1algebra∎

By [F3], the degenerate closed interval [0,0]={0} is Lebesgue measurable and has measure zero; [F4] identifies this measure as λ. Thus the uniform prior assigns the singleton mass ∫{0}1 dλ=0. The separate model atom in step 1.1 instead gives θ=0 prior weight w0 and positive posterior probability.

Depends on

Used by

Nothing in the library uses this result yet.

Dependency tree · two levels

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Sources