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Posterior kernel and dominated formula for a latent Gibbs observation
Statement
Assume the Axiom of Choice. Let the parameter and data spaces and of a finite latent Gibbs observation model both be standard Borel, and let be its proper prior. Let be the joint prior-predictive probability determined by and the marginal sampling kernel , and let be its data marginal. There exists a data-indexed probability kernel satisfying and any two such posterior kernels agree as probability measures for -almost every .
In the dominated case with data measure and joint likelihood density from the Definition, define Then is measurable, , and for -almost every with the posterior has the version The prior-predictive law gives zero mass to the set where or ; the conditional identities do not determine pointwise posterior values there.
Statement references
Facts & Assumptions
Given: A proper prior , the measurable canonical-parameter map and finite latent Gibbs sampling kernel in the Definition, standard-Borel parameter and data spaces, AC, and, for the dominated clause, a sigma-finite measure and jointly measurable normalized density .
The Axiom of Choice: every family of nonempty sets has a choice function; AC is an explicit hypothesis of the posterior-kernel result used below.
Finite latent Gibbs observation model: summing the finite latent state law with weights against the observation kernel gives a parameter-measurable probability kernel ; in the dominated case the finite sum is its joint likelihood density.
Standard Borel spaces: a measurable space is standard Borel when it is measurably isomorphic to the Borel space of a Polish topology; both parameter and data measurable structures are assumed to have this property.
Standard-Borel Bayesian posterior kernel exists: under AC, a proper prior and parameter-measurable probability kernel on standard-Borel parameter and data spaces give a data-indexed posterior probability kernel satisfying the rectangle identity, unique as a probability measure outside one data-marginal null set.
Tonelli's theorem for nonnegative measurable functions on a sigma-finite product: for a nonnegative product-measurable function on two sigma-finite measure spaces, section integrals are measurable and either iterated integral equals the product integral.
Measure kernel and probability kernel: a probability kernel is a measurable family of probability measures, with total mass one at every source point.
Proof
Given: The hypotheses and notation in the Statement.
By [F1], the prior and form a proper Bayesian model. The parameter and data spaces are standard Borel by [F2], and AC holds by [A1]. Therefore [F3] supplies the posterior probability kernel and its -almost-everywhere uniqueness, with the exact rectangle identity in the Statement.
In the dominated case, is nonnegative and jointly measurable by its finite-sum definition. The prior is finite and hence sigma-finite; is sigma-finite by the Definition. Apply [F4] to on their product. It gives measurability of and . For each , the same calculation with gives . Here the finite sum and each normalized observation density are those of [F1].
The set has -measure zero because has integral one, and the set has zero data-marginal mass because by step 1.2. For each , the numerator is measurable by [F4]. Define when , and set otherwise. On valid , the measure induced on by the nonnegative density with respect to has total mass , so after division it is a probability measure; on the exceptional set it is the prior. Thus each section is a probability measure, and its evaluations are measurable, so it is a probability kernel by [F5].
For every and , Tonelli and the data-marginal density established in step 1.2 give ; the exceptional values contribute zero because their -measure is zero. Thus the displayed ratio is a posterior version on its stated domain, and the general uniqueness assertion remains only -almost everywhere.
Remarks
The prior is part of this mathematical model, and the posterior is conditional on it and on the stated likelihood kernel. This theorem proves neither posterior concentration nor computational efficiency. It does not report data or establish that any Gibbs model describes a physical system.