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The unit-temperature likelihood update is ordinary Bayes in a finite model
Example
Let have prior masses and . Let the observation space be and define sampling laws by , , , and . These finite spaces with power-set sigma-algebras are standard Borel, and the displayed laws define a statistical experiment. Take for every . For observed at , the unnormalized masses are and , so the update is . The same values follow by conditioning the joint prior-sampling law on .
Facts & Assumptions
Given: The parameter and observation spaces with power-set sigma-algebras, prior , and the four displayed sampling probabilities.
A countable discrete measurable space is standard Borel: a nonempty at-most-countable set with its power-set sigma-algebra is standard Borel.
Probability measures and probability spaces: a probability measure has total mass one.
Statistical experiments: a statistical experiment consists of a sample measurable space, a parameter set, and a probability law on the sample space for each parameter.
Generalized Bayes loss update and temperature: at the update weights are proportional to and are normalized by their integral against the prior.
A finite-normalizer loss update is a probability measure: a finite-positive-normalizer update is a probability measure.
The natural logarithm as the inverse of the exponential function: is the inverse of on .
Conditional probability for : in a finite probability space, when .
Verification
Both parameter and sample spaces are nonempty finite sets, so [F1] makes them standard Borel. The prior masses are nonnegative and sum to one; each pair of sampling probabilities is nonnegative and sums to one. By [F2] these are probability measures, and [F3] therefore gives the stated finite statistical experiment.
All four likelihoods are positive, so [F6] makes real-valued on . Each parameter section is measurable because the parameter sigma-algebra is the power set, satisfying the loss hypotheses of [F4] for every . At , the inverse relation in [F6] gives . Hence the unnormalized weights are and their normalizer is , finite and positive.
By [F4]–[F5], the update is a probability measure with .
Define the joint masses by . The four masses are at , respectively; they sum to one, and . Applying [F7] to each parameter singleton gives Thus the loss update equals the ordinary finite-model posterior at .
Depends on
- Conditional probability $\mathbb P(A\mid B)$ for $\mathbb P(B)>0$
- Generalized Bayes loss update and temperature
- The natural logarithm as the inverse of the exponential function
- Probability measures and probability spaces
- Statistical experiments
- A countable discrete measurable space is standard Borel
- A finite-normalizer loss update is a probability measure
Used by
Nothing in the library uses this result yet.
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Sources
- P. G. Bissiri, C. C. Holmes, and S. G. Walker, A general framework for updating belief distributions, JRSS B 78(5), 2016 (standard reference, not scraped)
- J. Knoblauch, J. Jewson, and T. Damoulas, An Optimization-centric View on Bayes’ Rule: Reviewing and Generalizing Variational Inference, JMLR 23(132), 2022 (standard reference, not scraped)