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Test Functions on the Real Line: Unit Mass, Large Mass, Mean-Zero Correction, and the Primitive of a Mean-Zero Test Function

Test functions on the real line are Lebesgue integrable; there are nonnegative ones of unit mass, and ones bounded by one of arbitrarily large mass; subtracting a multiple of a unit-mass one makes any test function have mean zero; and a test function of mean zero is the derivative of a test function.

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 identification of R\mathbb{R} and R1\mathbb{R}^{1} and the notation of claims 1 and 2 of One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative in force; in particular each test function ψ∈Cc∞(R)\psi\in C_{c}^{\infty}(\mathbb{R}) has a derivative ψ′=∇ψ\psi'=\nabla\psi, itself continuous and bounded. Let λ1\lambda_{1} be the Lebesgue measure on B(R)\mathcal{B}(\mathbb{R}).

1. (Test functions are Lebesgue integrable) Every ψ∈Cc∞(R)\psi\in C_{c}^{\infty}(\mathbb{R}) is integrable with respect to λ1\lambda_{1}, and so is ψ′\psi'.

2. (A nonnegative test function of unit mass) There is θ∈Cc∞(R)\theta\in C_{c}^{\infty}(\mathbb{R}) with 0≤θ(x)0\le\theta(x) for every x∈Rx\in\mathbb{R} and ∫Rθ dλ1=1\int_{\mathbb{R}}\theta\,d\lambda_{1}=1.

3. (Test functions of large mass bounded by one) For every positive real number CC there is χ∈Cc∞(R)\chi\in C_{c}^{\infty}(\mathbb{R}) with 0≤χ(x)≤10\le\chi(x)\le1 for every x∈Rx\in\mathbb{R} and C≤∫Rχ dλ1C\le\int_{\mathbb{R}}\chi\,d\lambda_{1}.

4. (Mean-zero correction) Let θ\theta be as in claim 2 and let ψ∈Cc∞(R)\psi\in C_{c}^{\infty}(\mathbb{R}). Then the function φ=ψ−(∫Rψ dλ1)θ\varphi=\psi-\bigl(\int_{\mathbb{R}}\psi\,d\lambda_{1}\bigr)\theta belongs to Cc∞(R)C_{c}^{\infty}(\mathbb{R}) and satisfies ∫Rφ dλ1=0\int_{\mathbb{R}}\varphi\,d\lambda_{1}=0.

5. (Primitive of a mean-zero test function) Let φ∈Cc∞(R)\varphi\in C_{c}^{\infty}(\mathbb{R}) satisfy ∫Rφ dλ1=0\int_{\mathbb{R}}\varphi\,d\lambda_{1}=0. Then there is ψ∈Cc∞(R)\psi\in C_{c}^{\infty}(\mathbb{R}) with ψ′(x)=φ(x)\psi'(x)=\varphi(x) for every x∈Rx\in\mathbb{R}.

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