The diagonal Gaussian measure has relative score zero and zero weighted Fisher information; and a measure with finite weighted Fisher information has a unique score field in the square-integrable maps into the weighted sequence space, whose squared norm is the Fisher information.
In the settings of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation and Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation, let be a variance sequence and the diagonal Gaussian measure on with variances ; is the set of The Second Moment of a Borel Probability Measure on a Hilbert Space and the Probability Measures with Finite Second Moment §space; the relative score with respect to and its components are those of that definition, with as there; weight sequences, finite Fisher information relative to with weights and its value are those of Weight Sequences and the Weighted Fisher Information Relative to a Diagonal Gaussian Measure on a Hilbert Space §information.
1. (The Gaussian measure) , and has a relative score with respect to , every component of which is the zero vector of . Consequently, for every weight sequence , has finite Fisher information relative to with weights , and .
2. (The score field) Let be a weight sequence, let be the weighted sequence space with its standard orthonormal basis , a real Hilbert space by Weighted Square-Summable Sequence Spaces are Real Hilbert Spaces: the Standard Orthonormal Basis and the Embedding of a Hilbert Space under Bounded Weights §hilbert, and let have a relative score with respect to and finite Fisher information relative to with weights . Let be the space of square-integrable maps from the measure space to with the basis , with the norm of The Space of Square-Integrable Maps from a Measure Space into a Hilbert Space with an Orthonormal Basis §operations and the coordinates of its elements along given by The Space of Square-Integrable Hilbert-Valued Maps is a Real Hilbert Space: Coordinates and Synthesis §coordinates. Then there is exactly one with for every , where is the power of with exponent , and
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