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A rank-one finite-dimensional Gaussian process is a tight Banach prior

Example

Assume AC.

Take T={1,2}, B=R2, and Z∼N(0,1). Define X1=Z and X2=2Z. This is a singular finite Gaussian process and its coordinate vector is a tight Borel Gaussian random element of B.

Facts & Assumptions

[F1]

A symmetric positive-semidefinite kernel on a finite index set defines the corresponding Gaussian process law (A mean and positive-semidefinite kernel define a Gaussian process).

[F2]

The standard normal has mean zero, variance one, and density (2π)−1/2e−z2/2 (Standard normal and normal laws, Multivariate normal law, including singular covariance).

[F3]

The covariance operator and RKHS are defined from Cℓ=E[ℓ(W)W] and the covariance quotient norm (Covariance operator and reproducing-kernel Hilbert space of a Banach Gaussian).

[F4]

Probability is continuous from below on increasing events (Continuity from below for measures).

[F5]

The one-dimensional Gaussian integral is ∫Re−cx2dx=π/c for c>0 (The Gaussian integral ∫−∞∞e−x2 dx=π).

Verification

Given: AC, Z∼N(0,1), X=(X1,X2)=(Z,2Z), and B=R2 with its

Euclidean norm.

1.1F1F2givenalgebra

With v=(1,2), the mean is zero and E[XiXj]=vivj. The kernel k(i,j)=vivj is positive semidefinite because for all a1,a2, ∑i,jaiajk(i,j)=(a1+2a2)2≥0. Thus [F1] gives the same possibly singular Gaussian process law as the explicit vector.

1.2F2F4givenchoose

The map z↦(z,2z) is continuous, so its pushforward of the standard normal law is a Borel probability on B. For every positive integer R, the events {∣Z∣≤R} increase to the whole space; continuity from below [F4] therefore lets us choose R with P(∣Z∣≤R)>1−δ. The image segment {(z,2z):∣z∣≤R} is compact and has probability above 1−δ, so the law is tight.

2.1F2F3step 1.1algebra

For ℓa(x)=a1x1+a2x2, ℓa(X)=(a1+2a2)Z, and [F2] gives Cℓa=E[ℓa(X)X]=(a1+2a2)(1,2). The range is exactly span⁡{(1,2)}. If h=c(1,2), then every representative with a1+2a2=c has covariance norm squared E[ℓa(X)2]=c2, so ∥h∥H=∣c∣.

3.1F2F5step 1.1step 2.1algebra∎

The law is concentrated on this line. Every open ball around c(1,2) meets the line in an interval of positive normal probability, while a point outside the line has a sufficiently small ball disjoint from it. Hence the support is the line, equal to the RKHS. Since ∥X∥2=5Z2, [F2] and [F5] give Eea∥X∥2=Ee5aZ2=12π∫Re−(1/2−5a)z2 dz=(1−10a)−1/2<∞ for 0<a<1/10.

Depends on

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