The Gaussian reference measure is the Gaussian-tail extension of its rescaled head; extensions keep the head law, carry densities, relative entropy and relative score over from the head, and are no farther apart in the noise Wasserstein distance than their heads are in the Euclidean one. The relative entropies of the rescaled heads of a measure increase to its relative entropy.
6. (Densities) Let λ∈P(Rn) have a density f with respect to γ~n. Then f∘rn is a density of En(λ) with respect to γc.
7. (Relative entropy) A measure λ∈P(Rn) has finite relative entropy with respect to γ~n if and only if En(λ) has finite relative entropy with respect to γc, and then H(En(λ)∣γc)=H(λ∣γ~n).
8. (A Gaussian head with an arbitrary tail) Let σ∈P(X) have finite relative entropy with respect to τn. The product measureγ~n⊗σ on B(Rn)⊗B(X) exists, both factors being finite, and is a probability measure, its value on Rn×X being γ~n(Rn)σ(X)=1; and Ψn is Borel by The Gaussian-Tail Extension of a Probability Measure on the Rescaled Head §borel. Then (Ψn)#(γ~n⊗σ) has finite relative entropy with respect to γc, and
H((Ψn)#(γ~n⊗σ)γc)≤H(σ∣τn).
9. (Relative entropy of the rescaled heads) Let μ∈P(X) have finite relative entropy with respect to γc. Then for every m∈N the measure μ~m has finite relative entropy with respect to γ~m and H(μ~m∣γ~m)=H((pm)#μ∣γc(m)); the sequence (H(μ~m∣γ~m))m∈N is nondecreasing and converges to H(μ∣γc).
10. (Relative score) Let λ∈P2(Rn) have finite Fisher information relative to γ~n, and for k∈[n] let gk:Rn→R be a Borel representative of the component (ζλc~(n))k∈L2(λ). Then En(λ), which lies in P2(X) by claim 5, has a relative score (ζk)k∈N with respect to γc, where for k∈[n] the component ζk is the class of ak−1/2(gk∘rn), which is square-integrable with respect to En(λ) with a class independent of the choice of gk by claim 3 and the change-of-variables formula of Borel Probability Measures on a Real Hilbert Space with an Orthonormal Basis: Standing Notation §pushforward, and where ζk=0 for k>n.
11. (Fisher information) In the situation of claim 10, En(λ) has finite Fisher information relative to γc with weights a, and Ia(En(λ)∣γc)=I(λ∣γ~n).
12. (Noise Wasserstein distance) For λ,λ′∈P2(Rn), the measures En(λ) and En(λ′) belong to Pρa, and
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