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Likelihood-ratio limit for local cones in a QMD model

Statement

Assume the Axiom of Choice (The Axiom of Choice).

Let d≥1, let Θ0⊆Θ⊆Rd, and let θ0∈Θ0. Assume the full-model parameter set Θ is open in Rd, so θ0 is interior for the QMD model. Under Pθ0, let X1,…,Xn be IID and let ℓn(θ)=∑i=1nlog⁡pθ(Xi) be their sample log-likelihood. Define local parameter sets Cn:=n(Θ−θ0) and C0n:=n(Θ0−θ0). Assume the model is QMD at θ0 as in Quadratic-mean differentiability at a parameter, and write I:=Eθ0[sθ0sθ0T] for its Fisher information; assume I is positive definite, meaning vTIv>0 for every nonzero v. Suppose Cn and C0n are closed in the Euclidean metric (their complements are open), contain 0, and converge locally to nonempty closed convex cones C and C0 with C0⊆C. A cone contains 0 and is closed under multiplication by every nonnegative scalar; convex means that the set contains the line segment between each pair of its points. Local convergence means that, for every R>0, there are δn,R→0 such that every point of Cn∩B‾2(0,R) or C∩B‾2(0,R) is within δn,R in Euclidean distance of the other set, and likewise for C0n and C0. Here a point x is within δ of a set A when inf⁡a∈A∥x−a∥2≤δ.

Assume a uniform local quadratic likelihood expansion: for h∈Cn,

ℓn(θ0+h/n)−ℓn(θ0)=hTZn−12hTIh+rn(h),

where Zn⇒Z∼Nd(0,I) under Pθ0 and, for every R>0, sup⁡{∣rn(h)∣:h∈Cn, ∥h∥2≤R}→P0. Assume the full and null local log-likelihoods attain maxima at h^n∈Cn and h^0n∈C0n and that both maximizer sequences are tight, meaning that for every η>0 some R<∞ makes the limiting upper probability of either norm exceeding R at most η. For

Tn:=2[sup⁡h∈Cn{ℓn(θ0+h/n)−ℓn(θ0)}−sup⁡h∈C0n{ℓn(θ0+h/n)−ℓn(θ0)}],

the likelihood-ratio statistic satisfies

Tn⇒dI2(I−1Z,C0)−dI2(I−1Z,C),

where dI is the Fisher-information distance of Fisher-information metric distance to a set. QMD alone is not asserted to imply the uniform expansion or tightness hypotheses.

Facts & Assumptions

Given: AC, the model, local parameter sets, expansion, convergence, and tightness hypotheses in the Statement.

[A1]

The Axiom of Choice is assumed for the finite-dimensional normal-law convention used here (The Axiom of Choice).

[F1]

QMD at an interior point means the square-root-density expansion ∫[pθ0+h−pθ0−12hTsθ0pθ0]2dμ=o(∥h∥22) for a square-integrable score and common dominating measure (Quadratic-mean differentiability at a parameter).

[F2]

The Fisher distance is dI(x,A)=inf⁡a∈A(x−a)TI(x−a) (Fisher-information metric distance to a set).

[F3]

The Euclidean inner product is uTv and its norm is ∥u∥2 (The Euclidean inner product ⟨x,y⟩=∑k<nxkyk on Rn).

[F4]

B‾2(0,R)={h:∥h∥2≤R}, and the Euclidean metric has this norm as its distance (Euclidean spheres and closed balls as subspaces of Rn).

[F6]

For nonempty closed A, there is λ>0 with hTIh≥λ∥h∥22, and maximizing qz(h)=zTh−12hTIh over A gives 12zTI−1z−12dI2(I−1z,A); the maximum is attained (Quadratic likelihood optimization is squared Fisher distance).

[F7]

Under AC, Nd(0,I) is a Borel probability law with the stated covariance (Multivariate normal law, including singular covariance).

[F8]

Weak convergence of laws gives the closed-set upper bound lim sup⁡nP(Zn∈F)≤P(Z∈F) for each closed F (Portmanteau theorem).

[F9]

Continuous maps preserve convergence in distribution at points of continuity of the limiting law (Continuous mapping theorem).

[F10]

For real random variables, adding a term converging in probability to zero preserves convergence in distribution (Slutsky's theorem for real random variables).

[F11]

Convergence in probability means that every fixed positive error threshold is exceeded with probability tending to zero (Convergence in probability); convergence in distribution is weak convergence of the laws (Convergence in distribution of random elements).

Proof

Given: The objects and hypotheses in the Statement.

1.1F1F6F3F5givenalgebra

With the supplied QMD information I of [F1], write qz(h)=hTz−12hTIh and mA(z)=sup⁡h∈Aqz(h) for A=C,C0. By [F6], mA(z)=12zTI−1z−12dI2(I−1z,A). If hA(z) is a maximizer, then qz(hA(z))≥qz(0)=0. The lower bound in [F6] and [F5] imply ∥hA(z)∥2≤2∥z∥2/λ (with the bound immediate when hA(z)=0).

1.2F6F3F4F5givenalgebrachoose

Let λ be from [F6], fix M>0, and choose R>2M/λ+1. For An=Cn, A=C (and likewise for An=C0n, A=C0), write mAn,R(z)=sup⁡h∈An∩B‾2(0,R)qz(h). For every ∥z∥2≤M, [F6] gives a maximizer h(z) of qz on A with ∥h(z)∥2≤2M/λ<R−1. Local set convergence supplies points of An within δn,R−1+1/n of h(z), hence inside the radius-R ball for all large n. Conversely, every point of An∩B‾2(0,R) is within δn,R+1/n of a point of A. With BI=∑j,k=1d∣Ijk∣, [F3] and [F5] give ∣qz(h)−qz(h′)∣≤(M+BI(R+1))∥h−h′∥2 for ∥h∥2,∥h′∥2≤R+1 and ∥z∥2≤M. These two directions show sup⁡∥z∥2≤M∣mAn,R(z)−mA(z)∣→0. The same bounds apply to both full and null sets.

2.1A1F7F8step 1.1givenchoose

The sequence Zn is tight. Indeed, for any η>0 choose R with P(∥Z∥2≥R)<η, possible because [F7] supplies a Borel probability law on finite-dimensional Rd. The set {z:∥z∥2≥R} is closed, so [F8] bounds lim sup⁡nP(∥Zn∥2≥R) by η. step 1.1 then makes the maximizers of qZn over C and C0 tight as well.

2.2F11step 1.2given

For An=Cn or C0n, put LAn,R:=sup⁡h∈An∩B‾2(0,R){ℓn(θ0+h/n)−ℓn(θ0)}. The uniform expansion gives ∣LAn,R−mAn,R(Zn)∣≤sup⁡h∈Cn, ∥h∥2≤R∣rn(h)∣→P0 for each fixed R. For fixed M>0 and R>2M/λ+1, step 1.2 therefore gives, for every ε>0, P(∣LAn,R−mA(Zn)∣>ε, ∥Zn∥2≤M)→0, with A=C or C0, respectively.

3.1F11step 1.1step 2.2givenchoose

Given η>0, tightness of Zn lets us choose M so that ∥Zn∥2≤M with limiting probability at least 1−η/3. Choose R>2M/λ+1 large enough that the joint event that both local likelihood maximizers lie in the radius-R ball has limiting probability at least 1−η/3. By step 1.1 both quadratic maximizers also lie in that ball whenever ∥Zn∥2≤M. Thus all four full and truncated suprema agree except on events with total limiting upper probability at most 2η/3. step 2.2 and arbitrariness of η give Tn−2(mC(Zn)−mC0(Zn))→P0.

4.1F2F6F9F10step 1.1step 1.2step 3.1∎

The form ⟨u,v⟩I=uTIv is an inner product; its Cauchy–Schwarz inequality follows by requiring (u−tv)TI(u−tv)≥0 for every real t. Thus the induced norm satisfies the triangle inequality, and taking infima gives ∣dI(x,C)−dI(y,C)∣≤∥x−y∥I. Also vTIv≤BI∥v∥22, where BI is the finite entry sum from step 1.2, so the distance map is Euclidean Lipschitz after composition with the fixed linear map I−1. Therefore g(z):=dI2(I−1z,C0)−dI2(I−1z,C) is continuous. The formula in step 1.1 gives 2[mC(z)−mC0(z)]=g(z). By [F9], g(Zn)⇒g(Z). step 3.1 and [F10] then give Tn⇒g(Z), which is the stated distance-difference law.

Remarks

The uniform local expansion and tightness are explicit hypotheses. The proof does not infer uniformity over bounded local parameters from pointwise LAN, and it does not invoke the regular interior Wilks theorem at a boundary.

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