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Fixed-temperature generalized Bayes updates are sequentially coherent

Statement

Let π0 be a probability prior on the parameter space of Generalized Bayes loss update and temperature, let w>0 be fixed, and let x1,…,xn be any finite sequence of observations with measurable real loss sections ℓi(θ):=ℓ(θ,xi). Set πi:=Gw,πi−1,xi recursively, and assume each sequential normalizer zi:=∫e−wℓi(θ) πi−1(dθ) is finite and positive. Then, for every measurable A, πn(A)=∫Ae−w∑i=1nℓi(θ) π0(dθ)∫e−w∑i=1nℓi(θ) π0(dθ),∫e−w∑i=1nℓi(θ) π0(dθ)=∏i=1nzi. For n=0, the empty sum is zero, the empty product is one, and πn=π0. Thus sequential updating at a fixed temperature agrees with one update using the sum of the observed losses. No independence or sampling-model assumption is asserted.

Facts & Assumptions

Given: A probability prior π0, a fixed temperature w>0, measurable real loss sections ℓ1,…,ℓn, and finite-positive sequential normalizers zi.

[F1]

Generalized Bayes loss update and temperature: when a prior, observation, temperature, and finite-positive normalizer are supplied, Gw,π,x(A)=Zw(π,x)−1∫Ae−wℓx dπ.

[F2]

A finite-normalizer loss update is a probability measure: each such update is a probability measure.

[F3]

Integrating against a density agrees with integrating the product: for nonnegative measurable f,g, ∫g d(f dπ)=∫gf dπ.

[F4]

Probability measures and probability spaces: a probability measure is a measure of total mass one.

[F5]

The measure with density f relative to μ: f dπ is the measure A↦∫Af dπ for a nonnegative measurable f.

[F6]

The principle of mathematical induction: if a property holds at a natural number and each case implies the next, it holds for every later natural number.

[F7]

Arithmetic and lattice operations preserve measurability whenever they are defined: sums and real scalar multiples of measurable real functions are measurable.

[F9]

The real exponential function and the number e by a power series: the power series definition gives e0=1.

Proof

1.1F9F4givenalgebra

For n=0, the cumulative loss is the empty sum zero. In the power series definition [F9] at zero, the zeroth term is 1 and every positive-degree term vanishes, so its exponential weight is 1. By [F4], ∫1 dπ0=π0(Θ)=1. Thus the empty normalizer is the empty product one and the displayed formula is π0(A)=π0(A).

1.2F1F2givenbase

For n=1, the claim is exactly the update definition [F1], with z1=∫e−wℓ1 dπ0. This normalizer is finite positive by hypothesis, so the update is a probability by [F2].

1.3F7F1F8F3F5givenih

For n≥2, suppose the formula holds at n−1, with cumulative normalizer cn−1=∏i=1n−1zi and density fn−1(θ)=e−w∑i=1n−1ℓi(θ) relative to π0. The finite cumulative loss is measurable by repeated use of [F7], so [F1] gives measurability of fn−1 and of e−wℓn. Algebra and [F8] factor the cumulative exponential into fn−1e−wℓn. Then [F3] gives zn=∫e−wℓn dπn−1=cn−1−1∫e−w∑i=1nℓi dπ0. Thus the cumulative normalizer is cn=cn−1zn=∏i=1nzi, which is finite and positive.

2.1F1F3F8F7step 1.3algebra

By [F1], [F3], and the same factorization [F8], for every measurable A, πn(A)=zn−1∫Ae−wℓn dπn−1=cn−1∫Ae−w∑i=1nℓi dπ0. This proves the induction step.

3.1step 1.2step 1.3step 2.1F6step 1.1F4F2discharge-induction: step 2.1∎

Define Q(m) to be the claimed formula at n=m+1. Step 1.2 proves Q(0). For any m∈N, set n=m+2≥2; steps 1.3–2.1 prove that the formula at n−1=m+1 implies it at n=m+2, hence Q(m) implies Q(m+1). Therefore [F6] gives the formula for every n≥1; step 1.1 covers n=0. The initial π0 is a probability by [F4], and every later πi is a probability by [F2]. The proof uses only fixed-temperature updates and the stated normalizers.

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