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Moments of a Diagonal Gaussian Measure on a Hilbert Space: Coordinate Covariances, Finite Second Moment, and Exponential Moments of the Squared Norm

Under a diagonal Gaussian measure the coordinates are centred and uncorrelated with variances given by the variance sequence, the second moment is the sum of the variances, and the squared norm has exponential moments below the threshold set by the largest variance.

Statement

In the setting of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation, with the coordinates xkx_{k} of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §coordinates and integrability as in Measure Spaces and the Lebesgue Integral: Standing Notation, let cc be a variance sequence and γc\gamma_{c} the diagonal Gaussian measure on XX with variances cc, and let exp⁡\exp be the exponential function.

1. (Coordinates) For all j,k∈Nj,k\in\mathbb{N} the functions x↦xkx\mapsto x_{k} and x↦xjxkx\mapsto x_{j}x_{k} are Borel and integrable with respect to γc\gamma_{c}, ∫Xxk γc(dx)=0\int_{X}x_{k}\,\gamma_{c}(dx)=0, and

∫Xxjxk γc(dx)={ckif j=k,0if j≠k.\int_{X}x_{j}x_{k}\,\gamma_{c}(dx)=\begin{cases}c_{k}&\text{if }j=k,\\0&\text{if }j\ne k.\end{cases}

2. (Second moment) γc∈P2(X)\gamma_{c}\in\mathcal{P}_{2}(X) in the sense of The Second Moment of a Borel Probability Measure on a Hilbert Space and the Probability Measures with Finite Second Moment §space, and its second moment is M2(γc)=∑k=1∞ckM_{2}(\gamma_{c})=\sum_{k=1}^{\infty}c_{k}.

3. (Exponential moments) Let α,θ∈R\alpha,\theta\in\mathbb{R} with 0≤α0\le\alpha and θ<1\theta<1, and suppose that 2αck≤θ2\alpha c_{k}\le\theta for every k∈Nk\in\mathbb{N}. Then the function x↦exp⁡(α∣x∣2)x\mapsto\exp(\alpha|x|^{2}) is Borel and integrable with respect to γc\gamma_{c}, and

∫Xexp⁡(α∣x∣2) γc(dx)≤exp⁡(α1−θ∑k=1∞ck).\int_{X}\exp\bigl(\alpha|x|^{2}\bigr)\,\gamma_{c}(dx)\le\exp\Bigl(\frac{\alpha}{1-\theta}\sum_{k=1}^{\infty}c_{k}\Bigr).

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