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Finite Sudakov–Fernique comparison for Gaussian maxima

Statement

Assume AC. Let m≥2, and let X,Y∈Rm be independent, centered Gaussian vectors with finite covariance matrices. If

E[(Xi−Xj)2]≥E[(Yi−Yj)2](i,j∈{1,…,m}),

then E[max⁡iXi]≥E[max⁡iYi].

Facts & Assumptions

Given: AC and independent centered Gaussian vectors X,Y∈Rm satisfying the displayed increment-variance inequalities.

[A1]

Under AC, Multivariate normal law, including singular covariance constructs C1/2Z with law Nm(0,C) for C⪰0 and independent standard-normal coordinates Z. The uniqueness assertion of Characteristic function of a multivariate normal law identifies this law with that of any given centered Gaussian vector of covariance C, including singular C (The Axiom of Choice).

[F1]

A standard normal coordinate has density ϕ(x)=(2π)−1/2e−x2/2, with ϕ′(x)=−xϕ(x) (Standard normal and normal laws).

[F2]

A product of sigma-finite measure spaces has a product measure with the rectangle formula (For sigma-finite factors, the product measure exists, has the rectangle formula, is sigma-finite, and is unique).

[F3]

Dominated convergence permits passage to limits when the integrands have an integrable common majorant (Dominated convergence).

[F4]

An integrable function on a sigma-finite product can be integrated in either order (Fubini's theorem for L^1 functions on a sigma-finite product).

Proof

1.1givenconstructalgebra

For a>0 define Φa(x)=a−1log⁡∑i=1meaxi and pi(x)=eaxi/∑jeaxj. Direct differentiation gives ∂iΦa=pi and ∂ijΦa=a(pi1i=j−pipj), while max⁡ixi≤Φa(x)≤max⁡ixi+log⁡(m)/a.

2.1A1F1F2F3F4step 1.1algebra

Let CX,CY be the covariance matrices. By [A1], on a product probability space [F2] replace X,Y by copies X=CX1/2ξ, Y=CY1/2η with the same respective laws, where all coordinates of ξ,η are independent standard normals. The desired expectations depend only on these laws. Put Zt=tX+1−tY and Fa(t)=EΦa(Zt). For 0<t<1, differentiate under the expectation; on every closed subinterval of (0,1) the derivative is bounded by a constant times ∥ξ∥2+∥η∥2, which is integrable since ∫R∣x∣ϕ(x) dx=2/π. Thus [F3] applies. Using [F4] to integrate one standard-normal coordinate at a time, one-dimensional integration by parts against [F1], with the bounded first and second derivatives from step 1.1, gives Fa′(t)=12∑i,j(CX−CY)ij E[∂ijΦa(Zt)]. The boundary terms vanish because ϕ(x) decays to zero and ∂iΦa is bounded.

3.1F3step 1.1step 2.1givenalgebra

Substituting the Hessian from step 1.1 into step 2.1 and using ∑ipi=1 rewrites the derivative as Fa′(t)=a4E[∑i,jpi(Zt)pj(Zt)(E[(Xi−Xj)2]−E[(Yi−Yj)2])]≥0. Hence Fa is nondecreasing on (0,1). For all t∈[0,1], ∣Φa(Zt)∣≤∥X∥2+∥Y∥2+log⁡(m)/a, an integrable bound, so [F3] gives continuity at the endpoints and therefore Fa(1)≥Fa(0).

4.1step 1.1step 3.1algebra∎

The uniform approximation in step 1.1 gives ∣EΦa(X)−Emax⁡iXi∣≤log⁡(m)/a and the analogous bound for Y. Letting a→∞ in step 3.1 proves the asserted comparison.

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