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

lemmalem:test-function-gradient-integrable-2026a
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Each partial derivative of a compactly supported C1C^1 function is continuous and compactly supported by the Euclidean integration-by-parts lemma, hence bounded and Borel; applying this twice handles the Laplacian, whose continuity follows by induction over the finite sum. Bounded Borel functions are integrable against probability measures. Linearity is the sum and scalar-multiple rules for partial derivatives.

Proof

Each result cited is universally quantified over the data in its own statement. The topology of Test Functions on Euclidean Space, Their Gradient Maps and Laplacians §space is the topology of the open subsets of Rq\mathbb{R}^{q}, which is also the topology of Euclidean Space and Lebesgue Measure: Standing Notation §space used in Integration by Parts on Euclidean Space Against a Compactly Supported Function of Class C1C^{1} and the metric topology of (Rq,dE)(\mathbb{R}^{q},d_{E}) (Euclidean Openness Agrees with Metric Openness on Rn\mathbb{R}^n); compact support is the same notion for all three. By The Euclidean Distance on the Real Line is the Absolute Value Metric the Euclidean distance on R\mathbb{R} is dRd_{\mathbb{R}}, so continuity in the sense of Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §extrema is the continuity hypothesis of A Continuous Compactly Supported Function on Rn\mathbb{R}^n is Bounded and Integrable. A smooth function is of class C1C^{1} and of class C2C^{2} (Test Functions on Euclidean Space, Their Gradient Maps and Laplacians §gradient), and the partial derivatives of a smooth function are smooth by claim 3 of Coordinate Functions, the CkC^k Hierarchy, and Partial Derivatives of a Smooth Map. A continuous function RqR\mathbb{R}^{q}\to\mathbb{R} is Borel by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps. Finite sums of real numbers are those of Finite Sum Notation in a Field, with Properties of Finite Sums and Comparison and Absolute Value Bounds for Finite Sums of Real Numbers in force.

Step 1: claim 1. Fix i[q]i\in[q]. The function ψ\psi is of class C1C^{1} on Rq\mathbb{R}^{q} and compactly supported, so by Integration by Parts on Euclidean Space Against a Compactly Supported Function of Class C1C^{1} §vanishing (applied with h=ψh=\psi) the function iψ\partial_{i}\psi is continuous on Rq\mathbb{R}^{q} and compactly supported; by claim 1 of A Continuous Compactly Supported Function on Rn\mathbb{R}^n is Bounded and Integrable it is bounded, and we choose a bound Ki0K_{i}\ge0 with iψ(x)Ki|\partial_{i}\psi(x)|\le K_{i} for every xx. Being continuous, iψ\partial_{i}\psi is Borel, so ψ\nabla\psi, whose components are the iψ\partial_{i}\psi, is Borel by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps. Put K=i=1qKi2K=\sqrt{\sum_{i=1}^{q}K_{i}^{2}}, the nonnegative square root (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §spaces) of a sum of nonnegative terms (claim 2 of Nonnegativity of Squares in an Ordered Field and claim 5 of Properties of Finite Sums). For every xx, claim 1 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n gives ψ(x)2=i=1qiψ(x)2\lVert\nabla\psi(x)\rVert^{2}=\sum_{i=1}^{q}\partial_{i}\psi(x)^{2}; each term satisfies iψ(x)2=iψ(x)2Ki2\partial_{i}\psi(x)^{2}=|\partial_{i}\psi(x)|^{2}\le K_{i}^{2} by claim 1 of Nonnegativity of Squares in an Ordered Field and claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field, so ψ(x)2i=1qKi2=K2\lVert\nabla\psi(x)\rVert^{2}\le\sum_{i=1}^{q}K_{i}^{2}=K^{2} by claim 1 of Comparison and Absolute Value Bounds for Finite Sums of Real Numbers, and hence ψ(x)K\lVert\nabla\psi(x)\rVert\le K by claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field, both numbers being nonnegative. The function xψ(x)2x\mapsto\lVert\nabla\psi(x)\rVert^{2} is the composition of the Borel map ψ\nabla\psi with the Borel map yy2y\mapsto\lVert y\rVert^{2} of Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pairs, hence Borel by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps; it is bounded by K2K^{2}, so for every μP(Rq)\mu\in\mathcal{P}(\mathbb{R}^{q}) it is integrable with respect to μ\mu by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures, and claim 6(b) of Borel Measurability and Bounded Integration on a Metric Space gives ψ2dμK2μ(Rq)=K2\bigl|\int\lVert\nabla\psi\rVert^{2}\,d\mu\bigr|\le K^{2}\mu(\mathbb{R}^{q})=K^{2}, whence ψ2dμK2\int\lVert\nabla\psi\rVert^{2}\,d\mu\le K^{2} by claim 3 of Properties of the Absolute Value in an Ordered Field.

Step 2: claim 2. For i[q]i\in[q], the function iψ\partial_{i}\psi is smooth, hence of class C1C^{1}, and compactly supported (Step 1), so by Integration by Parts on Euclidean Space Against a Compactly Supported Function of Class C1C^{1} §vanishing (applied with h=iψh=\partial_{i}\psi) the function iiψ\partial_{i}\partial_{i}\psi is continuous and compactly supported, and by claim 1 of A Continuous Compactly Supported Function on Rn\mathbb{R}^n is Bounded and Integrable it is bounded; choose a bound Bi0B_{i}\ge0, and by claim 2 of Compact Support on Rn\mathbb{R}^n Means Vanishing Outside a Bounded Set a real number Ri>0R_{i}>0 with iiψ(x)=0\partial_{i}\partial_{i}\psi(x)=0 whenever x>Ri\lVert x\rVert>R_{i}. For m[q]m\in[q] let sm:RqRs_{m}:\mathbb{R}^{q}\to\mathbb{R} be sm(x)=i=1miiψ(x)s_{m}(x)=\sum_{i=1}^{m}\partial_{i}\partial_{i}\psi(x), so that Δψ=sq\Delta\psi=s_{q} by The Laplacian of a Twice Continuously Differentiable Function §laplacian. We show by induction that sms_{m} is continuous for every m[q]m\in[q]: let TT be the set of mNm\in\mathbb{N} such that either q<mq<m, or m[q]m\in[q] and sms_{m} is continuous on Rq\mathbb{R}^{q}. Then 1T1\in T, since 1[q]1\in[q] (claim 4 of Properties of the Order on the Natural Numbers) and s1=11ψs_{1}=\partial_{1}\partial_{1}\psi by claim 1 of Properties of Finite Sums; and if mTm\in T then m+1Tm+1\in T: by trichotomy (claim 3 of Properties of the Order on the Natural Numbers), either q<mq<m or q=mq=m, in which case q<m+1q<m+1 by claims 5 and 1 there, or m<qm<q, in which case q=m+kq=m+k for some kNk\in\mathbb{N} (claim 7 there), 1k1\le k (claim 4 there) and so m+1m+k=qm+1\le m+k=q (claim 6 there); in the last case q<mq<m fails by claim 3 there and mqm\le q by claim 1 there, so m[q]m\in[q] (Initial Segment of the Natural Numbers), sms_{m} is defined and, since mTm\in T, continuous, and sm+1=sm+m+1m+1ψs_{m+1}=s_{m}+\partial_{m+1}\partial_{m+1}\psi by the recursion in claim 1 of Properties of Finite Sums is continuous by claim 5 of Continuity of Sums and Products of Real-Valued Functions on a Metric Space. By Principle of Induction for the Natural Numbers, T=NT=\mathbb{N}, so Δψ=sq\Delta\psi=s_{q} is continuous, hence Borel. Let R=i=1qRiR=\sum_{i=1}^{q}R_{i}; then 0<R1R0<R_{1}\le R and RiRR_{i}\le R for every ii by claim 6 of Properties of Finite Sums, so for x>R\lVert x\rVert>R every term iiψ(x)\partial_{i}\partial_{i}\psi(x) vanishes and Δψ(x)=i=1q0=0\Delta\psi(x)=\sum_{i=1}^{q}0=0 by claim 3 of Properties of Finite Sums with the scalar 00 and claim 1 of Zero Products and Elementary Identities in a Field; thus Δψ\Delta\psi is compactly supported by claim 2 of Compact Support on Rn\mathbb{R}^n Means Vanishing Outside a Bounded Set. It is bounded, by i=1qBi\sum_{i=1}^{q}B_{i}, by claims 2 and 1 of Comparison and Absolute Value Bounds for Finite Sums of Real Numbers. Finally, a bounded Borel function is integrable with respect to every μP(Rq)\mu\in\mathcal{P}(\mathbb{R}^{q}) by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures.

Step 3: claim 3. The zero map on Rq\mathbb{R}^{q} is smooth by claim 2 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set and vanishes for x>1\lVert x\rVert>1, hence is compactly supported by claim 2 of Compact Support on Rn\mathbb{R}^n Means Vanishing Outside a Bounded Set; so it is a test function. Let ψ,ϕCc(Rq)\psi,\phi\in C_{c}^{\infty}(\mathbb{R}^{q}) and a,bRa,b\in\mathbb{R}. By claim 3 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set, aψ+bϕa\psi+b\phi is smooth; by claim 2 of Compact Support on Rn\mathbb{R}^n Means Vanishing Outside a Bounded Set there are Rψ,Rϕ>0R_{\psi},R_{\phi}>0 with ψ(x)=0\psi(x)=0 for x>Rψ\lVert x\rVert>R_{\psi} and ϕ(x)=0\phi(x)=0 for x>Rϕ\lVert x\rVert>R_{\phi}, so (aψ+bϕ)(x)=0(a\psi+b\phi)(x)=0 for x>Rψ+Rϕ\lVert x\rVert>R_{\psi}+R_{\phi}, and aψ+bϕa\psi+b\phi is compactly supported by the same claim. Hence Cc(Rq)C_{c}^{\infty}(\mathbb{R}^{q}) is closed under pointwise sums and scalar multiples and contains the zero map, and is a linear subspace by The Real Vector Space of Real-Valued Functions on a Set §subspace. For i[q]i\in[q] and every xx, the sum and scalar-multiple rules of claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set give i(aψ+bϕ)(x)=aiψ(x)+biϕ(x)\partial_{i}(a\psi+b\phi)(x)=a\,\partial_{i}\psi(x)+b\,\partial_{i}\phi(x); since sums and scalar multiples of points of Rq\mathbb{R}^{q} are formed coordinatewise (Sum of Points of Rn\mathbb{R}^n, Scalar Multiple of a Point of Rn\mathbb{R}^n), a point is determined by its coordinates (claim 1 of Euclidean Points as Tuples of Real Numbers), and the coordinates of ψ(x)\nabla\psi(x) are the iψ(x)\partial_{i}\psi(x) (Test Functions on Euclidean Space, Their Gradient Maps and Laplacians §gradient), this is (aψ+bϕ)(x)=aψ(x)+bϕ(x)\nabla(a\psi+b\phi)(x)=a\,\nabla\psi(x)+b\,\nabla\phi(x). Applying claim 1 of Constants, Coordinate Functions, Sums and Products of CkC^k Functions on a Euclidean Open Set once more to the identity i(aψ+bϕ)=aiψ+biϕ\partial_{i}(a\psi+b\phi)=a\,\partial_{i}\psi+b\,\partial_{i}\phi of functions gives ii(aψ+bϕ)(x)=aiiψ(x)+biiϕ(x)\partial_{i}\partial_{i}(a\psi+b\phi)(x)=a\,\partial_{i}\partial_{i}\psi(x)+b\,\partial_{i}\partial_{i}\phi(x), and summing over i[q]i\in[q] with claims 2 and 3 of Properties of Finite Sums gives Δ(aψ+bϕ)(x)=aΔψ(x)+bΔϕ(x)\Delta(a\psi+b\phi)(x)=a\,\Delta\psi(x)+b\,\Delta\phi(x).

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