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Proof of Test Functions Approximate Bounded Continuous Functions Pointwise, Determine a Finite Borel Measure, and Detect a Vanishing Density

lemmalem:test-functions-determine-measure-euclidean-2026a
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· 9,474 chars · 35 deps · depth 26 Reason: Phase B2b: proof by cutting off and mollifying a bounded continuous function, then dominated convergence, and comparison of the positive and negative parts of the density as two finite measures.

A bounded continuous function is cut off by a smooth bump and then mollified, which gives test functions bounded by the same constant and converging pointwise; dominated convergence then transfers equality of test-function integrals to bounded Lipschitz functions, and the positive and negative parts of a density are compared as two finite measures.

Proof

Throughout, each result cited is universally quantified over the data appearing in its own statement and is applied to the data named here. Let ι\iota denote the canonical map from N\mathbb{N} to R\mathbb{R}, positive with positive inverse by claim 3 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field; this is the only use of the symbol ι\iota here. Closed balls Bˉ(x,r)\bar{B}(x,r) and the Lebesgue measure λd\lambda_{d} are those of Euclidean Space and Lebesgue Measure: Standing Notation §space and Euclidean Space and Lebesgue Measure: Standing Notation §measure.

Step 1 (Claim 1). Let ff and MM be as in claim 1; we may assume 0M0\le M, since f(x)M|f(x)|\le M forces it by claim 1 of Properties of the Absolute Value in an Ordered Field. Fix a mollifier kernel ρ\rho of radius 11 on Rd\mathbb{R}^{d}, which exists by Existence of Mollifier Kernels of Every Radius, and for a positive real ε\varepsilon let ρε(y)=(ε1)dρ(ε1y)\rho_{\varepsilon}(y)=(\varepsilon^{-1})^{d}\rho(\varepsilon^{-1}y), a mollifier kernel of radius ε\varepsilon by Rescaling a Mollifier Kernel.

Let nNn\in\mathbb{N}. By Existence of Smooth Bump Functions on Euclidean Space, applied with x0=0Rdx_{0}=0_{\mathbb{R}^{d}}, r=ι(n)r=\iota(n) and s=ι(n)+1s=\iota(n)+1, there is a smooth map χn:RdR\chi_{n}:\mathbb{R}^{d}\to\mathbb{R} with 0χn10\le\chi_{n}\le1, with χn(x)=1\chi_{n}(x)=1 whenever xι(n)\lVert x\rVert\le\iota(n), and with χn(x)=0\chi_{n}(x)=0 whenever ι(n)+1x\iota(n)+1\le\lVert x\rVert. The product fχnf\chi_{n} is continuous on Rd\mathbb{R}^{d} by claim 3 of Continuity of Sums and Products of Real-Valued Functions on a Metric Space, χn\chi_{n} being continuous by claim 3 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous, and it vanishes outside Bˉ(0Rd,ι(n)+1)\bar{B}(0_{\mathbb{R}^{d}},\iota(n)+1).

Since fχnf\chi_{n} is continuous on the open set Rd\mathbb{R}^{d} and ρε\rho_{\varepsilon} is continuous and vanishes at every yy with ε<y\varepsilon<\lVert y\rVert, the convolution (fχn)ρε(f\chi_{n})*\rho_{\varepsilon} is defined on {x:Bˉ(x,ε)Rd}=Rd\{x:\bar{B}(x,\varepsilon)\subseteq\mathbb{R}^{d}\}=\mathbb{R}^{d}, and it is smooth by Convolution with a CkC^k Kernel is of Class CkC^k. It is bounded by MM: with hx(y)=(fχn)(xy)ρε(y)h_{x}(y)=(f\chi_{n})(x-y)\rho_{\varepsilon}(y) one has hxMρε|h_{x}|\le M\rho_{\varepsilon} pointwise, because fχnM|f\chi_{n}|\le M and ρε0\rho_{\varepsilon}\ge0, so claims 1 and 2 of Linearity and Monotonicity of the Lebesgue Integral and the unit mass of ρε\rho_{\varepsilon} give

((fχn)ρε)(x)MRdρεdλd=M.\bigl|\bigl((f\chi_{n})*\rho_{\varepsilon}\bigr)(x)\bigr|\le M\int_{\mathbb{R}^{d}}\rho_{\varepsilon}\,d\lambda_{d}=M .

It also vanishes at every xx with ι(n)+1+ε<x\iota(n)+1+\varepsilon<\lVert x\rVert: for such xx and any yy with ρε(y)0\rho_{\varepsilon}(y)\ne0 one has yε\lVert y\rVert\le\varepsilon, hence xyxy>ι(n)+1\lVert x-y\rVert\ge\lVert x\rVert-\lVert y\rVert>\iota(n)+1 by claim 6 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, so hxh_{x} vanishes identically. Its support is therefore a closed subset of Bˉ(0Rd,ι(n)+1+ε)\bar{B}(0_{\mathbb{R}^{d}},\iota(n)+1+\varepsilon), which is compact by Heine-Borel Theorem in Rn\mathbb{R}^n, hence compact by Closed Subset of a Compact Space is Compact; so (fχn)ρε(f\chi_{n})*\rho_{\varepsilon} is a test function.

The set Bˉ(0Rd,ι(n))\bar{B}(0_{\mathbb{R}^{d}},\iota(n)) is compact by Heine-Borel Theorem in Rn\mathbb{R}^n, so claim 2 of Mollification Converges Uniformly on Compact Subsets, applied to fχnf\chi_{n} on Ω=Rd\Omega=\mathbb{R}^{d} with the kernel ρ\rho and the positive real number ι(n)1\iota(n)^{-1}, provides a positive real εn\varepsilon_{n} with

((fχn)ρεn)(x)(fχn)(x)<ι(n)1for every xBˉ(0Rd,ι(n)).\bigl|\bigl((f\chi_{n})*\rho_{\varepsilon_{n}}\bigr)(x)-(f\chi_{n})(x)\bigr|<\iota(n)^{-1}\qquad\text{for every }x\in\bar{B}(0_{\mathbb{R}^{d}},\iota(n)).

Put ψn=(fχn)ρεn\psi_{n}=(f\chi_{n})*\rho_{\varepsilon_{n}}. Then ψnCc(Rd)\psi_{n}\in C_{c}^{\infty}(\mathbb{R}^{d}) and ψn(x)M|\psi_{n}(x)|\le M for every xx, by the previous paragraph. If xι(n)\lVert x\rVert\le\iota(n) then χn(x)=1\chi_{n}(x)=1, so (fχn)(x)=f(x)(f\chi_{n})(x)=f(x) and ψn(x)f(x)<ι(n)1|\psi_{n}(x)-f(x)|<\iota(n)^{-1}.

Finally, let xRdx\in\mathbb{R}^{d}. By claim 1 of The Archimedean Property of the Real Numbers there is n0Nn_{0}\in\mathbb{N} with x<ι(n0)\lVert x\rVert<\iota(n_{0}), and by claim 6 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field every nn0n\ge n_{0} satisfies x<ι(n)\lVert x\rVert<\iota(n) and hence ψn(x)f(x)<ι(n)1|\psi_{n}(x)-f(x)|<\iota(n)^{-1}. Since (ι(n)1)nN(\iota(n)^{-1})_{n\in\mathbb{N}} converges to 00 by claim 3 of The Archimedean Property of the Real Numbers, the sequence (ψn(x))nN(\psi_{n}(x))_{n\in\mathbb{N}} converges to f(x)f(x). This proves claim 1.

Step 2 (Claim 2). Let μ,ν\mu,\nu be as in claim 2 and let f:RdRf:\mathbb{R}^{d}\to\mathbb{R} be continuous and bounded, say fM|f|\le M with 0M0\le M. Take (ψn)nN(\psi_{n})_{n\in\mathbb{N}} as in claim 1. The constant function with value MM is integrable with respect to μ\mu and with respect to ν\nu by claim 6 of Borel Measurability and Bounded Integration on a Metric Space, both measures being finite, and ψnM|\psi_{n}|\le M for every nn while (ψn(x))n(\psi_{n}(x))_{n} converges to f(x)f(x) for every xx. Claim 7 of The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere, applied on the measure space (Rd,B(Rd),μ)(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}),\mu) and then on (Rd,B(Rd),ν)(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}),\nu), gives that (ψndμ)n\bigl(\int\psi_{n}\,d\mu\bigr)_{n} converges to fdμ\int f\,d\mu and (ψndν)n\bigl(\int\psi_{n}\,d\nu\bigr)_{n} converges to fdν\int f\,d\nu. The two sequences are equal term by term by hypothesis, so their limits agree by Uniqueness of Limits in a Metric Space:

Rdfdμ=Rdfdν.\int_{\mathbb{R}^{d}}f\,d\mu=\int_{\mathbb{R}^{d}}f\,d\nu .

Every bounded Lipschitz f:RdRf:\mathbb{R}^{d}\to\mathbb{R} is continuous by A Lipschitz Map is Uniformly Continuous, so the displayed identity holds for all such ff, and claim 1 of Lipschitz Test Functions Determine a Finite Borel Measure, and Uniqueness of Weak Limits, applied to the metric space (Rd,dE)(\mathbb{R}^{d},d_{E}), gives μ(B)=ν(B)\mu(B)=\nu(B) for every BB(Rd)B\in\mathcal{B}(\mathbb{R}^{d}).

Step 3 (Claim 3). Let gg be as in claim 3 and put g+=max(g,0)g^{+}=\max(g,0) and g=max(g,0)g^{-}=\max(-g,0), Borel by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions and nonnegative by claim 1 of Elementary Properties of the Maximum of Two Elements. At each point xx the identities g(x)=g+(x)g(x)g(x)=g^{+}(x)-g^{-}(x) and g+(x)+g(x)=g(x)g^{+}(x)+g^{-}(x)=|g(x)| hold, by a case distinction on the sign of g(x)g(x): if 0g(x)0\le g(x) then g+(x)=g(x)g^{+}(x)=g(x) and g(x)=0g^{-}(x)=0, while if g(x)<0g(x)<0 then g+(x)=0g^{+}(x)=0 and g(x)=g(x)g^{-}(x)=-g(x), in each case by claim 2 of Elementary Properties of the Maximum of Two Elements together with claim 1 of Properties of the Absolute Value in an Ordered Field. Both are integrable with respect to μ\mu, being nonnegative and dominated by the integrable g|g|, by claim 1 of Linearity and Monotonicity of the Lebesgue Integral.

By claim 3 of Image Measures, Measures with Densities, and Change of Variables, applied on (Rd,B(Rd),μ)(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}),\mu) with the densities g+g^{+} and gg^{-}, the set functions

μ+(A)=Rd1Ag+dμ,μ(A)=Rd1Agdμ(AB(Rd))\mu^{+}(A)=\int_{\mathbb{R}^{d}}\mathbf{1}_{A}\,g^{+}\,d\mu,\qquad \mu^{-}(A)=\int_{\mathbb{R}^{d}}\mathbf{1}_{A}\,g^{-}\,d\mu\qquad(A\in\mathcal{B}(\mathbb{R}^{d}))

are measures on (Rd,B(Rd))(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d})), hence Borel measures on (Rd,dE)(\mathbb{R}^{d},d_{E}), and for every AA-integrable datum the change-of-density formula of that clause holds. They are finite, since μ±(Rd)=g±dμ\mu^{\pm}(\mathbb{R}^{d})=\int g^{\pm}\,d\mu is a real number. Let ψCc(Rd)\psi\in C_{c}^{\infty}(\mathbb{R}^{d}). It is bounded, being continuous with compact support by A Continuous Compactly Supported Function on Rn\mathbb{R}^n is Bounded and Integrable, hence integrable with respect to μ+\mu^{+} and μ\mu^{-} by claim 6 of Borel Measurability and Bounded Integration on a Metric Space, and claim 3 of Image Measures, Measures with Densities, and Change of Variables gives ψdμ±=ψg±dμ\int\psi\,d\mu^{\pm}=\int\psi\,g^{\pm}\,d\mu. Therefore, by claim 2 of Linearity and Monotonicity of the Lebesgue Integral and the hypothesis,

Rdψdμ+Rdψdμ=Rdψ(g+g)dμ=Rdgψdμ=0.\int_{\mathbb{R}^{d}}\psi\,d\mu^{+}-\int_{\mathbb{R}^{d}}\psi\,d\mu^{-}=\int_{\mathbb{R}^{d}}\psi\,(g^{+}-g^{-})\,d\mu=\int_{\mathbb{R}^{d}}g\,\psi\,d\mu=0 .

So μ+\mu^{+} and μ\mu^{-} integrate every test function alike, and claim 2 gives μ+=μ\mu^{+}=\mu^{-}.

Let P={xRd:0<g(x)}P=\{x\in\mathbb{R}^{d}:0<g(x)\}, a member of B(Rd)\mathcal{B}(\mathbb{R}^{d}) as the preimage of a ray under the Borel map gg. On PP one has g=0g^{-}=0 and off PP one has g+=0g^{+}=0, by claim 1 of Elementary Properties of the Maximum of Two Elements. Hence 1Pg\mathbf{1}_{P}g^{-} vanishes identically, so μ(P)=0\mu^{-}(P)=0 by claim 1 of Linearity and Monotonicity of the Lebesgue Integral, while 1Pg+=g+\mathbf{1}_{P}g^{+}=g^{+} everywhere, so μ+(P)=g+dμ\mu^{+}(P)=\int g^{+}\,d\mu. From μ+(P)=μ(P)\mu^{+}(P)=\mu^{-}(P) we get Rdg+dμ=0\int_{\mathbb{R}^{d}}g^{+}\,d\mu=0, and claim 4 of The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere gives μ({x:g+(x)0})=0\mu(\{x:g^{+}(x)\ne0\})=0. The same argument applied to Q={x:g(x)<0}Q=\{x:g(x)<0\}, on which g+=0g^{+}=0 and off which g=0g^{-}=0, gives μ({x:g(x)0})=0\mu(\{x:g^{-}(x)\ne0\})=0.

Finally {x:g(x)0}={x:g+(x)0}{x:g(x)0}\{x:g(x)\ne0\}=\{x:g^{+}(x)\ne0\}\cup\{x:g^{-}(x)\ne0\}, since g=g+gg=g^{+}-g^{-} and at each point at least one of g+,gg^{+},g^{-} vanishes; it belongs to B(Rd)\mathcal{B}(\mathbb{R}^{d}), being the preimage of R{0}\mathbb{R}\setminus\{0\} under gg, and it is μ\mu-null by claim 1 of The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere. This proves claim 3.

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