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Gaussian activation covariance and tangent recursion preserve strict positivity

Statement

Assume AC. Let m≥1, let C∈Rm×m be symmetric positive definite, let Z=(Z1,…,Zm) have the centered multivariate normal law with covariance C, let σ:R→R be globally Lipschitz and nonconstant, and let β>0. Let s be a bounded Borel representative of the almost-everywhere derivative of σ: it agrees with the ordinary derivative wherever that derivative exists, and its values on the remaining Lebesgue-null set are arbitrary. Define Sij:=E[σ(Zi)σ(Zj)]+β2,Dij:=E[s(Zi)s(Zj)](1≤i,j≤m). Then S is strictly positive definite and D is positive semidefinite. Consequently, for every positive-semidefinite matrix T∈Rm×m, the matrix T∘D+S is strictly positive definite, where ∘ denotes entrywise multiplication.

Facts & Assumptions

Given: AC; a finite positive-definite covariance matrix C; its centered multivariate normal vector Z; a globally Lipschitz nonconstant activation σ; and β>0.

[A1]

AC supplies countable and dependent choice, as needed by the Gaussian-law and absolute-continuity interfaces (The Axiom of Choice, AC supplies countable selections and prescribed serial paths).

[F1]

On every compact interval a Lipschitz function is absolutely continuous, and an absolutely continuous function has an integrable derivative almost everywhere whose integral recovers its increments (C1 implies Lipschitz, Lipschitz implies absolutely continuous, and absolutely continuous implies continuous and bounded variation, Fundamental theorem of calculus for absolutely continuous functions).

[F2]

A finite centered multivariate normal vector with covariance C is realized as C1/2G for independent standard-normal coordinates Gj; each coordinate has the corresponding scalar normal law (Multivariate normal law, including singular covariance, Standard normal and normal laws).

[F3]
[F4]

Expectations of integrable variables are linear and satisfy Cauchy–Schwarz (Linearity, monotonicity, and the modulus bound for expectation, Cauchy-Schwarz for random variables).

Proof

technique · direct
1.1A1F1givenconstruct

On every compact interval, [F1] gives differentiability of σ outside a null set. Taking a countable union over intervals [−n,n] gives one Lebesgue-null exceptional set on R. The continuous difference quotients sn(x)=n(σ(x+1/n)−σ(x)) are bounded in modulus by the Lipschitz constant; their pointwise upper limit is a bounded Borel function and equals σ′(x) wherever the derivative exists. Thus a representative s as in the Statement exists.

1.2F2givenalgebra

Let A=C1/2 and G be the independent standard-normal vector in [F2]. Positive definiteness of C makes A invertible: if Av=0, then vTCv=vTA2v=∥Av∥22=0, so v=0. The product standard-normal density is positive on every nonempty open box; since A−1 maps nonempty open sets to nonempty open sets, Z=AG assigns positive probability to every nonempty open set in Rm.

2.1F2step 1.1

By [F2], each Zi has a scalar normal law with variance Cii>0, hence a density. Therefore changing s on the exceptional null set changes none of the random variables s(Zi) almost surely.

2.2step 1.2givenalgebrachoose

Fix a nonzero vector c∈Rm and set F(z)=∑i=1mciσ(zi). This function is continuous. If E[F(Z)2]=0, then for every integer k≥1, F(Z)2≥k−21{∣F(Z)∣≥1/k} forces P(∣F(Z)∣≥1/k)=0; the countable union gives F(Z)=0 almost surely. By the full-support conclusion of step 1.2, continuity forces F(z)=0 for every z∈Rm. Choose u,v with σ(u)≠σ(v). For each j, evaluate this identity at vectors whose coordinates other than j are zero and whose jth coordinates are u and v, then subtract; it gives cj(σ(u)−σ(v))=0, so cj=0. This contradicts c≠0. Hence E[F(Z)2]>0 and cTSc=E[F(Z)2]+β2(∑ici)2>0.

3.1F4step 2.1algebra

For any c∈Rm, cTDc=E[(∑icis(Zi))2]≥0; the expectation is finite because s is bounded. Thus D is positive semidefinite.

4.1F3step 3.1construct

Apply [F3] to T. Each eigenvalue λ is nonnegative because for a unit eigenvector q, λ=qTTq≥0. If q1,…,qm is an orthonormal eigenbasis with eigenvalues λ1,…,λm, the vectors ui=(λ1(q1)i,…,λm(qm)i) satisfy Tij=⟨ui,uj⟩. For D, the same finite-dimensional factorization applies because step 3.1 proves it is positive semidefinite, so there are vectors vi with Dij=⟨vi,vj⟩.

5.1step 2.2step 4.1algebra∎

Then (T∘D)ij=⟨ui⊗vi,uj⊗vj⟩, so T∘D is positive semidefinite. Adding the strictly positive quadratic form of S from step 2.2 shows T∘D+S is strictly positive definite.

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