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Linear-functional BvM limit and credible-interval calibration

Statement

Use the product-prior white-noise model and supplied posterior kernel of Weak nonparametric Bernstein–von Mises theorem for product priors, including its wavelet-basis, coefficient-density, truth, and countable-choice hypotheses. Let g∈H2s for some s>1/2, with g≠0, and put σg=∥g∥2. Let Qn be the posterior law of Lg(f) and let Cn,α=[qα/2(Qn),q1−α/2(Qn)],0<α<1. Then βBL,R ⁣(Qn∘[u↦n(u−Lg(X(n)))]−1,N(0,σg2))⟶0 in Pf0(n)-probability. The interval Cn,α is posterior credible at level 1−α, and its frequentist coverage satisfies Pf0(n){Lg(f0)∈Cn,α}⟶1−α.

Facts & Assumptions

Given: The white-noise experiment, product prior, posterior kernel, basis, density and truth assumptions of Weak nonparametric Bernstein–von Mises theorem for product priors, together with g≠0, g∈H2s, s>1/2, and 0<α<1.

[F1]

Weak nonparametric Bernstein–von Mises theorem for product priors: for every δ>1/2, the posterior law of n(f−X(n)) converges in bounded-Lipschitz distance in H(δ) to the canonical white-noise law N in Pf0(n)-probability. Its product-prior construction requires countable choice; the same axiom suffices for the scalar density-normal interface.

[F2]

Smooth functionals extend continuously to the white-noise topology: Lg is a continuous linear functional on H(δ) and agrees with f↦⟨f,g⟩L2 on L2.

[F3]

White noise is a Borel Gaussian law on the negative Sobolev space: the canonical law N is centered Gaussian on H(δ); for the coefficient pairing Lg, its variance is ∑l,k∣glk∣2=∥g∥22.

[F4]

Posterior quantiles stabilize under scalar weak convergence: bounded-Lipschitz convergence in probability to a law with continuous CDF locally strictly increasing at an interior quantile implies convergence in probability of that posterior quantile.

[F5]

Equal-tailed posterior quantile intervals are credible: the equal-tailed interval between posterior quantiles qα/2 and q1−α/2 is graph-measurable and has posterior mass at least 1−α.

[F6]

Density normal laws and square-summable Gaussian series under countable choice: Under countable choice, in its density convention, N(0,1) is defined by its continuous positive density, and N(0,σ2) for σ>0 is its image under x↦σx; change of variables gives a continuous strictly positive density and hence a continuous strictly increasing CDF.

[A1]

The Axiom of Countable Choice (ACω): countable choice is inherited through [F1] for the L2 product-prior construction and also suffices for the density normal-law interface [F6]; no full choice is used below.

Proof

1.1A1F1F2F3algebra

Fix δ>1/2. For every bounded 1-Lipschitz function h:R→R, the composition h∘Lg is bounded by 1 and has Lipschitz constant at most ∥Lg∥H(δ)∗. Rescaling by cg=max⁡(1,∥Lg∥H(δ)∗) makes it an admissible bounded-Lipschitz test on H(δ). Hence the scalar pushforward distance is at most cg times the distance in [F1]. The pushforward of N is N(0,σg2) by [F3], proving the asserted scalar BvM limit.

2.1F4F5F6step 1.1algebra

Translate the posterior law of Lg(f) by Lg(X(n)) and scale by n. By [F4] and the continuous strictly increasing normal CDF from [F6], the two quantiles of this scaled law converge in probability to σgzα/2 and σgz1−α/2, where zu is the u-quantile of N(0,1). Since the affine map is increasing, these are exactly the scaled endpoints of Cn,α−Lg(X(n)). The interval is credible by [F5].

3.1F3F6step 2.1algebra

Under the true white-noise law, n{Lg(X(n))−Lg(f0)}=Lg(W) has exactly the centered normal law N(0,σg2) by [F3]. On the event that both random scaled endpoints in step 2.1 lie within ε of their limits, the event Lg(f0)∈Cn,α is bounded between the corresponding deterministic normal-interval events with endpoints enlarged or contracted by ε. This sandwich uses no independence between the endpoints and the observation. The endpoint event has probability tending to one, and [F6] makes the normal mass of shrinking neighborhoods of the two endpoints tend to zero.

4.1F6step 3.1algebra∎

Letting n→∞ and then ε↓0 in the sandwich of step 3.1 gives limiting coverage Φ(z1−α/2)−Φ(zα/2)=1−α by the definition of the normal quantiles and CDF in [F6].

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