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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.

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