TheoremBase

The Diagonal Gaussian Random Series in a Hilbert Space: Almost Sure Convergence, Finite-Dimensional Projections, and the Unique Measure with Diagonal Gaussian Projections

For positive summable variances and independent standard normal coefficients, the random series of the scaled basis vectors converges almost surely to a random element of the Hilbert space whose finite-dimensional projections are diagonal Gaussian; exactly one Borel probability measure has these projections.

Statement

In the setting of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation, with the coordinate maps pnp_{n} of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §coordinates and push-forwards as in Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §pushforward, let cc be a variance sequence, with truncations c(n)c^{(n)} and diagonal Gaussian measures γc(n)\gamma_{c^{(n)}} on Rn\mathbb{R}^{n} (n∈Nn\in\mathbb{N}), and let s\sqrt{s} be the nonnegative square root of a nonnegative real number ss.

Claims 1 to 3 concern a probability space (Ω,F,P)(\Omega,\mathcal{F},P) and an independent sequence (ξk)k∈N(\xi_{k})_{k\in\mathbb{N}} of standard normal random variables on it. For n∈Nn\in\mathbb{N} let Yn:Ω→XY_{n}:\Omega\to X be the map Yn(ω)=∑k=1nck ξk(ω) ekY_{n}(\omega)=\sum_{k=1}^{n}\sqrt{c_{k}}\,\xi_{k}(\omega)\,e_{k}, and let GG be the set of those ω∈Ω\omega\in\Omega for which the series ∑k=1∞ck ξk(ω)2\sum_{k=1}^{\infty}c_{k}\,\xi_{k}(\omega)^{2} converges. Define Y:Ω→XY:\Omega\to X (well defined by claim 1) by Y(ω)=lim⁡n→∞Yn(ω)Y(\omega)=\lim_{n\to\infty}Y_{n}(\omega), the limit in (X,d)(X,d), for ω∈G\omega\in G, and Y(ω)=0XY(\omega)=0_{X} for ω∉G\omega\notin G.

1. (Almost sure convergence) G∈FG\in\mathcal{F}, P(G)=1P(G)=1, and for every ω∈G\omega\in G the sequence (Yn(ω))n∈N(Y_{n}(\omega))_{n\in\mathbb{N}} converges in (X,d)(X,d).

2. (A random element) YY is a random element of (X,d)(X,d), and ⟨Y(ω),ek⟩=ck ξk(ω)\langle Y(\omega),e_{k}\rangle=\sqrt{c_{k}}\,\xi_{k}(\omega) for every ω∈G\omega\in G and every k∈Nk\in\mathbb{N}.

3. (Projections) The law PYP_{Y} of YY belongs to P(X)\mathcal{P}(X), and (pn)#PY=γc(n)(p_{n})_{\#}P_{Y}=\gamma_{c^{(n)}} for every n∈Nn\in\mathbb{N}.

4. (The unique measure with these projections) There is exactly one μ∈P(X)\mu\in\mathcal{P}(X) such that (pn)#μ=γc(n)(p_{n})_{\#}\mu=\gamma_{c^{(n)}} for every n∈Nn\in\mathbb{N}. For every probability space and every independent sequence of standard normal random variables on it, this μ\mu is the law PYP_{Y} of the corresponding map YY defined above.

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