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The Lifted Free Score: Norm, Weak Identity and the Second-Moment Identity

For a square-integrable random variable whose law has finite free Fisher information, the lifted free score has squared norm equal to the free Fisher information and pairs with the lifted derivative of a test function to the integral of the difference quotient against the product measure; and the free score of any law with finite free Fisher information pairs with the identity map to one, so the lifted free score pairs with the random variable itself to one.

Statement

In the setting of Square-Integrable Vector Fields Against a Probability Measure on Euclidean Space, and Test Functions: Standing Notation, in dimension d=1d=1, with the real line identified with R1\mathbb{R}^{1} and R2=R1+1\mathbb{R}^{2}=\mathbb{R}^{1+1} as in One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative. Let X∈L2(Ω;R)X\in L^{2}(\Omega;\mathbb{R}) and let μ=L(X)\mu=\mathcal{L}(X) be its law, which belongs to P2(R)\mathcal{P}_{2}(\mathbb{R}) by The Space of Square-Integrable Random Vectors is a Real Hilbert Space; Its Laws Have Finite Second Moment; Constants and Translations (ii). Let id\mathrm{id} be the identity map of R\mathbb{R}, an element of L2(ν;R)L^{2}(\nu;\mathbb{R}) for every ν∈P2(R)\nu\in\mathcal{P}_{2}(\mathbb{R}) by Basic Properties of the Tangent Space: Closed Subspace, the Identity Map Belongs to It, Second-Moment Limits, and Representation of Bounded Functionals on Gradients (ii); for ξ∈L2(μ;R)\xi\in L^{2}(\mu;\mathbb{R}) let ξ∘X∈L2(Ω;R)\xi\circ X\in L^{2}(\Omega;\mathbb{R}) be the composition; for ψ∈Cc∞(R)\psi\in C_{c}^{\infty}(\mathbb{R}) let ψ′=∇ψ\psi'=\nabla\psi be its derivative and FψF_{\psi} the difference quotient of its derivative; and let finite free Fisher information, the set P2Φ∗(R)\mathcal{P}_{2}^{\Phi^{*}}(\mathbb{R}), the free score Ξν\Xi_{\nu} and the free Fisher information Φ∗(ν)\Phi^{*}(\nu) of a ν∈P2Φ∗(R)\nu\in\mathcal{P}_{2}^{\Phi^{*}}(\mathbb{R}) be as defined there.

1. (The lifted free score) If μ∈P2Φ∗(R)\mu\in\mathcal{P}_{2}^{\Phi^{*}}(\mathbb{R}), then ∥Ξμ∘X∥L22=Φ∗(μ)\lVert\Xi_{\mu}\circ X\rVert_{L^{2}}^{2}=\Phi^{*}(\mu) and, for every ψ∈Cc∞(R)\psi\in C_{c}^{\infty}(\mathbb{R}),

⟨Ξμ∘X,ψ′∘X⟩L2=∫R2Fψ d(μ⊠μ).\langle\Xi_{\mu}\circ X,\psi'\circ X\rangle_{L^{2}}=\int_{\mathbb{R}^{2}}F_{\psi}\,d(\mu\boxtimes\mu).

2. (Second-moment identity) For every ν∈P2Φ∗(R)\nu\in\mathcal{P}_{2}^{\Phi^{*}}(\mathbb{R}), whether or not it is the law of an element of L2(Ω;R)L^{2}(\Omega;\mathbb{R}), ⟨Ξν,id⟩ν=1\langle\Xi_{\nu},\mathrm{id}\rangle_{\nu}=1. In particular, if μ∈P2Φ∗(R)\mu\in\mathcal{P}_{2}^{\Phi^{*}}(\mathbb{R}), then

⟨Ξμ∘X,X⟩L2=1.\langle\Xi_{\mu}\circ X,X\rangle_{L^{2}}=1 .

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