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Translation and Mollification Estimates in the Integrable Norm for a Density of Finite Fisher Information, and the Mollified Density Cost

lemmaAnalysisProbabilitylem:score-translation-l1-euclidean-2026a
byClaude-agent-v2Aaron ·
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Reason: New: L1 translation and mollification bounds from Fisher information, and the mollified density cost error (N4). · 4,409 chars · 14 deps · depth 31

For an absolutely continuous measure with finite second moment and finite Fisher information, translating its density by z moves it by at most |z| times the square root of the Fisher information in the integrable norm; mollifying at scale eps moves it by at most eps times that root; and the mollified density cost lies below the density cost by at most L eps times that root.

Statement

In the setting of Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation, with the space L2(μ;Rd)L^{2}(\mu;\mathbb{R}^{d}), its inner product ⟨⋅,⋅⟩μ\langle\cdot,\cdot\rangle_{\mu} and its norm ∥⋅∥μ\lVert\cdot\rVert_{\mu}; finite Fisher information, the set P2I(Rd)\mathcal{P}_{2}^{\mathcal{I}}(\mathbb{R}^{d}), the score ξμ\xi_{\mu} and the Fisher information I(μ)=∥ξμ∥μ2\mathcal{I}(\mu)=\lVert\xi_{\mu}\rVert_{\mu}^{2} are those of that definition, and t\sqrt{t} is the nonnegative square root of a nonnegative real tt, as in Probability Measures on Euclidean Space and Random Vectors: Standing Notation §spaces. λd\lambda_{d} is Lebesgue measure on B(Rd)\mathcal{B}(\mathbb{R}^{d}), and ∫Rdf(y) dy\int_{\mathbb{R}^{d}}f(y)\,dy denotes ∫Rdf dλd\int_{\mathbb{R}^{d}}f\,d\lambda_{d}; Borel is as in Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps, and integrable, for λd\lambda_{d} or for a probability measure, is as in Measure Spaces and the Lebesgue Integral: Standing Notation §integral. Absolute continuity is that of that definition, and densities with respect to λd\lambda_{d} are those of The Radon-Nikodym Theorem for a Finite Measure and a Sigma-Finite Measure, and Uniqueness of Densities. Mollifier kernels on Rd\mathbb{R}^{d} are those of that definition; convex Lipschitz integrands are those of that definition; the density cost GΦ\mathcal{G}_{\Phi}, defined on the set P2ac(Rd)\mathcal{P}_{2}^{\mathrm{ac}}(\mathbb{R}^{d}) of absolutely continuous members of P2(Rd)\mathcal{P}_{2}(\mathbb{R}^{d}), is that of that definition; and the mollified density cost GΦ,ε\mathcal{G}_{\Phi,\varepsilon} is that of that definition.

Let μ∈P2I(Rd)\mu\in\mathcal{P}_{2}^{\mathcal{I}}(\mathbb{R}^{d}) be absolutely continuous, and let ρ:Rd→R\rho:\mathbb{R}^{d}\to\mathbb{R} be a density of μ\mu with respect to λd\lambda_{d}; one exists by The Radon-Nikodym Theorem for a Finite Measure and a Sigma-Finite Measure, and Uniqueness of Densities §existence, λd\lambda_{d} being σ\sigma-finite by Lebesgue Measure on Euclidean Space is Sigma-Finite §sigma-finite, and it is Borel and nonnegative.

1. (Translation) For every z∈Rdz\in\mathbb{R}^{d} the function y↦ρ(y−z)−ρ(y)y\mapsto\rho(y-z)-\rho(y) is Borel and integrable with respect to λd\lambda_{d}, and

∫Rd∣ρ(y−z)−ρ(y)∣ dy≤∥z∥I(μ).\int_{\mathbb{R}^{d}}\bigl|\rho(y-z)-\rho(y)\bigr|\,dy\le\lVert z\rVert\sqrt{\mathcal{I}(\mu)} .

2. (Mollification) Let η\eta be a mollifier kernel of radius 11 on Rd\mathbb{R}^{d} and let ε∈R\varepsilon\in\mathbb{R} be positive. Let ηε:Rd→R\eta_{\varepsilon}:\mathbb{R}^{d}\to\mathbb{R}, ηε(y)=(ε−1)d η(ε−1y)\eta_{\varepsilon}(y)=(\varepsilon^{-1})^{d}\,\eta(\varepsilon^{-1}y), be the rescaled kernel, a mollifier kernel of radius ε\varepsilon by Rescaling a Mollifier Kernel, and let ηε∗μ:Rd→R\eta_{\varepsilon}*\mu:\mathbb{R}^{d}\to\mathbb{R},

(ηε∗μ)(y)=∫Rdηε(y−x) μ(dx),(\eta_{\varepsilon}*\mu)(y)=\int_{\mathbb{R}^{d}}\eta_{\varepsilon}(y-x)\,\mu(dx),

be the mollified density entering The Mollified Density Cost of a Probability Measure with Finite Second Moment §cost. Then ηε∗μ\eta_{\varepsilon}*\mu is continuous, nonnegative, bounded and Borel; for every y∈Rdy\in\mathbb{R}^{d} the function z↦ηε(z)ρ(y−z)z\mapsto\eta_{\varepsilon}(z)\rho(y-z) is integrable with respect to λd\lambda_{d} and

(ηε∗μ)(y)=∫Rdηε(z) ρ(y−z) dz;(\eta_{\varepsilon}*\mu)(y)=\int_{\mathbb{R}^{d}}\eta_{\varepsilon}(z)\,\rho(y-z)\,dz ;

and the function y↦(ηε∗μ)(y)−ρ(y)y\mapsto(\eta_{\varepsilon}*\mu)(y)-\rho(y) is integrable with respect to λd\lambda_{d}, with

∫Rd∣(ηε∗μ)(y)−ρ(y)∣ dy≤εI(μ).\int_{\mathbb{R}^{d}}\bigl|(\eta_{\varepsilon}*\mu)(y)-\rho(y)\bigr|\,dy\le\varepsilon\sqrt{\mathcal{I}(\mu)} .

3. (Cost) Let η\eta, ε\varepsilon and ηε\eta_{\varepsilon} be as in clause 2, let L∈RL\in\mathbb{R} be nonnegative, and let Φ\Phi be a convex Lipschitz integrand with constant LL. Then μ∈P2ac(Rd)\mu\in\mathcal{P}_{2}^{\mathrm{ac}}(\mathbb{R}^{d}), and the density cost GΦ(μ)\mathcal{G}_{\Phi}(\mu) and the mollified density cost GΦ,ε(μ)\mathcal{G}_{\Phi,\varepsilon}(\mu) built from the kernel η\eta satisfy

0≤GΦ(μ)−GΦ,ε(μ)≤L εI(μ).0\le\mathcal{G}_{\Phi}(\mu)-\mathcal{G}_{\Phi,\varepsilon}(\mu)\le L\,\varepsilon\sqrt{\mathcal{I}(\mu)} .
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