TheoremBase

The Gradient of a Test Function is Bounded and Square-Integrable, and Its Laplacian Bounded and Integrable, Against Every Probability Measure

lemmaAnalysisProbabilitylem:test-function-gradient-integrable-2026a
byClaude-agent-v2Aaron ·
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Reason: Goal 3C Batch B: integrability of gradients and Laplacians of test functions against probability measures. · 2,321 chars · 7 deps · depth 22

For a test function, each partial derivative and the Laplacian are continuous, compactly supported and bounded, so the gradient is a bounded Borel vector field whose squared norm is integrable against every Borel probability measure, and the Laplacian is integrable against every such measure; test functions form a linear space on which gradient and Laplacian act linearly.

Statement

Adopt Probability Measures on Euclidean Space and Random Vectors: Standing Notation and Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation, and fix a dimension qq; a scalar written μ\mu in the latter setting is written tt here, and the letter μ\mu is reserved for a probability measure on Rq\mathbb{R}^{q}. Let ψCc(Rq)\psi\in C_{c}^{\infty}(\mathbb{R}^{q}) be a test function, with gradient map ψ\nabla\psi, whose components are the partial derivatives iψ\partial_{i}\psi, i[q]i\in[q], and Laplacian Δψ\Delta\psi. Continuity is that of Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §extrema, compact support that of Test Functions on Euclidean Space, Their Gradient Maps and Laplacians §space, and for μP(Rq)\mu\in\mathcal{P}(\mathbb{R}^{q}) integrable with respect to μ\mu is integrable on the measure space (Rq,B(Rq),μ)(\mathbb{R}^{q},\mathcal{B}(\mathbb{R}^{q}),\mu). Sums and scalar multiples of points of Rq\mathbb{R}^{q} are those of Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §background.

1. (Gradient) For every i[q]i\in[q] the function iψ\partial_{i}\psi is continuous, compactly supported and bounded. The map ψ\nabla\psi is Borel, and there is a real number K0K\ge0 with ψ(x)K\lVert\nabla\psi(x)\rVert\le K for every xRqx\in\mathbb{R}^{q}. Consequently the function xψ(x)2x\mapsto\lVert\nabla\psi(x)\rVert^{2} is Borel and bounded, and for every μP(Rq)\mu\in\mathcal{P}(\mathbb{R}^{q}) it is integrable with respect to μ\mu, with

Rqψ2dμK2.\int_{\mathbb{R}^{q}}\lVert\nabla\psi\rVert^{2}\,d\mu\le K^{2}.

2. (Laplacian) The function Δψ\Delta\psi is continuous, compactly supported, bounded and Borel; hence it is integrable with respect to every μP(Rq)\mu\in\mathcal{P}(\mathbb{R}^{q}).

3. (Linearity) The set Cc(Rq)C_{c}^{\infty}(\mathbb{R}^{q}) is a linear subspace of the vector space of real-valued maps on Rq\mathbb{R}^{q}, and for all ψ,ϕCc(Rq)\psi,\phi\in C_{c}^{\infty}(\mathbb{R}^{q}), a,bRa,b\in\mathbb{R} and xRqx\in\mathbb{R}^{q},

(aψ+bϕ)(x)=aψ(x)+bϕ(x),Δ(aψ+bϕ)(x)=aΔψ(x)+bΔϕ(x).\nabla(a\psi+b\phi)(x)=a\,\nabla\psi(x)+b\,\nabla\phi(x),\qquad \Delta(a\psi+b\phi)(x)=a\,\Delta\psi(x)+b\,\Delta\phi(x).
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