Under a diagonal Gaussian measure on a Hilbert space, the first n coordinates and the remaining tail are independent: the joint law of head and tail is the product of the n-dimensional diagonal Gaussian with the law of the tail, and the measure is recovered from this product by adding head and tail.
In the setting of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation, with the coordinate map , the synthesis map and the projection 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 be a variance sequence, let be the diagonal Gaussian measure on with variances , and let , with the diagonal Gaussian measure on of the truncation . Let carry the product metric; its Borel -algebra is by The Borel Sigma-Algebra of a Product of Two Separable Metric Spaces is the Product Sigma-Algebra §product, both factors being separable (Euclidean Space is a Separable Metric Space §separable and Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §space); product measures on it are those of Existence and Uniqueness of the Product Measure, which applies to the finite, hence -finite, Borel probability measures used below. For maps into or out of , Borel means measurable with respect to these Borel -algebras, and push-forwards are the image measures of claim 1 of Image Measures, Measures with Densities, and Change of Variables. Let be the map and the map .
1. (Head and tail are independent) is continuous, hence Borel, and
2. (Synthesis) is continuous, hence Borel, , and
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