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IID posterior contraction by entropy and prior mass

Statement

Let (X,A,μ) be a sample space with a fixed sigma-finite dominating measure. Let (Θ,T) be a measurable parameter space with prior probability measure Π, and let pθ be finite-valued probability densities relative to μ such that (θ,x)↦pθ(x) is jointly measurable. Let p0 be a true density relative to μ, and observe X1,…,Xn IID from P0, the law with density p0. Assume AC for the imported directional KL convention (The Axiom of Choice). The joint density family is explicit input; no arbitrary-index selection of versions is performed in this theorem.

Choose one metric d for both the entropy and conclusion: the root-L2 Hellinger distance h of Root-L2 Hellinger distance between density laws, the full density distance d1(p,q)=∫∣p−q∣ dμ, or the density distance d2(p,q)=(∫∣p−q∣2 dμ)1/2. In the d2 case assume one finite constant B bounds p0 and every density pθ in the model by B μ-almost everywhere. For each n, let Θn∈T be a nonempty measurable parameter sieve and put Fn:={pθ:θ∈Θn}. Assume θ↦d(pθ,p0) is measurable; this follows from the jointly measurable density family by integration of the relevant nonnegative distance integrands. Let D(r,Fn,d) be the packing number defined in Sieve metric entropy produces uniform exponential tests. Suppose C>0, ϵn>0, ϵn→0, nϵn2→∞, and log⁡D(ϵn,Fn,d)≤nϵn2,Π(Θnc)≤e−(C+4)nϵn2, while Π ⁣{θ:KL(P0∥Pθ)≤ϵn2,∫[log⁡pθp0]2p0 dμ≤ϵn2}≥e−Cnϵn2. Here KL(P0∥Pθ) has the directional convention of Kullback–Leibler divergence. In the log-square integral, set the weighted integrand to zero on {p0=0}; on {p0>0,pθ=0} the log ratio is −∞ and its square is +∞, as in KL prior mass gives a posterior denominator lower bound in probability. Define the data-indexed posterior by normalizing ∏ipθ(Xi) against Π on fibers with finite positive evidence. Then for all sufficiently large fixed M, the posterior contracts outside the Mϵn-ball in the selected metric: Π{θ:d(pθ,p0)>Mϵn∣X1,…,Xn}⟶0 in P0n-probability.

For d=d1, the radius is in the full density L1 norm; by Hellinger distance is a metric and controls L1 and total variation, d1=2∥P−Q∥TV under the library event-supremum convention. The theorem asserts only convergence in probability and gives no automatic almost-sure or minimax-optimality conclusion.

Facts & Assumptions

Given: A sigma-finite dominated IID density model with a jointly measurable density evaluation map, a prior Π, a true finite-valued density p0, measurable parameter sieves Θn, their density images Fn, and the displayed entropy, sieve-tail, and local prior-mass conditions.

[A1]

Assume the Axiom of Choice The Axiom of Choice for the imported directional KL convention Kullback–Leibler divergence. The jointly measurable density family is explicitly supplied, so no arbitrary-index selection of these versions is used.

[F1]

KL prior mass gives a posterior denominator lower bound in probability: the local KL/log-square mass condition gives Dn≥e−(C+2)nϵn2 with probability at least 1−1/(nϵn2).

[F2]

Sieve metric entropy produces uniform exponential tests: under the same metric entropy condition on Fn, tests exist with null error at most 2e−(cdM2−1)nϵn2 and error at most e−cdM2nϵn2 for every density in Fn outside the Mϵn-ball.

[F3]

Tonelli's theorem for nonnegative measurable functions on a sigma-finite product: nonnegative product-measurable functions have measurable section integrals and may be integrated in either order on sigma-finite product spaces.

[F4]

Expectations factor over finite products of independent random variables: for IID observations, expectations of finite products of nonnegative one-observation functions factor.

[F5]

Markov's inequality for random variables: for a nonnegative random variable Y and a>0, P(Y>a)≤E[Y]/a.

[F6]

Arithmetic and lattice operations preserve measurability whenever they are defined and Composition with a Borel measurable outer map preserves measurability: arithmetic operations and Borel functions of jointly measurable density maps preserve product measurability, including absolute values, squares, and square roots.

[F7]

Monotonicity and nonnegative homogeneity of the nonnegative integral and Additivity of the nonnegative Lebesgue integral: the nonnegative integral preserves order, is additive, and is homogeneous under positive finite scalars.

[F8]

Independent random elements have product joint law: a finite IID sample has the product joint law. For the supplied one-observation density pθ, Tonelli and The measure with density f relative to μ show that ∏ipθ(xi) defines its product-law density relative to μn: the two measures agree on measurable rectangles, and Measures agreeing on a generating pi-system are equal under an increasing finite-measure exhaustion from that pi-system identifies them on the product sigma-algebra The product sigma-algebra and its finite iterates.

Proof

1.1A1F1given

On the P0n-full event where 0<∏ip0(Xi)<∞, set Rn(θ):=∏i=1npθ(Xi)/p0(Xi) and Dn:=∫Rn(θ) Π(dθ). By [F1], on an event Ωn with P0n(Ωnc)≤1/(nϵn2), the scaled denominator Dn is finite and at least e−(C+2)nϵn2. The evidence ∫∏ipθ(Xi)Π(dθ)=Dn∏ip0(Xi) is therefore finite and positive, and on this event the posterior is the quotient of these likelihood integrals.

1.2F2F3F6F7givenchoose

Joint measurability of pθ and the arithmetic/Borel-composition rules [F6] make each nonnegative distance integrand ∣pθ−p0∣, ∣pθ−p0∣2, or (pθ−p0)2 product-measurable. Tonelli [F3] therefore gives measurability of θ↦d(pθ,p0). Its values are finite: the Hellinger bound follows from the definition remark, d1≤2 follows from ∣pθ−p0∣≤pθ+p0 and [F7], and in the d2 case [F7] and the uniform bound give d22≤∫(pθ+p0)2dμ≤2B∫(pθ+p0)dμ=4B. Thus An is measurable. Apply [F2] with the selected metric and choose M large enough that cdM2≥C+4. The resulting test ϕn has P0n(ϕn=1)→0 and error at most e−cdM2nϵn2 for every θ∈Θn with d(pθ,p0)>Mϵn.

1.3F2F3F6F8given

Put An:={θ:d(pθ,p0)>Mϵn}, Nn:=∫An∩ΘnRn(θ) Π(dθ) and Tn:=∫An∩ΘncRn(θ) Π(dθ). The piecewise likelihood ratio is jointly measurable: on the measurable set where p0>0 it is a Borel function of (pθ,p0), and it is zero where p0=0, by [F6]. Thus the product-density identity [F8], joint measurability, and Tonelli [F3] give EP0n[(1−ϕn)Nn]≤∫An∩ΘnPθn(1−ϕn) Π(dθ)≤e−cdM2nϵn2. The first inequality allows Pθ to put mass outside the support of P0, since the likelihood-ratio integral then contains only the P0-support and is no larger than the full Pθn probability.

1.4F3F4givenalgebra

For every fixed θ, EP0[pθ(X1)/p0(X1)]=∫{p0>0}pθ dμ≤1. Independence and [F4] therefore give EP0nRn(θ)≤1. Tonelli [F3] and the sieve-tail premise yield EP0nTn≤Π(Θnc)≤e−(C+4)nϵn2.

2.1F1F2F3F5step 1.1step 1.2step 1.3step 1.4algebra∎

Fix δ>0. On Ωn∩{ϕn=0}, posterior mass Π(An∣Xn)>δ implies (1−ϕn)(Nn+Tn)>δe−(C+2)nϵn2. Markov's inequality [F5], step 1.1, and [F2]–[F3] give P0n{Π(An∣Xn)>δ}≤1nϵn2+2e−(cdM2−1)nϵn2+e(C+2)nϵn2δ(e−cdM2nϵn2+e−(C+4)nϵn2). By the choice cdM2≥C+4 and nϵn2→∞, the right side tends to zero. Since this holds for every δ>0, the posterior mass outside the stated ball converges to zero in P0n-probability.

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