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LAN, Contiguity and Efficiency

1 · Prerequisites

2 · Summary

This page defines contiguity and pointwise LAN using mean-one likelihood proxies, then proves the matching-mean criterion for contiguity and Le Cam's third lemma. For dominated iid models, QMD yields LAN after the local alternative is restricted to the base-law support and normalized; the proof separately controls singular and zero-overlap mass, so it never asserts a full Radon–Nikodym derivative when one may not exist. The page also defines regularity under each fixed local alternative and proves the convolution bound under the stated LAN and regularity hypotheses.

The local asymptotic minimax theorem uses only pointwise LAN. Its proof passes through finite priors, approximates diffuse Gaussian Bayes values by finite-support priors, and approximates a bounded Borel bowl-shaped loss from below by bounded Lipschitz minorants. A separate posterior approximation lemma states an explicit compact-uniform likelihood-field condition; that stronger condition is not used by the minimax proof. Brunn–Minkowski and Gaussian centering are proved locally as supporting results.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Contiguous sequences of probability measures

Definition

Let (X,A) be one measurable space and let Pn,Qn be probability measures on it (Probability measures and probability spaces). The sequence (Qn) is contiguous with respect to (Pn), written Qn◃Pn, if for every sequence An∈A, Pn(An)⟶0⟹Qn(An)⟶0. The sequences are mutually contiguous, written Qn◃▹Pn, if both Qn◃Pn and Pn◃Qn.

Contiguity is a relation between sequences of laws, not absolute continuity at each finite n. It says that events negligible under one sequence remain negligible under the other in the indicated direction.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

The boundary of a convex set is Lebesgue null

Statement

Assume countable choice. For every convex set C⊆Rd, its topological boundary ∂C=C‾∖C∘ has d-dimensional Lebesgue measure zero. If C has empty interior, then C itself is contained in a proper affine subspace and is Lebesgue null.

Facts & Assumptions

Given: Countable choice, a finite integer d≥1, and a convex set C⊆Rd.

[A1]

The Axiom of Countable Choice (ACω): Countable choice permits the countable approximations used by the Lebesgue measure suppliers.

[F1]
[F2]

The geometric simplex spanned by affinely independent vertices, Every Euclidean linear map has a unique matrix and satisfies ∥Lh∥2≤K∥h∥2 for some K≥0, and The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn: Affine independence of c0,x1,…,xd means the differences xi−c0 are linearly independent. Their closed simplex contains the image of {ti>0:∑i=1dti<1} under t↦c0+∑iti(xi−c0). The linear part and its inverse are continuous, so this image is a nonempty open set; balls use the Euclidean norm.

[F4]

Measure of a set difference when the smaller set has finite measure and Measures are monotone: For nested measurable sets of finite measure, the measure of the difference is the difference of their measures, and measure is monotone.

[F5]

Finite and countable subadditivity of measures: A countable union of null measurable sets is null.

[F6]

A finite-dimensional normed subspace is closed and Lebesgue outer measure, Lebesgue measurability and Lebesgue measure are unchanged by translation: Finite-dimensional linear subspaces are closed, and translation preserves Lebesgue measurability and measure.

Proof

technique · affine-hull reduction and homothetic contraction
1.1F1F2F6givenchoosealgebra

If C=∅, the claim is immediate. Otherwise choose c0∈C and let W be the linear span of {x−c0:x∈C}. If W=Rd, finite-dimensional linear algebra selects d linearly independent differences xi−c0 from this spanning family. By definition these d+1 points are affinely independent; their simplex lies in C by convexity and contains a nonempty open set by [F2], contradicting empty interior. Thus W is proper and C⊆c0+W. By [F1], W is null; [F6] makes c0+W closed and null. Since C‾⊆c0+W, both C and its boundary are null. This proves the empty-interior case.

1.2A1givenalgebra

Suppose C has nonempty interior. Choose x0∈C∘ and ρ>0 with B(x0,ρ)⊆C. If y∈C‾ and 0<t<1, [A1] selects yj∈C with yj→y. Convexity gives B(x0+t(yj−x0),(1−t)ρ)⊆C. The centers converge to x0+t(y−x0), so that limit point has a ball of radius (1−t)ρ/2 contained in C. Therefore x0+t(C‾−x0)⊆C∘.

2.1F3F4F6F7step 1.2algebra

For each integer r large enough that Kr=C‾∩B‾(0,r) contains x0, [F7] makes Kr compact with finite measure. The contraction x0+t(Kr−x0) lies in C∘ by step 1.2 and in Kr by convexity. Write this contraction as tKr+(1−t)x0. Applying [F3] to tId and then translation invariance [F6] gives its measure as tdλd(Kr). Hence ∂C∩Kr⊆Kr∖(x0+t(Kr−x0)), and [F4] gives λd(∂C∩Kr)≤(1−td)λd(Kr). Let t↑1 to obtain λd(∂C∩Kr)=0.

3.1A1F5step 2.1∎

The bounded sets Kr cover C‾ as r ranges over sufficiently large integers. Therefore ∂C is a countable union of the null sets in step 2.1 and is null by [F5].

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Local asymptotic normality for local experiments

Definition

Let Pn,h be probability laws on a common measurable space for each integer n≥1 and local parameter h∈Rd, where d<∞ and Pn,0 is the base law. Suppose that for every fixed h we are supplied a nonnegative measurable function Ln,h with ∫Ln,h dPn,0=1. It defines an absolutely continuous proxy Pˉn,h(A):=∫ALn,h dPn,0. The actual local law is allowed to have a singular part; the approximation condition below is what connects it to this proxy.

The experiments are locally asymptotically normal (LAN) at h=0 with information matrix K and central sequence Δn if K is a symmetric positive semidefinite d×d matrix, Δn is an Rd-valued statistic, Δn⇒Nd(0,K)under Pn,0, and for every fixed h∈Rd, ∥Pn,h−Pˉn,h∥TV→0,log⁡Ln,h=hTΔn−12hTKh+oPn,0(1), where ∥⋅∥TV is the event-supremum total variation distance (Total variation distance for probability laws) and oPn,0(1) means convergence to zero in Pn,0-probability. We set log⁡0=−∞; the finite-valued expansion entails Pn,0(Ln,h=0)→0. Convergence in distribution is as in Convergence in distribution of random elements, and Nd(0,K) allows singular K (Multivariate normal law, including singular covariance).

If Pn,h=Pˉn,h, this is the usual dominated LAN comparison. The proxy formulation also covers QMD paths whose local alternatives are not absolutely continuous with respect to the base law, provided the singular product mass tends to zero in total variation. This definition is pointwise in each fixed h; it does not assert uniformity over bounded sets of h.

TheoremStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

Brunn–Minkowski inequality for compact convex sets

Statement

Assume countable choice. Let d≥1 and let A,B⊆Rd be nonempty compact convex sets. With A+B={a+b:a∈A,b∈B} and λd denoting Lebesgue measure, λd(A+B)1/d≥λd(A)1/d+λd(B)1/d. Zero-volume and lower-dimensional sets are included.

Facts & Assumptions

Given: Countable choice, an integer d≥1, and nonempty compact convex sets A,B⊆Rd.

[A1]

The Axiom of Countable Choice (ACω): Countable choice is sufficient for the Lebesgue-measure change-of-variables and Tonelli suppliers used here; full AC is not assumed.

[F1]

Lebesgue measurable sets, the family L(Rn), and the restricted set function λn: Lebesgue volume of a measurable set is its measure λd.

[F2]

Tonelli's theorem for nonnegative measurable functions on a sigma-finite product: For a nonnegative measurable function, integration over Rd equals iterated integration over its one-dimensional slices.

[F3]

The weighted arithmetic-geometric mean inequality for real weights: For positive x,y and 0≤λ≤1, (1−λ)+λx≥xλ.

[F4]

A C^1 diffeomorphism satisfies the change-of-variables formula for nonnegative Lebesgue measurable functions: For a C1 diffeomorphism of open sets, the nonnegative Lebesgue integral transforms with the absolute Jacobian.

[F7]

The first fundamental theorem: if f is integrable on [a,b] and continuous at c, then F′(c)=f(c); in particular a continuous f has F as a primitive and Derivative of an inverse: if f is continuous and injective on a nondegenerate interval I and differentiable at c∈I with f′(c)≠0, then the inverse g is differentiable at f(c) with g′(f(c))=1/f′(c); and if f′(c)=0 then g is not differentiable at f(c): On each compact interval inside a projection interval, the fundamental theorem gives the derivative of the cumulative integral as its continuous integrand. The inverse theorem then gives (FB−1)′(u)=1/g(FB−1(u)); this derivative is continuous because g is continuous and positive and FB−1 is continuous.

[F8]

Monotone convergence for the integral: Increasing nonnegative integrals converge to the integral of their pointwise limit.

[F9]

Lebesgue measure is sigma-finite, and every metrically bounded subset of Rn has finite outer measure: Every bounded measurable subset of Rd has finite Lebesgue measure.

[F10]

The boundary of a convex set is Lebesgue null: A convex set with empty interior has zero d-dimensional Lebesgue measure.

[F11]

Heine-Borel in Rn: with the Euclidean metric a subset of Rn is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line: Compact subsets of finite-dimensional Euclidean space are closed and bounded, and closed bounded subsets are compact. In particular, A×B is closed and bounded in R2d, hence compact; continuous images of compact sets are compact, so A+B, positive dilations of A and B, and every weighted convex sum used below are compact and convex (an open cover of the image pulls back to one of the compact domain, which has a finite subcover). When d≥2, for a compact C⊆R×Rd−1, each coordinate projection is compact (and is an interval when C is convex) and each slice Cz={y:(z,y)∈C} is closed and bounded, hence compact. Thus these bodies and slices are Borel and have well-defined finite Lebesgue volumes; applying [F2] to 1C makes z↦λd−1(Cz) measurable and gives its integral as λd(C).

Proof

Proof technique: induction on dimension using convex slices and a one-dimensional monotone transport.

1.1F1F6F9F11givenalgebra

If one of A,B has zero volume, say λd(A)=0, choose a∈A. By [F11], A+B is compact and measurable. Then a+B⊆A+B, so [F6] gives λd(A+B)≥λd(B); the stated inequality follows after taking dth roots. If both volumes vanish the right side is zero. Thus assume both volumes are positive.

2.1A1F1F5F9F11step 1.1givenalgebra

Put a=λd(A)1/d, b=λd(B)1/d, A′=a−1A, B′=b−1B, and λ=b/(a+b). By [F5], λd(A′)=λd(B′)=1; [F11] makes these dilates and their convex combinations compact. It suffices to show that every convex combination (1−λ)A′+λB′ has volume at least one, because A+B=(a+b)((1−λ)A′+λB′). The cases λ=0,1 are immediate, so take 0<λ<1 and rename A′,B′ as A,B.

3.1A1F1F2F9F10F11step 2.1givenbaseihinduction

We prove the normalized claim by induction on d. In dimension one, A and B are intervals of length one, so their convex combination is an interval of length (1−λ)+λ=1. Now let d≥2 and assume the normalized claim in dimension d−1. The normalization calculation in step 2.1 is dimension-independent, so this induction hypothesis also gives the full weighted inequality in dimension d−1 for positive-volume compact convex sets. By [F10], positive volume implies each body has nonempty interior and contains an interior ball. By [F11], their coordinate projections are compact intervals and their slices are compact and measurable; [F2] makes the slice-volume functions measurable. Project each convex body onto the first coordinate; its projection is a nondegenerate compact interval. For an interior coordinate x, let Ax⊆Rd−1 be its slice and f(x)=λd−1(Ax). Define By and g(y) likewise. These slice volumes are positive and finite in the open projection intervals. Write the projections as [a−,a+] and [b−,b+]. An interior ball in A has center with first coordinate x0. If a−<x<x0, choose p∈A with first coordinate p1<x and combine p with the ball centered at x0; the convex combination with weight λ=(x−p1)/(x0−p1)∈(0,1) on the ball lies in the slice at x and contains a (d−1)-ball of radius λρ>0. If x0<x<a+, choose p1>x and use weight (p1−x)/(p1−x0) on the interior ball. At x=x0, the original ball supplies a positive-radius slice. The same argument applies to B.

4.1F2F11step 3.1step 2.1inductionalgebra

Convexity gives A(1−t)x0+tx1⊇(1−t)Ax0+tAx1 for interior x0,x1. The compact slices in [F11] let the induction hypothesis apply to these sums. It therefore makes f1/(d−1) concave on the open projection interval; likewise g1/(d−1). To see continuity of ψ=f1/(d−1), fix an interior point x0 and a<x0<b in the interval. For x↓x0, concavity gives the chord lower bound ψ(x)≥b−xb−x0ψ(x0)+x−x0b−x0ψ(b). Writing x0=ηa+(1−η)x with η=(x−x0)/(x−a) gives the upper bound ψ(x)≤ψ(x0)−ηψ(a)1−η. Both bounds tend to ψ(x0); exchanging left and right proves continuity from the other side. Thus f,g are continuous and strictly positive on their open intervals. By [F2], ∫f=∫g=1.

5.1F6F7F9step 3.1step 2.1step 4.1algebra

Define the cumulative functions FA(x)=∫a−xf(t)dt and FB(y)=∫b−yg(t)dt on their projection intervals. Since A,B lie in bounded boxes, all their slices lie in one fixed bounded box in Rd−1; [F6, F9] therefore bound f,g uniformly. Their cumulative integrals consequently extend continuously to the projection endpoints with values zero and one, using ∫f=∫g=1 from step 4.1. Positivity of f,g on the open intervals makes FA,FB strictly increasing there, so they map those intervals onto (0,1). On every compact interior subinterval [F7] gives derivatives FA′=f and FB′=g. The inverse theorem then gives that φ=FB−1∘FA is C1 on the open interval and φ′(x)=f(x)/g(φ(x)). Let z(x)=(1−λ)x+λφ(x); then z′(x)=(1−λ)+λf(x)/g(φ(x))>0.

6.1F2F3F11step 5.1step 4.1step 2.1step 3.1inductionalgebra

Let C=(1−λ)A+λB, which is compact by [F11], and let cz be the (d−1)-dimensional volume of its compact slice at coordinate z. The slice-volume function is measurable by [F2] and [F11]. The slice of C at z(x) contains (1−λ)Ax+λBφ(x). The induction hypothesis yields cz(x)≥((1−λ)f(x)1/(d−1)+λg(φ(x))1/(d−1))d−1. Set r=g(φ(x))/f(x)>0. Multiplying this bound by z′(x) and using [F3] twice gives cz(x)z′(x)≥f(x)((1−λ)+λr1/(d−1))d−1((1−λ)+λ/r)≥f(x). The last inequality follows by applying [F3] to both positive brackets.

7.1F1F2F4F7F8F11step 6.1step 5.1step 4.1step 2.1step 3.1givenalgebra

Restrict x to an open interval J strictly inside (a−,a+). The map z is C1 with positive derivative by step 5.1, and [F7] makes it a C1 diffeomorphism onto its open image z(J). Thus [F4] and step 6.1 give λd(C)=∫czdz≥∫z(J)czdz=∫Jcz(x)z′(x)dx≥∫Jf(x)dx. Here cz is measurable and the equality is the one-dimensional change of variables. For all sufficiently large integers m, take Jm=(a−+1/m,a+−1/m); these intervals increase to (a−,a+). By [F8] and ∫f=1, λd(C)≥1. This proves the normalized claim in dimension d.

8.1F1step 1.1step 2.1step 3.1step 7.1algebradischarge-induction∎

The induction proves the normalized claim in every finite dimension. Undoing the normalization in step 2.1 gives λd(A+B)1/d≥a+b=λd(A)1/d+λd(B)1/d, including the zero-volume cases from step 1.1.

TheoremStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

A mean-one likelihood-ratio limit implies contiguity

Statement

For each n, let Pn,Qn be probability measures on one measurable space, and let Ln≥0 satisfy Qn(A)=∫ALn dPn for every measurable A. Suppose EPnLn=1, Ln⇒L under Pn, L≥0, and EL=1. Then (Qn) is contiguous with respect to (Pn).

Facts & Assumptions

Given: Probability measures Pn,Qn, mean-one densities Ln, and the stated nonnegative distributional limit L with matching mean.

[F1]

Contiguous sequences of probability measures: Qn◃Pn means Pn(An)→0 implies Qn(An)→0 for every event sequence An.

[F2]

Convergence in distribution of random elements: Ln⇒L means expectations converge for every bounded continuous function.

Proof

technique · direct uniform-integrability argument
1.1F2givenalgebra

For fixed M>0, x↦x∧M is bounded and continuous on [0,∞), so [F2] and the mean assumptions give E(Ln−M)+=ELn−E(Ln∧M)⟶EL−E(L∧M)=E(L−M)+.

2.1step 1.1givenalgebra

If x>2M, then x≤2(x−M); hence lim sup⁡nE[Ln1{Ln>2M}]≤2E(L−M)+. The right side tends to zero as M→∞ because L is integrable. Each of the finitely many initial integrable Ln also has vanishing tail integral, so (Ln) is uniformly integrable.

3.1F1F2step 2.1givenalgebra∎

For any event sequence An and any M>0, Qn(An)=E[Ln1An]≤MPn(An)+E[Ln1{Ln>M}]. If Pn(An)→0, the first term tends to zero for fixed M, and uniform integrability makes the limsup of the second term arbitrarily small as M→∞. Thus Qn(An)→0, which is Qn◃Pn by [F1].

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Regular estimator under local alternatives

Definition

In a local experiment {Pn,h:h∈Rd} at h=0 (Local asymptotic normality for local experiments), let Tn be an Rd-valued statistic. It is regular at zero with limit law W if, for every fixed h∈Rd, Tn−h⇒Wunder Pn,h, where the same probability law W works for all h. In a parametric model with true parameter θ0, this is the definition for Tn=n(θ^n−θ0) and local laws at θ0+h/n; equivalently the centered error n(θ^n−θ0−h/n) has a limit independent of the fixed local displacement h.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Compact-uniform LAN approximates compact-prior posteriors

Statement

Assume AC.

Let H⊂Rd be compact, let π be a probability measure on H, and let Pn,0 be base laws. Suppose Ln(h,x) is jointly measurable in (h,x), nonnegative, and satisfies ∫Ln(h,x)Pn,0(dx)=1 for every h∈H. Let Δn⇒Z∼Nd(0,K) under Pn,0, where K is positive semidefinite, and put gh(z)=exp⁡(hTz−12hTKh). Assume the random variable an(x):=sup⁡h∈H∣Ln(h,x)−gh(Δn(x))∣ is measurable and EPn,0an→0. Let the prior-predictive law be Mn(dx)=mn(x)Pn,0(dx) with mn(x)=∫HLn(h,x)π(dh), and define posteriors Πn(dh∣x)=Ln(h,x)π(dh)mn(x),ΠG(dh∣z)=gh(z)π(dh)m(z),m(z)=∫Hgh(z)π(dh), where an arbitrary probability measure is assigned if a denominator is zero. Then EMn∫H∣Ln(h,X)mn(X)−gh(Δn(X))m(Δn(X))∣π(dh)⟶0. In particular the posterior laws converge in expected total variation, because their event-probability differences are bounded by this L1(π) distance. The convention for total variation is Total variation distance for probability laws.

This lemma assumes an L1 uniform likelihood-field approximation. Pointwise LAN alone does not supply that hypothesis.

Facts & Assumptions

Given: AC; the compact set and prior, the mean-one likelihood field, the central sequence and its Gaussian limit, and the measurable L1 uniform approximation above.

[A1]

The Axiom of Choice: AC is assumed for the multivariate normal law.

[F1]

Convergence in distribution of random elements: Weak convergence of Δn gives convergence of expectations for bounded continuous functions.

[F2]

Dominated convergence: For a nonnegative integrable U, E(U−Q)+→0 as Q→∞, since (U−Q)+≤U.

[F3]

Multivariate normal law, including singular covariance and Standard normal and normal laws: For Z∼Nd(0,K), hTZ∼N(0,hTKh); completing the square in the standard normal density gives Eexp⁡(hTZ)=exp⁡(hTKh/2), so Egh(Z)=1.

[F4]

Measurability of integration against a kernel: Integrating a jointly measurable nonnegative function against the prior gives measurable predictive densities and posterior integrals.

[F5]

Markov's inequality for random variables: For nonnegative integrable U and b>0, P(U>b)≤EU/b.

[F6]

Tonelli's theorem for nonnegative measurable functions on a sigma-finite product: A nonnegative jointly measurable function may be integrated in either order.

[F7]

Continuous mapping theorem: Applying a continuous map to weakly convergent random elements preserves convergence in distribution.

[F8]

Dominated convergence: Pointwise convergence under a common integrable majorant passes through the integral.

[F10]

Weakly convergent sequences are tight: A weakly convergent sequence of probability laws on Rd is tight.

Proof

Proof technique: normalize the two posterior densities and control their denominators on tight central-sequence sets.

1.1A1F1F2F3F4F6F7F8givenalgebra

By [F4], integration against the prior makes mn measurable; [F6] gives EPn,0mn=1. Also ∣mn(x)−m(Δn(x))∣≤an(x), so EPn,0m(Δn)→1. The function m is continuous: if zj→z, then gh(zj)→gh(z) for each h, and compactness of H gives a common finite bound on gh(zj); [F8] passes the limit through the prior integral. Thus [F1] and [F7] give m(Δn)⇒m(Z). By [F3], Em(Z)=1. Write Un=m(Δn) and U=m(Z), and discard finitely many indices so EUn<∞. For Q>0, weak convergence of the bounded continuous cutoff and convergence of the means give E(Un−Q)+=EUn−E(Un∧Q)→EU−E(U∧Q)=E(U−Q)+. Since u1{u>2Q}≤2(u−Q)+, the limsup of the tail expectations is at most 2E(U−Q)+, which tends to zero by [F2]. The finitely many initial integrable terms also have vanishing tails; thus (Un) is uniformly integrable on this eventual index range.

1.2F9givenalgebra

Fix R>0. On the compact set {z:∥z∥2≤R}, the continuous function m(z) has a positive minimum cR, since each gh(z)>0 and π is a probability. On the event ∥Δn∥2≤R and an≤cR/2, one has mn≥cR/2. For the two posterior densities with respect to π, ∫H∣Ln(h,x)mn(x)−gh(Δn(x))m(Δn(x))∣π(dh)≤2an(x)mn(x)≤4an(x)cR. Thus the posterior total variation distance is at most 4an/cR on this event.

2.1F1F2F10step 1.1givenalgebra

The sequence Δn is tight by [F10] because it converges in distribution. For any Q>0, E[m(Δn)1{∥Δn∥2>R}]≤E[m(Δn)1{m(Δn)>Q}]+QP(∥Δn∥2>R). First choose Q large using uniform integrability from step 1.1, then R large using tightness. Since mn≤m(Δn)+an and Ean→0, the predictive probability of ∥Δn∥2>R is correspondingly small.

3.1F4F5step 1.2step 2.1givenalgebra

On {∥Δn∥2≤R}, m(Δn)≤MR for some finite MR. By [F5], Mn(∥Δn∥2≤R, an>cR/2)≤MR2EancR+Ean→0, using mn≤m+an. On the complement of the exceptional events established in the preceding two steps, step 1.2 bounds the posterior L1(π) distance by 4an/cR, and mn≤MR+cR/2. Its predictive expectation is therefore at most 4(MR+cR/2)Ean/cR→0. The distance is at most two on the exceptional events, whose predictive probabilities vanish as first n→∞ and then R→∞. This proves the first conclusion.

4.1F1step 1.1F3givenalgebra∎

For bounded continuous f, the predictive law satisfies EMnf(Δn)=EPn,0[mnf(Δn)]=EPn,0[m(Δn)f(Δn)]+o(1). For a cutoff Q, (m∧Q)f is bounded and continuous, so its expectation converges by [F1]. The tail error is at most ∥f∥∞E[m(Δn)1{m(Δn)>Q}], which tends uniformly to zero as Q→∞ by step 1.1. Thus the limit is E[m(Z)f(Z)]. This is the Gaussian-shift mixture with base law Nd(0,K) and density m(z).

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

A centered Gaussian minimizes bounded symmetric quasi-convex loss

Statement

Assume AC. Let X∼Nd(m,Σ) with positive-definite covariance Σ. Let L:Rd→[0,M] be Borel measurable and symmetric, L(−x)=L(x), and quasi-convex, meaning each sublevel set {x:L(x)≤t} is convex. Then for every a∈Rd, EL(X−a)≥EL(X−m). Thus the Gaussian center m minimizes expected loss. The result includes quasi-convex losses whose sublevel sets are not closed.

Facts & Assumptions

Given: AC; a finite-dimensional nondegenerate Gaussian vector; and a bounded Borel measurable symmetric loss with convex sublevel sets.

[A1]

The Axiom of Choice: AC is assumed for the finite-dimensional multivariate normal construction and characteristic laws used here.

[F1]

Brunn–Minkowski inequality for compact convex sets: For nonempty compact convex U,V⊂Rd, λd(U+V)1/d≥λd(U)1/d+λd(V)1/d.

[F2]

The boundary of a convex set is Lebesgue null: A convex set and its closure differ only by a Lebesgue-null boundary; lower-dimensional convex sets are null.

[F3]

Multivariate normal law, including singular covariance, Standard normal and normal laws, and The standard normal density has total mass one: A nondegenerate Gaussian is an invertible affine image of a standard Gaussian vector with density (2π)−d/2e−∥z∥22/2. The Euclidean norm is the one in The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn.

[F4]

Tonelli's theorem for nonnegative measurable functions on a sigma-finite product: Nonnegative measurable integrands may be integrated in either order.

[F5]

A linear map T of Rn sends Lebesgue measurable sets to Lebesgue measurable sets, with λn(T[E])=∣det⁡T∣ λn(E) when T is invertible and T[E] Lebesgue null when it is not: An invertible linear map scales Lebesgue measure by the absolute determinant. In particular, reflection x↦−x preserves volume and scaling by 1/2 multiplies it by 2−d. Thus the unweighted inequality in [F1], applied to U,V, gives λd((U+V)/2)1/d≥λd(U)1/d+λd(V)1/d2.

[F6]

Lebesgue outer measure, Lebesgue measurability and Lebesgue measure are unchanged by translation: Translation preserves Lebesgue measure; accordingly, translating the variable in a Lebesgue integral does not change the integral after the integrand is translated.

[F7]

Heine-Borel in Rn: with the Euclidean metric a subset of Rn is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line: Closed bounded subsets of Rd are compact. Thus intersections of the closed set C with the closed balls used below are compact and measurable.

Proof

Proof technique: prove the Gaussian shift inequality for convex level sets by Brunn–Minkowski, then integrate their indicators.

1.1F5F7givenalgebra

First let C⊆Rd be closed, symmetric, and convex. For each radius r>0 and shift v, put U=C∩(v+B‾(0,r)),V=C∩(−v+B‾(0,r)). They are compact convex sets by [F7], and V=−U, so they have equal volume by [F5]. For u∈U and w∈V, symmetry and convexity put (u+w)/2 in C, while u−v and w+v lie in the radius-r ball, so ∥(u+w)/2∥2=∥(u−v+w+v)/2∥2≤r. Thus (U+V)/2⊆C∩B‾(0,r). This sets up the Brunn–Minkowski comparison.

2.1F1F5step 1.1algebra

If U has positive volume, [F1] and its derived weighted form [F5] give λd(C∩B‾(0,r))≥λd((U+V)/2)≥λd(U), since λd(V)=λd(U). If U has zero volume the same inequality follows from nonnegativity. Therefore λd(C∩(v+B‾(0,r)))≤λd(C∩B‾(0,r)). This is the required shifted-volume inequality.

3.1F3F4F5F6step 2.1algebra

Let Z∼Nd(0,Id). Its density is a positive constant times e−∥z∥22/2. For any shift v, translation invariance [F6] and symmetry of C (using the reflection in [F5]) give P(Z∈C+v)=cd∫Ce−∥z+v∥22/2dz=cd∫Ce−∥z−v∥22/2dz, where cd>0 is the normalizing constant. The identity e−∥z−v∥22/2=∫0∞e−t1{∥z−v∥22/2≤t}dt and [F4] express the latter integral as cd∫0∞e−tλd(C∩(v+B‾(0,2t)))dt. By step 2.1, this is at most the same expression at shift zero. Hence P(Z∈C+v)≤P(Z∈C). This proves the Gaussian shift inequality.

4.1F2F6step 3.1given

If C is convex, symmetric, but not closed, replace it by C‾. The difference is contained in ∂C, which is null by [F2]; its translate is also null by [F6]. Thus the probability inequality in step 3.1 holds for every convex symmetric Borel set. If C has empty interior, [F2] makes both probabilities zero, which also covers this boundary case.

5.1A1F2F3step 4.1algebra

Write X=m+AZ with A=Σ1/2 invertible. For any symmetric convex Borel set C, the event X−a∈C is Z∈A−1C+A−1(a−m). The set A−1C is again symmetric convex, so step 4.1 gives P(X−a∈C)≤P(X−m∈C). Apply this to every sublevel set Ct={x:L(x)≤t}. This gives the comparison for each loss sublevel.

6.1F4step 5.1givenalgebra∎

For any random variable Y with 0≤Y≤M, EY=∫0MP(Y>t)dt, by [F4]. Step 5.1 says P(L(X−a)≤t)≤P(L(X−m)≤t) for each t, hence the corresponding tail probabilities are ordered in the reverse direction. Integrating them gives EL(X−a)≥EL(X−m). This proves the statement without requiring closed loss sublevels.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Le Cam's third lemma for a Gaussian likelihood-ratio limit

Statement

Assume AC.

Let Pn be probability measures and let Qn=LnPn, where Ln≥0 and EPnLn=1. Let Tn take values in Rk. Suppose under Pn that (Tn,Ln)⇒(T,eZ), where Z is normal with mean −σ2/2 and variance σ2; the joint law of (T,Z) need not be Gaussian. Then under Qn, Tn converges in distribution to the probability law determined by E[f(T(Q))]=E[eZf(T)] for every bounded continuous f. In particular, Qn is contiguous with respect to Pn. If (T,Z) is jointly Gaussian with T∼Nk(μ,Σ) and Cov⁡(T,Z)=τ, this tilted law is Nk(μ+τ,Σ), including singular Σ.

Facts & Assumptions

Given: AC; the sequences of laws, mean-one densities, and joint convergence above.

[A1]

The Axiom of Choice: AC supplies the standard-normal coordinate representation and the finite-dimensional Gaussian law facts used in the jointly Gaussian tilt calculation, and implies the Countable Choice premise of the C1 change-of-variables supplier used below.

[F1]

A mean-one likelihood-ratio limit implies contiguity: If Ln≥0, EPnLn=1, Ln⇒L≥0, and EL=1, then LnPn is contiguous with respect to Pn.

[F2]

Multivariate normal law, including singular covariance, Characteristic function of a multivariate normal law, Standard normal and normal laws, and The standard normal density has total mass one: A jointly Gaussian vector is an affine image of independent standard normal coordinates, and its characteristic function is determined by its mean and covariance. The standard normal density is ϕ(x)=(2π)−1/2e−x2/2.

[F3]

A C^1 diffeomorphism satisfies the change-of-variables formula for nonnegative Lebesgue measurable functions: Translation by b on Rm is a C1 diffeomorphism with Jacobian one, so the change-of-variables formula applies to the positive and negative parts of the bounded integrand in the Gaussian tilt calculation.

[F4]

Contiguous sequences of probability measures: Qn◃Pn means Pn(An)→0 implies Qn(An)→0 for every measurable event sequence.

[F5]

Convergence in distribution of random elements and Dominated convergence: Bounded continuous expectations converge under weak convergence, and integrable majorants permit passage to limits.

[F6]

Independent random elements have product joint law, Tonelli's theorem for nonnegative measurable functions on a sigma-finite product, and On Borel subsets of R^{m+n}, the product lambda_m times lambda_n agrees with lambda_{m+n}: Independent coordinates have product joint law; repeated scalar integration and the Borel product-Lebesgue identity identify its product density. AC supplies the countable choice required by the last supplier.

Proof

Proof technique: uniform integrability transfers expectations, then a Gaussian exponential tilt computes the shifted limit.

1.1A1F2givenalgebra

If σ>0, write Z=−σ2/2+σG with G∼N(0,1). Completing the square gives EeσG=∫eσxϕ(x)dx=eσ2/2∫ϕ(x−σ)dx=eσ2/2, so EeZ=1. If σ=0, then Z=0 and the same equality holds. The hypothesis gives the joint likelihood-ratio convergence.

2.1F5step 1.1givenalgebra

For M>0, [F5] and step 1.1 give E(Ln−M)+=1−E(Ln∧M)→1−E(eZ∧M)=E(eZ−M)+. Since x1{x>2M}≤2(x−M)+, the limsup of the tail expectations is at most 2E(eZ−M)+→0 by dominated convergence [F5]. Each finite initial set of integrable Ln has vanishing tails as well, so (Ln) is uniformly integrable. For bounded continuous f and M>0, the function (t,ℓ)↦f(t)(ℓ∧M) is bounded and continuous. Its expectations converge by [F5] and the given joint convergence; uniform integrability lets M→∞, giving EQnf(Tn)=EPn[Lnf(Tn)]⟶E[eZf(T)]. The equality on the left follows from Qn=LnPn, first for indicators and then for bounded measurable functions by simple approximation. Thus the right side is the distributional limit under Qn.

3.1A1F2F3F6step 2.1algebra

Suppose (T,Z) is jointly Gaussian. By [F2], represent its law as T=μ+BG and Z=−σ2/2+bTG, where G has m independent standard-normal coordinates, BBT=Σ, Bb=τ, and bTb=σ2. By [F6] and the scalar density in [F2], G has Borel density ϕm(g)=∏j=1m(2π)−1/2e−gj2/2 with respect to m-dimensional Lebesgue measure (the one-coordinate case uses the scalar law directly). Completing the square coordinatewise gives ebTg−∥b∥2/2ϕm(g)=ϕm(g−b). Thus for every bounded continuous f, the translation change of variables justified by [F3] gives E[eZf(T)]=∫Rmf(μ+Bg)ϕm(g−b) dg=∫Rmf(μ+B(g+b))ϕm(g) dg. The integrals are absolutely convergent because f is bounded and the shifted Gaussian density integrates to one. The final integral is E[f(μ+Bb+BG)], so the tilted law from step 2.1 is the affine Gaussian law Nk(μ+τ,Σ) by [F2]. No inverse of Σ is used, and the argument includes singular Σ and b=0.

4.1F1F4step 1.1∎

Contiguity is the first conclusion of [F1] under the present hypotheses; [F4] states its event-sequence meaning.

LemmaStatement: AI-adaptedProof: AI-adaptedOpen item page →

Bounded bowl-shaped losses have Gaussian-centered Lipschitz minorants

Statement

Assume AC. Let L:Rd→[0,M] be Borel measurable, symmetric and quasi-convex, with M>0. For integers N≥2 and m≥1, put δ=M/N, Ck={x:L(x)≤kδ}‾ and gN,m(x)=δ∑k=1N−1min⁡(1,m d(x,Ck)). For Ck=∅ the corresponding summand is defined to be one, and for Ck=Rd it is zero. Then 0≤gN,m≤L, and gN,m is bounded and Lipschitz. For every nondegenerate Gaussian H∼Nd(b,S), inf⁡aEgN,m(a−H)=EgN,m(H−b),lim⁡N→∞lim⁡m→∞EgN,m(H−b)=EL(H−b). Each summand is symmetric and quasi-convex; no quasi-convexity of their sum is asserted.

Facts & Assumptions

Given: AC, the bounded bowl-shaped loss, integers and Gaussian law.

[F2]

The boundary of a convex set is Lebesgue null: the boundary of a convex set is Lebesgue-null, including lower-dimensional convex sets.

[F3]

A centered Gaussian minimizes bounded symmetric quasi-convex loss: a bounded Borel symmetric quasi-convex loss has least Gaussian shift risk at the Gaussian center.

[F4]

Multivariate normal law, including singular covariance: A nondegenerate Gaussian can be realized as b+AG, where A=S1/2 is invertible and G has independent standard-normal coordinates.

[F5]

Dominated convergence passes limits of functions bounded by M through the Gaussian expectation.

[F6]

Bounded subset, diameter, distance from a point to a set, and distance between two sets in a metric space, Greatest lower bound (infimum), and Every nonempty set bounded below has an infimum: d(x,C)=inf⁡c∈C∥x−c∥2, and for every ϵ>0 a point of nonempty C can be chosen within ϵ of this infimum.

[F7]

The inner-product norm is definite, homogeneous, and satisfies the triangle inequality: The Euclidean norm satisfies ∥u+v∥2≤∥u∥2+∥v∥2.

[F8]

The Lebesgue integral is linear on L1(μ): The expectation of a finite sum of bounded measurable functions is the sum of their expectations.

[F9]

Borel measurable and Lebesgue measurable functions on Rn: Borel functions on Rd are measurable for the Gaussian and Lebesgue integrals.

[F10]

A convex set and its closure have the same interior and boundary: Under AC and countable choice, a nonempty convex subset and its closure have the same interior and boundary, and the closure is convex. AC supplies countable choice here.

[F11]

A point lies in the closure of A iff some sequence in A converges to it, and a set is closed iff it is sequentially closed: A point in the closure of a subset of Euclidean space is the limit of a sequence from that subset.

[A1]

The Axiom of Choice is retained for the Gaussian and centering suppliers.

[F12]

Standard normal and normal laws, Independent random elements have product joint law, Tonelli's theorem for nonnegative measurable functions on a sigma-finite product, and On Borel subsets of R^{m+n}, the product lambda_m times lambda_n agrees with lambda_{m+n}: The scalar standard normal has density ϕ(t)=(2π)−1/2e−t2/2; independent coordinates have product law, repeated integration is valid, and product Lebesgue measure agrees with Euclidean Lebesgue measure on Borel sets.

Proof

1.1A1F1F6F7F9F10F11givenchooseconstructalgebra

Each sublevel Ak={L≤kδ} is convex and symmetric by hypothesis. Its closure Ck is closed; it is convex by [F10] when Ak is nonempty, and is convex by vacuity when Ak=∅. If x∈Ck, [F11] supplies xj∈Ak with xj→x; then −xj∈Ak and −x∈Ck, so Ck is symmetric (the empty case is symmetric as well). For a nonempty closed convex C, choose cx,cy∈C within ϵ of d(x,C),d(y,C) using [F6]. Their convex combination lies in C, and [F7] gives d((1−t)x+ty,C)≤(1−t)d(x,C)+td(y,C)+ϵ. Let ϵ↓0 to prove convexity of the distance function. When C=−C, replacing each c by −c in the infimum shows d(−x,C)=d(x,C). Thus for a nonempty proper Ck, q(x)=min⁡(1,md(x,Ck)) is symmetric; its sublevel at 0≤t<1 is {d(x,Ck)≤t/m}, which is convex, and its sublevel for t≥1 is the whole space. It is Borel and m-Lipschitz by [F1] and [F9]. For empty Ck or Ck=Rd, the stated constant conventions have the same properties.

2.1F3F8A1step 1.1algebra

If L(x)≤kδ, then x∈Ck and the kth term is zero. Every remaining term is at most one, so 0≤gN,m(x)≤δ#{1≤k<N:kδ<L(x)}≤L(x). The finite sum is bounded by M and has Lipschitz constant at most Mm. Apply F3 separately to each summand. Every summand's expected loss is minimized at a=b (use its symmetry to replace b−H by H−b), so the same action minimizes their sum by [F8]. This proves the first displayed identity without assuming the sum quasi-convex.

3.1A1F2F4F5F9F10F12F13step 2.1algebra∎

Since Ck is closed, its kth term increases to 1Ckc as m→∞. If Ck=Rd, then [F10] gives int⁡{L≤kδ}=Rd, so the level set is all of Rd and both indicators vanish. If Ck=∅, the level set is empty and both indicators equal one. Otherwise the difference between {L>kδ} and Ckc is contained in the boundary of the convex set {L≤kδ}, which is null by [F2]. To justify the Gaussian nullity, [F4] realizes H−b=AG. By [F12], repeated integration of the scalar densities gives P(G∈E)=∫E∏j=1dϕ(zj) dλd(z) for every Borel E (for d=1 this is the scalar definition). The closed boundary D is Borel and null, and A−1D is null by [F13], so P(H−b∈D)=P(G∈A−1D)=0. Therefore F5 gives lim⁡mEgN,m(H−b)=E[δ∑k=1N−11{L(H−b)>kδ}]. The expression inside the expectation differs from L(H−b) by at most δ: count the grid thresholds strictly below each value in [0,M]. Let N→∞ to obtain the second identity.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

A QMD score is centered and has finite information

Statement

Assume AC and a parametric model QMD at θ0 with score sθ0. Then Eθ0sθ0=0, and the information matrix Iθ0=Eθ0[sθ0sθ0T] has finite entries and is positive semidefinite. The QMD convention and square-integrability of the score are those of Quadratic-mean differentiability at a parameter.

Facts & Assumptions

Given: AC; an open parameter set in Rd, a common sigma-finite dominator with density versions pθ, an interior point θ0, and the QMD score s=sθ0 with Eθ0∥s∥22<∞.

[A1]

The Axiom of Choice: AC supplies the selected density versions in Likelihood densities.

[F1]

Likelihood densities: Each pθ is a measurable density version satisfying Pθ(A)=∫Apθ dμ.

[F2]

Quadratic-mean differentiability at a parameter: For u→0, pθ0+u=pθ0+12(uTs)pθ0+ru,∥ru∥L2(μ)=o(∥u∥2).

[F3]

The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn: uTs=∑j=1dujsj and ∥u∥22=uTu are the Euclidean inner product and norm.

[F5]

Holder's inequality for integrals, including the endpoint cases and Minkowski's inequality for integrals, including p=∞: On a probability space, ∣EUV∣≤(EU2)1/2(EV2)1/2 and the L2 norm satisfies the triangle inequality.

Proof

technique · differentiate the squared $L^2(\mu)$ norm along a line
1.1A1F1F2givenalgebra

Fix v∈Rd and put ft=pθ0+tv, f0=pθ0. By [F1]–[F2], ft−f0=t2(vTs)f0+rtv,∥rtv∥2=o(∣t∣). Since each density integrates to one, ∥ft∥2=∥f0∥2=1, and 0=2⟨f0,ft−f0⟩+∥ft−f0∥22. This identity uses the unit norms of the square-root densities.

2.1F2F5step 1.1givenalgebra

The increment has norm O(∣t∣), so its squared norm divided by t tends to zero. By Cauchy–Schwarz, the residual inner product ⟨f0,rtv⟩/t also tends to zero. Divide the identity in step 1.1 by t and let t→0; the remaining term is Eθ0(vTs)=0. Since this holds for every v, each coordinate of Eθ0s is zero.

3.1F2F3F4F5givenalgebra∎

Each sj is square-integrable under a probability law, so E∣sj∣<∞ by Cauchy–Schwarz. Also E∣sjsk∣≤(Esj2)1/2(Esk2)1/2<∞; hence every entry of Iθ0 is finite. For any a∈Rd, aTIθ0a=E(aTs)2≥0, proving positive semidefiniteness, with no nonsingularity assertion.

TheoremStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

Convolution bound for regular estimators

Statement

Assume AC. Let {Pn,h:h∈Rd} be LAN at h=0 with positive-definite information matrix K and central sequence Δn. Let Tn=n(θ^n−θ0) be regular under every fixed local alternative, with common limit law W as in Regular estimator under local alternatives. Then there is a probability law ν on Rd such that L(W)=Nd(0,K−1)∗ν. Here ∗ is convolution, the law of the sum of independent random vectors with the two indicated laws. In particular, the efficient Gaussian component with covariance K−1 is a convolution factor of every regular limit.

Facts & Assumptions

Given: AC; the LAN experiment, positive-definite K, central sequence, and regular estimator with common limit law W.

[A1]

The Axiom of Choice: AC is assumed by Prokhorov tightness, the Gaussian laws, and characteristic-function uniqueness.

[F1]

Local asymptotic normality for local experiments: For each fixed h, an absolutely continuous proxy has log likelihood hTΔn−12hTKh+oPn,0(1) and is total-variation close to the true local law.

[F2]

Regular estimator under local alternatives: Under every fixed Pn,h, Tn−h⇒W with the same W.

[F3]

Le Cam's third lemma for a Gaussian likelihood-ratio limit: A joint limit tilted by the mean-one Gaussian likelihood ratio describes limits under the proxy local alternative; total-variation closeness transfers that law to the true alternative.

[F4]

Weakly convergent sequences are tight and Prokhorov tightness theorem on polish spaces: Weakly convergent laws on Euclidean space are tight, and under AC every tight sequence of laws on a Polish space has a weakly convergent subsequence.

[F5]

Vector Slutsky theorem: If one component converges in distribution and another differs in probability by oP(1) from a continuous function of it, the joint vector converges to the corresponding joint limit.

[F6]

Multivariate normal law, including singular covariance and Characteristic function of a multivariate normal law: If Δ∼Nd(0,K), then EehTΔ=ehTKh/2 and its characteristic function is e−uTKu/2.

[F7]

Identity theorem for holomorphic functions: Two holomorphic functions on a connected domain that agree on a set with an interior accumulation point agree throughout the domain.

[F8]

Uniqueness of a law from its characteristic function: Under AC, probability laws on R with identical characteristic functions are equal.

[F9]

The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn: Tightness and compact balls use the Euclidean norm on Rd.

[F10]

Continuous mapping theorem: Continuous maps preserve convergence in distribution at points where they are continuous.

[F11]

Cramer wold device: Under AC, Borel probability laws on a finite-dimensional Euclidean space are determined by all their real linear projection laws.

[F12]

The product measure of two sigma-finite measure spaces, For sigma-finite factors, the product measure exists, has the rectangle formula, is sigma-finite, and is unique, and Tonelli's theorem for nonnegative measurable functions on a sigma-finite product: The product of two Borel probability laws exists, and bounded product integrals factor into the marginal integrals, by applying Tonelli to the positive and negative parts of their real and imaginary parts.

Proof

Proof technique: extract a joint weak limit, use the third lemma for every fixed local shift, and analytically continue the Gaussian tilt identity.

1.1A1F1F2F4F9givenchoosealgebra

Under Pn,0, Tn⇒W by regularity at h=0 and Δn⇒Nd(0,K) by LAN. By [F4], both marginal sequences are tight. Their joint laws are tight: for any ϵ>0, choose compact balls CT,CΔ with marginal outside probabilities below ϵ/2; the union bound puts the joint law on the compact product with probability at least 1−ϵ.

2.1A1F4step 1.1

By [F4] and Prokhorov's theorem, select a subsequence along which (Tn,Δn)⇒(T,Δ). Its marginals are T∼W and Δ∼Nd(0,K), since the full marginal sequences already converge. This supplies the joint-limit subsequence used below.

3.1F1F2F3F5F10step 2.1givenalgebra

Fix h∈Rd. Along this subsequence [F1] and [F5] give (Tn,Δn,log⁡Ln,h)⇒(T,Δ,hTΔ−12hTKh). The final coordinate is normal with mean −hTKh/2 and variance hTKh. By [F1], Pn,0(Ln,h=0)→0. Assign any finite value to the log on that vanishing event; [F10] then gives (Tn,Δn,Ln,h)⇒(T,Δ,ehTΔ−hTKh/2). By [F3], under the true Pn,h law, the first coordinate has limit T(h) given by tilting the joint law of (T,Δ) by ehTΔ−hTKh/2. Regularity [F2] also gives Tn⇒W+h under Pn,h. Therefore for every t∈Rd and every real h, E[ehTΔ−hTKh/2eitTT]=eitThφW(t), where φW is the characteristic function of W.

4.1F6F7step 3.1algebra

Rearranging step 3.1 gives, for real h, Ft(h):=E[eitTT+hTΔ]=ehTKh/2+itThφW(t). For complex z∈Cd, Ft(z)=E[eitTT+zTΔ] is entire in each coordinate: on every compact set of z, its exponential power series and coordinate derivatives are dominated by eR∥Δ∥1 for some finite R, whose expectation is finite because each Gaussian coordinate has finite exponential moments. The right-hand side is also entire. Apply [F7] one coordinate at a time, holding the other coordinates real and then successively allowing them to be complex. The equality therefore holds for every complex z.

5.1F6step 4.1givenalgebra

Set z=iu in step 4.1. Then E[eitTT+iuTΔ]=φW(t)e−tTu−uTKu/2. Let R=T−K−1Δ. Replacing u by u−K−1t gives E[eitTR+iuTΔ]=(φW(t)etTK−1t/2)e−uTKu/2. The first factor equals EeitTR by setting u=0; the second is the characteristic function of Δ. Thus the joint characteristic function of (R,Δ) factors into its marginals.

6.1A1F6F8F11F12step 5.1algebra∎

By [F12], form the product law ρ=L(R)⊗L(Δ) on R2d. Step 5.1 and factorization of the bounded product integrals show that ρ and L(R,Δ) have identical joint characteristic functions. For every a,b∈Rd and real v, evaluate these functions at (va,vb); this gives equality of the scalar characteristic functions of the projection (r,z)↦aTr+bTz under the two laws. Scalar uniqueness [F8] identifies each projection law, and Cramér–Wold [F11], under the existing AC hypothesis [A1], gives L(R,Δ)=ρ. Thus R and Δ are independent. Since K is invertible, K−1Δ∼Nd(0,K−1), and T=K−1Δ+R. The law of T, which is W, is therefore Nd(0,K−1)∗L(R), proving the claimed convolution with ν=L(R).

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

QMD controls singular and zero-overlap masses

Statement

Assume AC and the hypotheses of Quadratic-mean differentiability at a parameter. Write p0=pθ0, pu=pθ0+u, and P0=Pθ0. Let α(u):=Pθ0+u(p0=0),β(u):=P0(pu=0). Then α(u)=o(∥u∥22) and β(u)=o(∥u∥22) as u→0.

Facts & Assumptions

Given: AC; QMD at θ0 with score s square-integrable under P0, and density versions p0,pu relative to the common measure μ.

[A1]

The Axiom of Choice: AC supplies the density representatives in Likelihood densities.

[L1]

Likelihood densities: Each selected pθ is nonnegative and measurable with Pθ(A)=∫Apθ dμ.

[F1]

Quadratic-mean differentiability at a parameter: The residual ru=pu−p0−12(uTs)p0 satisfies ∥ru∥L2(μ)=o(∥u∥2).

[F2]

A QMD score is centered and has finite information: E0∥s∥22<∞.

[F4]

Holder's inequality for integrals, including the endpoint cases and Minkowski's inequality for integrals, including p=∞: Cauchy–Schwarz bounds L2 inner products and the L2 norm satisfies the triangle inequality.

[F5]

Absolute continuity of the integral: If g∈L1(P0) and P0(Bu)→0, then E0[∣g∣1Bu]→0.

Proof

Proof technique: restrict the QMD residual to the two support-complement sets.

1.1A1F1L1givenalgebra

Set S={p0>0}. On Sc, both p0 and (uTs)p0 vanish, so ru=pu there. Therefore α(u)=∫Scpu dμ=∫Scru2 dμ≤∥ru∥22=o(∥u∥22). This is the claimed singular-mass bound.

1.2F1F2F3F4L1givenalgebra

Let Bu=S∩{pu=0}. On Bu, pu−p0=−p0, so P0(Bu)≤∥pu−p0∥22=O(∥u∥22)→0, where the last bound follows from [F1], [F2], [F3], and [F4]. Thus the sets Bu shrink to zero in P0 measure.

2.1F1F2F3F4L1step 1.2given

On Bu, the residual identity in [F1] gives p0 1Bu=−12(uTs)p0 1Bu−ru1Bu. Taking L2(μ) norms and using [F3] yields β(u)≤12∥u∥2(E0[∥s∥221Bu])1/2+o(∥u∥2). This is the required norm bound.

3.1F2F5step 1.2step 2.1algebra∎

Since ∥s∥22 is integrable and P0(Bu)→0, [F5] gives E0[∥s∥221Bu]→0. Step 2.1 therefore gives β(u)=o(∥u∥2) and β(u)=o(∥u∥22). Because P0(pu=0)=P0(Bu), this is the claimed zero-overlap bound.

LemmaStatement: AI-adaptedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

Finite-prior Bayes envelopes converge under pointwise LAN

Statement

Assume AC. In a pointwise LAN experiment Local asymptotic normality for local experiments with K≻0, fix h1,…,hs∈Rd and weights wi>0 summing to one. Let g:Rd→[0,M] be Lipschitz. The Bayes values for estimating h with loss g(a−h) and this finite prior, allowing all measurable randomized rules, converge to the corresponding Bayes value in the Gaussian shift Y∣h∼Nd(h,K−1). No likelihood-field uniformity or measurable-selection hypothesis is required.

Facts & Assumptions

Given: AC, the pointwise LAN experiment, finite prior and bounded Lipschitz loss.

[F1]

Local asymptotic normality for local experiments gives mean-one likelihood proxies Ln,h, pointwise total-variation approximation, and log⁡Ln,h=hTΔn−hTKh/2+oP(1) with Δn⇒Nd(0,K). Its finite log expansion also gives Pn,0(Ln,h=0)→0.

[F2]

Vector Slutsky theorem and Continuous mapping theorem give joint finite-dimensional convergence after adjoining finitely many remainders that tend to zero in probability.

[F3]

A mean-one likelihood-ratio limit implies contiguity proves uniform integrability for nonnegative mean-one variables converging in law to a mean-one limit.

[F4]

Bayes risk and minimax risk defines the Bayes risk of a rule δ as rπ(δ)=∫R(h,δ) π(dh), while Measure kernel and probability kernel describes randomized rules. In this proof the Bayes value means the infimum of rπ(δ) over all measurable randomized rules; the infimum is local notation and is not part of the supplier's definition.

[F5]

Total variation distance for probability laws and Tonelli's theorem for nonnegative measurable functions on a sigma-finite product imply ∣EPf−EQf∣≤M∥P−Q∥TV for 0≤f≤M, by integrating the tail probabilities of f.

[F6]

Both Q and R∖Q are dense in R, and every nonempty open subset of R is uncountable gives a countable dense rational grid in finite-dimensional Euclidean action space by taking finite products.

[F8]

The Lebesgue integral is linear on L1(μ): Expectation commutes with the finite weighted sums defining Un and U.

[A1]

The Axiom of Choice is retained for the LAN and Gaussian suppliers.

Proof

1.1F4F6givenconstructalgebra

For l∈[0,∞)s, set F(l)=inf⁡a∑iwilig(a−hi). For any l,l′, each action's objective changes by at most M∑iwi∣li−li′∣; taking infima proves the same bound for F. Also 0≤F(l)≤M∑iwili. For fixed l the objective is continuous in a, so F6 makes its infimum equal to the infimum over a fixed enumeration (qj) of the rational grid. For ϵ>0, choose the first j whose objective is at most F(l)+ϵ. This index is Borel: its defining set and the finitely many failures at smaller indices are Borel. Thus this is an explicit measurable ϵ-optimal action function of l.

1.2F1F2F3F7F8A1givenconstruct

Under the base law, F1 and F2 imply (Ln,hi)i=1s⇒(li(Z))i=1s, where Z∼Nd(0,K) and li(z)=exp⁡(hiTz−hiTKhi/2). The log expansions imply that zero likelihoods have vanishing probability, so exponentiating the finite vector is legitimate. By [F7], completing the square in the Gaussian density gives Eli(Z)=1. Hence Un=∑iwiLn,hi converges in law to U=∑iwili(Z), and [F8] gives EUn=EU=1. [F3] makes (Un) uniformly integrable.

2.1F2F3step 1.1step 1.2algebra

For each cutoff b, F∧b is bounded continuous, so its expectations converge by step 1.2. The error from this cutoff is bounded by ME[Un1{MUn>b}], which vanishes uniformly as b→∞; the limit variable has the same integrable bound. Therefore EF((Ln,hi)i)→EF((li(Z))i).

3.1F1F4F5step 1.1step 2.1algebra∎

Under the proxy mixture, the predictive density is Un=∑iwiLn,hi and, when Un>0, the posterior weights are wiLn,hi/Un. Conditional on the data, every randomized action rule has posterior risk at least F((Ln,hi)i)/Un, because F is the infimum over deterministic actions and randomization averages those action risks. The measurable selector from step 1.1 has posterior risk at most this envelope plus ϵ. Multiplying by the predictive density and integrating shows that the proxy Bayes value differs from EPn,0F((Ln,hi)i) by at most ϵ; the set Un=0 has zero predictive probability. Letting ϵ↓0 identifies the proxy Bayes value with that expectation. The same argument with li(Z) identifies the limiting envelope expectation as the finite-prior Gaussian Bayes value: tilting the base Gaussian by li gives Z∼Nd(Khi,K), and Y=K−1Z has law Nd(hi,K−1). Finally [F5] bounds the actual/proxy risk difference uniformly over rules by M∑iwi∥Pn,hi−Ln,hiPn,0∥TV→0. Infima preserve this bound, proving the assertion.

LemmaStatement: AI-adaptedProof: AI-adaptedOpen item page →

Finite priors approximate Gaussian-shift Bayes values

Statement

Assume AC. Let Qh=Nd(h,S) with S≻0 and let g:Rd→[0,M] have Lipschitz constant B<∞. For every Borel probability prior π on Rd and ϵ>0, there is a finite-support prior πf whose Bayes value for loss g(a−h) differs from that of π by less than ϵ. The comparison is uniform over all measurable randomized rules. In particular this applies to every diffuse Gaussian prior; no posterior selector assumption is needed.

Facts & Assumptions

Given: AC, the Gaussian shift, bounded Lipschitz loss, prior and accuracy.

[F1]

Multivariate normal law, including singular covariance: For positive finite dimension, Nd(h,S) is realized as h+S1/2G with independent standard-normal coordinates. For S≻0, the square root is invertible.

[F2]

Dominated convergence passes pointwise limits under an integrable envelope through an integral.

[F3]

Bayes risk and minimax risk defines the prior risk rπ(δ) of a rule, and Measure kernel and probability kernel defines randomized rules. Here the Bayes value means inf⁡δrπ(δ) over those rules; this infimum is the local value under comparison, not a separate definition supplied by the linked item.

[F4]

Total variation distance for probability laws and Tonelli's theorem for nonnegative measurable functions on a sigma-finite product give the bound ∣EPf−EQf∣≤M∥P−Q∥TV for 0≤f≤M. The event-supremum distance satisfies the triangle inequality by the triangle inequality for each event difference.

[F6]

Continuity from below for measures: If Br↑Rd, then π(Br)↑1.

[F7]

The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn: ∥h−h′∥2 is the Euclidean distance used for the ball cover and Lipschitz bound.

[F8]

Measurability of integration against a kernel: Integrating a jointly measurable nonnegative function against a probability kernel gives a measurable function of the parameter.

[F9]

A definite quadratic form has a uniform signed bound on the Euclidean unit sphere: A positive definite quadratic form on Rd has a positive lower bound on the Euclidean unit sphere.

[A1]

The Axiom of Choice is retained for the Gaussian construction.

[F10]

Standard normal and normal laws, Independent random elements have product joint law, and On Borel subsets of R^{m+n}, the product lambda_m times lambda_n agrees with lambda_{m+n}: Standard-normal coordinates have scalar density ϕ(t)=(2π)−1/2e−t2/2 and product joint law; product Lebesgue measure agrees with Euclidean Lebesgue measure on Borel sets. Tonelli [F4] therefore permits repeated integration of their product density.

[F11]

A C^1 diffeomorphism satisfies the change-of-variables formula for nonnegative Lebesgue measurable functions: Under countable choice, a C1 diffeomorphism transforms a nonnegative Lebesgue integral with the absolute Jacobian determinant. AC supplies countable choice here and in [F10].

Proof

1.1givenconstructalgebra

If dimension zero is admitted with the singleton empty-tuple Gaussian convention, there is only one parameter, observation and action. Every prior is the point mass at that parameter and is already finitely supported; every rule has risk g(0). Taking πf=π gives zero discrepancy. No positive-dimension density, sphere or compactness theorem is needed. Henceforth let d≥1.

2.1F1F2F4F5F7F9F10F11A1step 1.1givenalgebra

Write A=S1/2. By [F1] and [F10], Qh is the law of h+AG, and repeated scalar integration gives G density (2π)−d/2e−∥z∥22/2. Applying [F11] to z↦h+Az gives the density qh(y)=(2π)−d/2∣det⁡A∣−1exp⁡[−(y−h)TS−1(y−h)/2]. The map h↦Qh is continuous in total variation: when hj→h, these densities converge pointwise. The matrix S−1 is positive definite because xTS−1x=(S−1x)TS(S−1x)>0 for x≠0. By [F9], yTS−1y≥c∥y∥22 for some c>0. On a fixed bounded set of shifts, the density formula and ∥y−h∥22≥∥y∥22/2−∥h∥22 bound all these densities by Cexp⁡(−c′∥y∥22) for constants C,c′>0. This envelope is integrable by repeated scalar Gaussian integration [F4, F10, F11], so [F2] gives L1 convergence; for every event, its probability difference is at most that L1 distance. On a compact ball this continuity is uniform: otherwise there are hj,hj′ in the ball with ∥hj−hj′∥2→0 but TV distances bounded below. Compactness gives a subsequence with both converging to the same h; pointwise continuity and the event-supremum triangle inequality from [F4] contradict that lower bound.

3.1F1F3F4F8step 2.1algebra

For a randomized rule δy(da), write Rδ(h)=∫∫g(a−h)δy(da)Qh(dy). Change the loss argument first and the sampling law second. [F4] yields ∣Rδ(h)−Rδ(h′)∣≤B∥h−h′∥2+M∥Qh−Qh′∥TV, independently of the rule. Each risk is between zero and M. The inner kernel integral is jointly measurable in (h,y) by [F8]; multiplying by the jointly measurable Gaussian density and integrating in y makes Rδ(h) measurable.

4.1F3F5F6step 2.1step 3.1constructalgebra∎

The balls Br={h:∥h∥2≤r} increase to Rd, so [F6] lets us choose a closed ball with discarded prior mass less than τ. Cover this compact ball by open balls of radius η/2; [F5] gives a finite subcover. Intersect the first ball with the closed ball, then successively remove the previous covering sets from each later intersection. This makes a finite Borel partition whose cells have diameter at most η. Assign one point to each nonempty cell and send points outside the closed ball to zero. The resulting finite-valued map q is Borel, and πf=π∘q−1. On the ball, step 3.1 bounds ∣Rδ(h)−Rδ(q(h))∣ by Bη+Mω(η), where the compact-ball TV modulus satisfies ω(η)→0 by step 2.1. Outside, use M. Thus prior risks differ uniformly over rules by at most Bη+Mω(η)+Mτ. Choose the ball first for small tail, then the cell diameter small on that fixed ball. This makes the bound less than ϵ; taking infima over the same rules preserves it.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

Normalized product likelihood expansion under QMD

Statement

Assume AC and Quadratic-mean differentiability at a parameter at θ0 with score s and information I. Let hn→h in Rd, put un=hn/n, and write P0=Pθ0 and Pun=Pθ0+un. On S={pθ0>0} define, for all sufficiently large n, qn(x)=1S(x)pθ0+un(x)(1−αn)pθ0(x),αn=Pun(Sc). Then qn is a probability density relative to P0. For IID X1,…,Xn∼P0, let Ln=∏i=1nqn(Xi) and Δn=n−1/2∑i=1ns(Xi). Under P0⊗n, log⁡Ln=hnTΔn−12hTIh+oP(1),P0⊗n(Ln=0)→0. Moreover, if Pˉn=qnP0 is the normalized absolutely continuous component of Pun relative to P0, then ∥Pun⊗n−Pˉn⊗n∥TV→0. No full likelihood ratio for Pun⊗n is asserted.

Facts & Assumptions

Given: AC; a common sigma-finite dominator μ, the QMD density versions at θ0 and θ0+u, a square-integrable score s, and hn→h.

[A1]

The Axiom of Choice: AC supplies the simultaneous density versions in Likelihood densities.

[L1]

Likelihood densities: Each selected pθ is a measurable nonnegative density with Pθ(A)=∫Apθ dμ.

[F1]

Quadratic-mean differentiability at a parameter: With p0=pθ0, pθ0+u−p0−12(uTs)p0=ru,∥ru∥L2(μ)=o(∥u∥2).

[F2]

A QMD score is centered and has finite information: E0s=0 and I=E0[ssT] is finite.

[F3]

QMD controls singular and zero-overlap masses: If α(u)=Pθ0+u(p0=0) and β(u)=P0(pθ0+u=0), then both are o(∥u∥22).

[F4]

Khinchin weak law for integrable IID variables: For IID integrable real variables Zi, n−1∑i=1nZi→EZ1 in probability.

[F5]

Identical distribution and IID families: Under P0⊗n, the coordinate variables Xi are IID with common law P0.

[F7]

Total variation distance for probability laws: Total variation is sup⁡A∣P(A)−Q(A)∣ over measurable events.

[F9]

L1 convergence implies uniform integrability: An L1-convergent sequence of nonnegative random variables is uniformly integrable.

[F10]

Markov's inequality for random variables: For a nonnegative integrable variable W and a>0, P(W>a)≤EW/a.

[F11]

The Lagrange and Cauchy forms of Taylor's remainder: A C3 function with bounded third derivative on an interval has a quadratic Taylor remainder bounded by a constant times the cube of the increment.

Proof

Proof technique: square-root expansion, a triangular-array logarithm calculation, and a product-mixture bound.

1.1A1F1F2F3F8L1givenalgebra

Write pu=pθ0+u, S={p0>0}, and α(u)=∫Scpu dμ. For small u, [F3] gives α(u)<1/2. Define qu=1Spu/((1−α(u))p0) on S and qu=0 on Sc. It is nonnegative and measurable, and ∫qu dP0=(1−α(u))−1∫Spu dμ=1, so it is a probability density. At u=0, α(0)=0 and q0=1 P0-almost surely, since P0(Sc)=∫Scp0 dμ=0. On S, qu=(1−α(u))−1/2(1+12uTs+rup0). The residual term has L2(P0) norm ∥ru1S∥L2(μ)=o(∥u∥2). Also ∣(1−α)−1/2−1∣=α1−α(1+1−α)=O(α), and [F2], [F8] give ∥uTs∥L2(P0)=O(∥u∥2). Therefore Yu:=2(qu−1)=uTs+Ru,∥Ru∥L2(P0)=o(∥u∥2). This is the required square-root expansion.

1.2F5F6givenalgebra

The product function Ln=∏iqun(Xi) is a density of Pˉn⊗n relative to P0⊗n. For a measurable rectangle A1×⋯×An, Tonelli gives ∫A1×⋯×An∏iqun(xi) dP0⊗n=∏i∫Aiqun dP0=∏iPˉn(Ai). By [F6], agreement on rectangles identifies the product measures. Taking the whole space gives EP0⊗nLn=1.

2.1F2F8step 1.1givenalgebra

Since E0qu=1, E0Yu=−14E0Yu2. By step 1.1, [F2], and [F8], E0Yu2=uTIu+o(∥u∥22),E0Yu=−14uTIu+o(∥u∥22). Indeed, the difference between Yu and uTs has L2(P0) norm o(∥u∥2), so Cauchy–Schwarz makes the difference of their squared norms o(∥u∥22).

2.2F2F4F8step 1.1givenalgebra

Apply [F4] to Zi=∥s(Xi)∥22, whose mean is finite by [F2]. Then 1n∑i=1n(hnTs(Xi))2→hTIh in probability: for fixed h this is [F4] applied to (hTs)2, and the difference for hn is bounded by ∥hn−h∥2∥hn+h∥21n∑i=1n∥s(Xi)∥22→0. Step 1.1 and [F8] also give ∑i=1nYun(Xi)2−1n∑i=1n(hnTs(Xi))2→0 in probability, because its expected absolute value is at most n∥Run∥2(∥Yun∥2+∥unTs∥2)=o(n∥un∥22)=o(1). Consequently ∑iYun(Xi)2→hTIh.

2.3F3F8F9F10step 1.1givenalgebra

Put Vn=nYun(X1). Step 1.1 implies Vn−hnTs(X1)→0 in L2(P0), so Vn→hTs(X1) in L2. By [F8], Vn2→(hTs(X1))2 in L1; [F9] makes (Vn2) uniformly integrable. For every ε>0, [F10] and the union bound give P0⊗n ⁣(max⁡i≤n∣Yun(Xi)∣>ε)≤ε−2E0[Vn21{∣Vn∣>εn}]→0. Also P0⊗n(Ln=0)≤nβ(un)→0 by [F3] and the union bound.

3.1F2F5F10step 2.1givenalgebra

Let Run=Yun−unTs. Its centered IID sum has variance at most nE0Run2=o(n∥un∥22)=o(1). By step 2.1, nE0Run=nE0Yun=−14hnTIhn+o(1)→−14hTIh. Markov's inequality [F10], applied to the square of the centered sum, gives ∑iYun(Xi)=hnTΔn−14hTIh+oP(1). This is the required expansion of the sum.

4.1F11step 2.2step 3.1step 2.3given

On the event that every qun(Xi)>0 and max⁡i∣Yun(Xi)∣≤1, Taylor's formula gives log⁡qun(Xi)=Yun(Xi)−14Yun(Xi)2+O(∣Yun(Xi)∣3), with one constant valid for all i,n by [F11], since the third derivative of y↦2log⁡(1+y/2) is bounded on [−1,1]. The total cubic remainder is bounded by a constant times max⁡i∣Yun(Xi)∣∑iYun(Xi)2, which tends to zero by the square-sum limit in step 2.2 and the maximum bound in step 2.3. Combining the sum expansion in step 3.1 with the square-sum limit gives log⁡Ln=∑ilog⁡qun(Xi)=hnTΔn−12hTIh+oP(1). This is the normalized log-likelihood expansion.

5.1F3F7givenalgebra∎

The full one-observation law decomposes as Pun=(1−αn)Pˉn+αnSn, where Sn is the normalized restriction of Pun to Sc when αn>0. In the product mixture, the probability that at least one coordinate is drawn from Sn is at most nαn. Conditioning on the all-absolutely-continuous component shows, for every event, its probability under the full product differs from that under Pˉn⊗n by at most nαn. Since nαn=o(n∥un∥22)=o(1), [F7] proves the total-variation claim. If αn=0, the singular component is absent and the same bound is zero.

TheoremStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

Local asymptotic minimax bound

Statement

Assume AC and let d≥1 be finite. Let {Pn,h:h∈Rd} be a finite-dimensional experiment that is LAN at h=0 with positive-definite information K and central sequence Δn⇒Nd(0,K) as in Local asymptotic normality for local experiments. Let M≥0 be finite and L:Rd→[0,M] be Borel measurable, symmetric (L(−x)=L(x)), and quasi-convex (each sublevel set is convex). Then lim inf⁡c→∞lim inf⁡n→∞inf⁡h^nsup⁡∥h∥2≤cEPn,hL(h^n−h)≥EL(Z),Z∼Nd(0,K−1). The infimum ranges over measurable, possibly randomized estimators. The experiment is pointwise LAN in each fixed h; no uniform likelihood-field assumption is added.

Facts & Assumptions

Given: AC; the pointwise LAN experiment with K≻0; and the stated bounded, Borel, symmetric quasi-convex loss.

[A1]

The Axiom of Choice: AC is assumed by the Gaussian and LAN prerequisites used here.

[F1]

Local asymptotic normality for local experiments: For each fixed h, there are mean-one likelihood proxies with pointwise log-likelihood expansion and total-variation approximation to the actual local law.

[F2]

Finite-prior Bayes envelopes converge under pointwise LAN: For a finite prior and a bounded Lipschitz loss, pointwise LAN makes the actual finite-prior Bayes values converge to those in the Gaussian shift.

[F3]

Finite priors approximate Gaussian-shift Bayes values: In the Gaussian shift, the Bayes value under any prior can be approximated arbitrarily closely by a finite-support prior, uniformly over decision rules.

[F4]

Bounded bowl-shaped losses have Gaussian-centered Lipschitz minorants: For every N≥2 and m≥1 it constructs a bounded Lipschitz minorant gN,m≤L and proves its Gaussian shift risk is minimized at the center; it also gives lim⁡N→∞lim⁡m→∞EgN,m(Z)=EL(Z).

[F5]

Loss functions and risk and Bayes risk and minimax risk: A rule's risk is its expected loss and its prior risk is rπ(δ). In this proof write BE(π,g):=inf⁡δrπ(δ) for the Bayes value in experiment E, with the infimum over measurable randomized estimators; this is local notation, since the supplier defines rπ and the minimax value but does not name a Bayes-value infimum. For any prior supported in a parameter set, every rule's worst-case risk on that set is at least its prior risk. Write Bn and BG for this value in the nth experiment and the Gaussian shift, respectively.

[F9]

Borel measurable and Lebesgue measurable functions on Rn: Borel measurability on Rd uses the sigma-algebra generated by its open sets.

Proof

Proof technique: compare finite-prior Bayes risks, compute a Gaussian prior Bayes value, then approximate the loss from below.

1.1F4F5F6F8givenconstructalgebra

If M=0, then L is identically zero and the claimed bound is equality. Assume M>0 for the rest of the proof. Fix arbitrary integers N≥2 and m≥1, and set g=gN,m from [F4]; it is bounded Lipschitz and g≤L. For each ρ>0, set Γ=ρ−1K−1, and let πΓ=Nd(0,Γ). Define Vn,c(g)=inf⁡h^nsup⁡∥h∥2≤cEPn,hg(h^n−h) and V(g)=lim inf⁡c→∞lim inf⁡n→∞Vn,c(g). If a finite prior πf is supported in the radius-c ball, then every worst-case risk is at least its prior average by [F5]. Taking infima gives Vn,c(g)≥Bn(πf,g), the finite-prior Bayes value.

2.1A1F4F6step 1.1givenalgebra

In the Gaussian shift, Y∣h∼Nd(h,K−1). Multiplying its likelihood by the prior density Nd(0,Γ) and completing the square gives H∣Y∼Nd(SKY,S),S=(K+Γ−1)−1. For the fixed constructed loss g=gN,m, [F4] gives that the posterior risk is minimized at SKY, with value Eg(Nd(0,S)) independent of Y. The action Y↦SKY is measurable and attains this value, so BG(πΓ,g)=Eg(Nd(0,S)).

2.2F1F2step 1.1givenalgebra

Let Cf=max⁡{∥h∥2:h∈supp⁡(πf)}. For every c≥Cf, [F2] gives Bn(πf,g)→BG(πf,g), where BG is the Bayes value in the Gaussian shift. Hence V(g)≥BG(πf,g). Since this holds for every finite prior, the bound also holds for any value approximated by finite-prior Bayes values.

3.1F3step 1.1step 2.2givenalgebra

For every η>0, [F3] supplies a finite prior πf whose Gaussian-shift Bayes value differs from BG(πΓ,g) by less than η. Step 2.2 therefore gives V(g)≥BG(πΓ,g)−η. Let η↓0 to obtain V(g)≥BG(πΓ,g).

4.1F6F7step 1.1step 2.1step 3.1algebra

Here S=(1+ρ)−1K−1. Couple Nd(0,S) as (1+ρ)−1/2Z for Z∼Nd(0,K−1). If Bg is a Lipschitz constant for g, then ∣Eg((1+ρ)−1/2Z)−Eg(Z)∣≤Bg(1−(1+ρ)−1/2)E∥Z∥2→0 as ρ↓0 by [F7]. By steps 3.1 and 2.1, for each ρ>0 we have V(g)≥Eg((1+ρ)−1/2Z). Since the construction applies for every ρ>0, taking ρ↓0 yields V(g)≥Eg(Z).

5.1F4F9step 1.1step 4.1givenalgebra∎

Since g≤L, every estimator's risk under L dominates its risk under this fixed g, so the local minimax value for L is at least V(g). Step 4.1 gives the lower bound EgN,m(Z). The choices N,m in step 1.1 were arbitrary; first let m→∞ and then N→∞. By [F4] these lower bounds converge to EL(Z). This is the stated inequality.

TheoremStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Quadratic-mean differentiability implies iid LAN

Statement

Assume the Axiom of Choice. Let {Pθ:θ∈Θ⊆Rd} be dominated by a common sigma-finite measure, with Θ open, and suppose the model is QMD at an interior θ0 with score s and information I=Eθ0[ssT]. Let X1,…,Xn be IID Pθ0, and for each fixed local sequence hn→h set un=hn/n. Then the local product laws Pθ0+un⊗n admit mean-one likelihood-ratio proxies Ln relative to Pθ0⊗n such that ∥Pθ0+un⊗n−LnPθ0⊗n∥TV→0, and under Pθ0⊗n, log⁡Ln=hnTΔn−12hTIh+oP(1),Δn=n−1/2∑i=1ns(Xi)⇒Nd(0,I). Thus the IID QMD experiment is LAN in the proxy sense of Local asymptotic normality for local experiments. This assertion does not claim that the full local product law has a Radon–Nikodym derivative relative to the base law.

Facts & Assumptions

Given: AC; the QMD model, common dominator, score, and information above; and IID observations from Pθ0.

[A1]

The Axiom of Choice: AC is the stated set-theoretic axiom. It is assumed here because the multivariate IID CLT supplier explicitly assumes it.

[L1]

Likelihood densities: The chosen density versions satisfy Pθ(A)=∫Apθ dμ for every measurable A.

[F1]

Quadratic-mean differentiability at a parameter: At θ0, the square-root densities have an L2(μ) first-order expansion with score s.

[F2]

Normalized product likelihood expansion under QMD: For every hn→h, the normalized absolutely continuous product proxy has mean-one likelihood Ln, differs from the full product law in total variation by o(1), has Pθ0⊗n(Ln=0)→0, and its log likelihood has expansion hnTΔn−12hTIh+oP(1).

[F3]

Multivariate iid central limit theorem: Under AC and for a finite integer d≥1, IID vectors with finite second moment and covariance I satisfy n−1/2∑i(Xi−EXi)⇒Nd(0,I); singular I is allowed.

[F4]

Local asymptotic normality for local experiments: LAN means a Gaussian central-sequence limit, the stated log-likelihood expansion for each fixed local direction, and a total-variation-close mean-one absolutely continuous proxy.

[F5]

The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn: The local directions and score sums use the Euclidean inner product and norm on Rd.

[F6]

A QMD score is centered and has finite information: A QMD score has mean zero and finite positive-semidefinite information matrix.

Proof

Proof technique: combine the normalized QMD likelihood expansion with the score central limit theorem.

1.1F4F5givenconstructalgebra

If d=0, the parameter space containing θ0 is the singleton empty tuple by [F5]. Thus hn=h=0, un=0, and every local law equals the base law. The score and Δn are empty vectors and I is the empty matrix. Choose Ln=1: its mean is one, the total variation error is zero, and the log expansion is the exact identity 0=0. The law of Δn is the unique law on the singleton, denoted N0(0,0) under the empty-tuple convention; its weak convergence is immediate. These facts give LAN by [F4] without a CLT. Henceforth suppose d≥1.

2.1A1F1F2L1step 1.1given

By [A1, L1, F1] the path is QMD with the specified density versions. [F2] applies to the chosen sequence un=hn/n and supplies the normalized proxy Ln, the total variation approximation, and the log expansion. Its normalizer is 1−αn>0 for all sufficiently large n, since αn=o(∥un∥22) and un→0.

2.2A1F1F3F5F6step 1.1given

By [F6], the score has Eθ0s=0 and covariance Eθ0[ssT]=I with finite entries. QMD also supplies Eθ0∥s∥22<∞ by [F1]. Thus [F3] applies to s(Xi) and yields Δn⇒Nd(0,I), including singular information.

3.1F2F4step 1.1step 2.1step 2.2∎

For each fixed h, steps 2.1 and 2.2 give the proxy approximation, the log expansion and the Gaussian central-sequence limit required in [F4]. Hence the local experiment is LAN. The proof used the full likelihood only for the normalized absolutely continuous component; singular mass is handled by the total-variation bound in [F2]. This proves the stated proxy-LAN conclusion.

5 · Examples, counterexamples and false statements

None yet.

Sources