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A degenerate GP concentration function does not bound unknown-scale prior mass

Statement

Let W≡0, w0=0, and let its covariance RKHS be H={0}. Define ϕ0(ϵ)=inf⁡h∈H, ∣h−w0∣<ϵ{∥h∥H2}−log⁡Pr⁡(∣W∣<ϵ). For n large, set ϵn=log⁡log⁡n/n and take an independent σ∼Unif⁡[1/2,3/2] with true value σ0=1. Then ϕ0(ϵn)=0, ϵn→0, and nϵn2→∞, but −log⁡Pr⁡(∣σ−σ0∣<ϵn)≠O(nϵn2). Thus the Gaussian concentration condition alone does not verify the joint local prior-mass bound used by the denominator argument for the unknown-scale branch. This calculation is a proof-gap example, not a posterior counterexample.

Facts & Assumptions

Given: The point-mass Gaussian prior, the displayed rate sequence, and the independent uniform scale prior.

[F1]

The natural logarithm has derivative 1/x and equals the integral from 1 to x of 1/t: log⁡x=∫1xdt/t and, for x≥1, log⁡x≤2x.

Verification

1.1givenalgebra

The RKHS of the point-mass prior is {0}; its approximation cost at w0=0 is zero. Also Pr⁡(∣W∣<ϵ)=1 for every ϵ>0, so the explicitly defined concentration function satisfies ϕ0(ϵ)=0.

1.2givenalgebra

For n sufficiently large, ϵn<1/2, hence the uniform prior assigns mass 2ϵn to (1−ϵn,1+ϵn). Therefore −log⁡(2ϵn)=12log⁡n−12log⁡log⁡log⁡n−log⁡2, while nϵn2=log⁡log⁡n. Along nm=⌈eem⌉, the first quantity grows on the order of em and the second on the order of m, so their ratio is unbounded.

2.1F1step 1.2given∎

Since log⁡log⁡n→∞ and log⁡log⁡n/n→0, the rate has nϵn2→∞ and ϵn→0 while the scale interval mass has negative logarithm not O(nϵn2) by step 1.2. Thus the Gaussian concentration condition does not establish this particular denominator-mass check; it does not establish failure of posterior contraction. Any separate posterior-contraction argument requires a specified sampling likelihood and its own hypotheses; a local bound on the scale-prior density alone is insufficient.

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