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Proof of Gaussian Smoothing of a Probability Measure on Euclidean Space: Regularity, Mass, Duality, Approximation of a Bounded Function with a Modulus of Continuity, and the Pairing Identity

lemmalem:gaussian-smoothing-measure-euclidean-2026a
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· 9,519 chars · 17 deps · depth 21 Reason: First publication of the proof of the Gaussian smoothing lemma (Goal 3F, batch F0).

Differentiation under the integral sign with the uniform derivative bounds of the Gaussian kernel gives the C3C^3 regularity; Tonelli and Fubini on the product of Lebesgue measure with the probability measure give the mass and duality identities; the approximation bound splits the integral at distance r and uses the Gaussian tail; the pairing identity is Tonelli on the product measure together with the convolution identity gsg_s * gsg_s = g2sg_{2s}.

Proof

Each result cited is universally quantified over the data in its own statement. Borel is as in the preamble of Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets; a continuous function on a Euclidean space is Borel (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps), a composition of Borel maps is Borel (claim 4 of Borel Measurability and Bounded Integration on a Metric Space), and for yRqy\in\mathbb{R}^{q} the map xyxx\mapsto y-x is continuous, since dE(yx,yx)=xx=dE(x,x)d_{E}(y-x,y-x')=\lVert x'-x\rVert=d_{E}(x,x') by claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n. Throughout, λq\lambda_{q} is σ\sigma-finite by claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l and μ\mu, ν\nu are finite, so Tonelli and Fubini Theorems applies to the product measures λqμ\lambda_{q}\otimes\mu, λqλq\lambda_{q}\otimes\lambda_{q}, μν\mu\otimes\nu and λq(μν)\lambda_{q}\otimes(\mu\boxtimes\nu) (Existence and Uniqueness of the Product Measure). A function of the first variable alone, (y,x)ϕ(y)(y,x)\mapsto\phi(y) with ϕ\phi Borel, is measurable for the product σ\sigma-algebra, the first coordinate projection being measurable by Product Sigma-Algebra. For measurability with respect to a product σ\sigma-algebra B(Ra)B(Rb)\mathcal{B}(\mathbb{R}^{a})\otimes\mathcal{B}(\mathbb{R}^{b}) we use Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §product: for a Borel F:Ra+b[0,]F:\mathbb{R}^{a+b}\to[0,\infty] the function Fιa,bF\circ\iota^{a,b} on Ra×Rb\mathbb{R}^{a}\times\mathbb{R}^{b} is measurable with respect to B(Ra)B(Rb)\mathcal{B}(\mathbb{R}^{a})\otimes\mathcal{B}(\mathbb{R}^{b}), and a real-valued Borel FF is handled through its positive and negative parts (claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions). The map Rq+qRq\mathbb{R}^{q+q}\to\mathbb{R}^{q}, zpr1(z)pr2(z)z\mapsto\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z), is Borel, its components being differences of the Borel components of the projections (Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §projections, claim 2 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps); hence for every Borel G:RqRG:\mathbb{R}^{q}\to\mathbb{R} the function zG(pr1(z)pr2(z))z\mapsto G(\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z)) is Borel on Rq+q\mathbb{R}^{q+q}, and (y,x)G(yx)(y,x)\mapsto G(y-x), which is this function composed with ιq,q\iota^{q,q}, is measurable with respect to B(Rq)B(Rq)\mathcal{B}(\mathbb{R}^{q})\otimes\mathcal{B}(\mathbb{R}^{q}).

Claim 1. For a continuous bounded G:RqRG:\mathbb{R}^{q}\to\mathbb{R} we write GμG*\mu for the function yG(yx)μ(dx)y\mapsto\int G(y-x)\,\mu(dx) of The Convolution of a Bounded Continuous Function with a Probability Measure on Euclidean Space: Continuity, Boundedness and Differentiation Under the Integral §continuous, so that gsμg_{s}*\mu is the function of the statement. By The Gaussian Kernels on Euclidean Space: Scaling, Derivatives up to Order Three, the Convolution Identity, Moments and Tails §derivatives and The Gaussian Kernels on Euclidean Space: Scaling, Derivatives up to Order Three, the Convolution Identity, Moments and Tails §bounds, each of gsg_{s}, igs\partial_{i}g_{s} and jigs\partial_{j}\partial_{i}g_{s} is smooth, in particular of class C1C^{1}, and is bounded together with its partial derivatives by the constant C=max{A0,A1,A2,A3}s(q+3)/2C=\max\{A_{0},A_{1},A_{2},A_{3}\}\,s^{-(q+3)/2} (as s1s\le1, sm/2s(q+3)/2s^{-m/2}\le s^{-(q+3)/2} for mq+3m\le q+3, by claim 2 of Real Powers Through the Exponential, and Elementary Asymptotic Tools: Monotonicity, Null Sequences of Negative Powers, Exponential Domination, Integer Rounding, and Square-Root and Exponential Inequalities applied to the base 1/s11/\sqrt{s}\ge1 and the exponents mq+3m\le q+3). The Convolution of a Bounded Continuous Function with a Probability Measure on Euclidean Space: Continuity, Boundedness and Differentiation Under the Integral §derivative applied to G=gsG=g_{s} shows that gsμg_{s}*\mu is of class C1C^{1} with i(gsμ)=(igs)μ\partial_{i}(g_{s}*\mu)=(\partial_{i}g_{s})*\mu; applied to G=igsG=\partial_{i}g_{s} it shows that (igs)μ(\partial_{i}g_{s})*\mu is of class C1C^{1} with ji(gsμ)=(jigs)μ\partial_{j}\partial_{i}(g_{s}*\mu)=(\partial_{j}\partial_{i}g_{s})*\mu; and applied to G=jigsG=\partial_{j}\partial_{i}g_{s} it shows that this is of class C1C^{1} with kji(gsμ)=(kjigs)μ\partial_{k}\partial_{j}\partial_{i}(g_{s}*\mu)=(\partial_{k}\partial_{j}\partial_{i}g_{s})*\mu, continuous. By clause 2 of C^k Maps on a Euclidean Open Set, applied twice, gsμg_{s}*\mu is of class C3C^{3}. The displayed formulas are the identities just obtained, and the integrands are bounded Borel functions of xx by The Convolution of a Bounded Continuous Function with a Probability Measure on Euclidean Space: Continuity, Boundedness and Differentiation Under the Integral §continuous. The bounds follow from claim 6(b) of Borel Measurability and Bounded Integration on a Metric Space and the pointwise bounds of The Gaussian Kernels on Euclidean Space: Scaling, Derivatives up to Order Three, the Convolution Identity, Moments and Tails §bounds; and gsμ0g_{s}*\mu\ge0 because its integrand is nonnegative (claim 2 of Linearity and Monotonicity of the Lebesgue Integral, monotonicity applied against the zero function).

Claim 2. The function (y,x)gs(yx)(y,x)\mapsto g_{s}(y-x) is nonnegative and B(Rq)B(Rq)\mathcal{B}(\mathbb{R}^{q})\otimes\mathcal{B}(\mathbb{R}^{q})-measurable (preamble). By Tonelli and Fubini Theorems (Tonelli) the function ygs(yx)μ(dx)=(gsμ)(y)y\mapsto\int g_{s}(y-x)\,\mu(dx)=(g_{s}*\mu)(y) is Borel and

Rqgsμdλq=Rq(Rqgs(yx)dy)μ(dx)=Rq1μ(dx)=1,\int_{\mathbb{R}^{q}}g_{s}*\mu\,d\lambda_{q}=\int_{\mathbb{R}^{q}}\Bigl(\int_{\mathbb{R}^{q}}g_{s}(y-x)\,dy\Bigr)\mu(dx)=\int_{\mathbb{R}^{q}}1\,\mu(dx)=1,

using gs(yx)dy=1\int g_{s}(y-x)\,dy=1 for every xx (claim 1 of The Gaussian Smoothing Weight: Normalization, Derivatives, Exponential Tilting, Moments, and First-Order Remainder, with the evenness gs(yx)=gs(xy)g_{s}(y-x)=g_{s}(x-y)) and claim 6(a) of Borel Measurability and Bounded Integration on a Metric Space. Being nonnegative, Borel and of finite integral, gsμg_{s}*\mu is integrable. Now let ϕ\phi be bounded Borel with ϕM|\phi|\le M. The function (y,x)ϕ(y)gs(yx)(y,x)\mapsto\phi(y)g_{s}(y-x) is measurable for the product σ\sigma-algebra (product of two such functions, claim 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions), and ϕ(y)gs(yx)μ(dx)dyMgsμdλq=M<\int\int|\phi(y)|g_{s}(y-x)\,\mu(dx)\,dy\le M\int g_{s}*\mu\,d\lambda_{q}=M<\infty by claim 1 of Linearity and Monotonicity of the Lebesgue Integral; so by Tonelli it is integrable with respect to λqμ\lambda_{q}\otimes\mu, and by Fubini (Tonelli and Fubini Theorems) its two iterated integrals coincide:

Rqϕ(y)(gsμ)(y)dy=Rq(Rqϕ(y)gs(yx)dy)μ(dx)=Rq(gsϕ)(x)μ(dx),\int_{\mathbb{R}^{q}}\phi(y)\,(g_{s}*\mu)(y)\,dy=\int_{\mathbb{R}^{q}}\Bigl(\int_{\mathbb{R}^{q}}\phi(y)\,g_{s}(y-x)\,dy\Bigr)\mu(dx)=\int_{\mathbb{R}^{q}}(g_{s}*\phi)(x)\,\mu(dx),

the inner integral being (gsϕ)(x)(g_{s}*\phi)(x) by the evenness of gsg_{s}. Here ϕ(gsμ)\phi\cdot(g_{s}*\mu) is integrable, being Borel and dominated by MgsμM\,g_{s}*\mu; gsϕg_{s}*\phi is Borel, being the difference of the Tonelli section integrals of ϕ+gs\phi^{+}g_{s} and ϕgs\phi^{-}g_{s}; and (gsϕ)(x)gs(xy)ϕ(y)dyM|(g_{s}*\phi)(x)|\le\int g_{s}(x-y)|\phi(y)|\,dy\le M by claim 2 of Linearity and Monotonicity of the Lebesgue Integral and gs(xy)dy=1\int g_{s}(x-y)\,dy=1.

Claim 3. Fix xx. Since gs(xy)dy=1\int g_{s}(x-y)\,dy=1, claim 2 of Linearity and Monotonicity of the Lebesgue Integral gives

(gsϕ)(x)ϕ(x)=Rqgs(xy)(ϕ(y)ϕ(x))dyRqgs(xy)ϕ(y)ϕ(x)dy.\bigl|(g_{s}*\phi)(x)-\phi(x)\bigr|=\Bigl|\int_{\mathbb{R}^{q}}g_{s}(x-y)\bigl(\phi(y)-\phi(x)\bigr)\,dy\Bigr|\le\int_{\mathbb{R}^{q}}g_{s}(x-y)\,|\phi(y)-\phi(x)|\,dy .

For yy with xyr\lVert x-y\rVert\le r the integrand is at most ϵgs(xy)\epsilon\,g_{s}(x-y); for yy with xy>r\lVert x-y\rVert>r it is at most 2Mgs(xy)2M\,g_{s}(x-y) (claim 5 of Properties of the Absolute Value in an Ordered Field). Hence, by monotonicity and additivity (claim 1 of Linearity and Monotonicity of the Lebesgue Integral), with Ar={z:r<z}A_{r}=\{z:r<\lVert z\rVert\} and 1Ar(xy)\mathbf{1}_{A_{r}}(x-y) the indicator of the second set of yy's,

gs(xy)ϕ(y)ϕ(x)dyϵgs(xy)dy+2M1Ar(xy)gs(xy)dy=ϵ+2M1Ar(z)gs(z)dzϵ+2Mqsr2,\int g_{s}(x-y)\,|\phi(y)-\phi(x)|\,dy\le\epsilon\int g_{s}(x-y)\,dy+2M\int\mathbf{1}_{A_{r}}(x-y)\,g_{s}(x-y)\,dy=\epsilon+2M\int\mathbf{1}_{A_{r}}(z)\,g_{s}(z)\,dz\le\epsilon+\frac{2Mqs}{r^{2}},

where the substitution z=xyz=x-y is the reflection and translation invariance of Translation and Reflection Invariance of Lebesgue Measure on Rn\mathbb{R}^n, and the last inequality is The Gaussian Kernels on Euclidean Space: Scaling, Derivatives up to Order Three, the Convolution Identity, Moments and Tails §moments.

Claim 4. Let 0<s120<s\le\tfrac12 and νP(Rq)\nu\in\mathcal{P}(\mathbb{R}^{q}). The function (y,z)gs(ypr1(z))gs(ypr2(z))(y,z)\mapsto g_{s}(y-\mathrm{pr}_{1}(z))\,g_{s}(y-\mathrm{pr}_{2}(z)) on Rq×Rq+q\mathbb{R}^{q}\times\mathbb{R}^{q+q} is nonnegative and measurable for B(Rq)B(Rq+q)\mathcal{B}(\mathbb{R}^{q})\otimes\mathcal{B}(\mathbb{R}^{q+q}): it is the composition with ιq,q+q\iota^{q,q+q} of a function on Rq+(q+q)\mathbb{R}^{q+(q+q)} that is a product of two functions of the form G(Borel map)G\circ(\text{Borel map}) with G=gsG=g_{s} (the maps wpr1q,q+q(w)pr1(pr2q,q+q(w))w\mapsto\mathrm{pr}^{q,q+q}_{1}(w)-\mathrm{pr}_{1}(\mathrm{pr}^{q,q+q}_{2}(w)) and wpr1q,q+q(w)pr2(pr2q,q+q(w))w\mapsto\mathrm{pr}^{q,q+q}_{1}(w)-\mathrm{pr}_{2}(\mathrm{pr}^{q,q+q}_{2}(w)) are Borel, as compositions and differences of Borel maps). For fixed yy, by Tonelli on μν\mu\otimes\nu and the image-measure identity of Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §product,

Rq+qgs(ypr1(z))gs(ypr2(z))(μν)(dz)=(gs(yx)gs(yx)ν(dx))μ(dx)=(gsμ)(y)(gsν)(y),\int_{\mathbb{R}^{q+q}}g_{s}(y-\mathrm{pr}_{1}(z))\,g_{s}(y-\mathrm{pr}_{2}(z))\,(\mu\boxtimes\nu)(dz)=\int\Bigl(\int g_{s}(y-x)\,g_{s}(y-x')\,\nu(dx')\Bigr)\mu(dx)=(g_{s}*\mu)(y)\,(g_{s}*\nu)(y),

the inner integral being gs(yx)(gsν)(y)g_{s}(y-x)\,(g_{s}*\nu)(y) by claim 1 of Linearity and Monotonicity of the Lebesgue Integral, and the outer one then (gsν)(y)(gsμ)(y)(g_{s}*\nu)(y)\,(g_{s}*\mu)(y). For fixed zz, with x=pr1(z)x=\mathrm{pr}_{1}(z) and x=pr2(z)x'=\mathrm{pr}_{2}(z), gs(yx)gs(yx)dy=g2s(xx)\int g_{s}(y-x)g_{s}(y-x')\,dy=g_{2s}(x-x') by The Gaussian Kernels on Euclidean Space: Scaling, Derivatives up to Order Three, the Convolution Identity, Moments and Tails §convolution. Tonelli on λq(μν)\lambda_{q}\otimes(\mu\boxtimes\nu), applied through the image measure as before (or directly, μν\mu\boxtimes\nu being a probability measure on Rq+q\mathbb{R}^{q+q}), therefore gives

Rq(gsμ)(gsν)dλq=Rq+qg2s(pr1(z)pr2(z))(μν)(dz),\int_{\mathbb{R}^{q}}(g_{s}*\mu)(g_{s}*\nu)\,d\lambda_{q}=\int_{\mathbb{R}^{q+q}}g_{2s}\bigl(\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z)\bigr)\,(\mu\boxtimes\nu)(dz),

and the right side is at most A0(2s)q/2A_{0}(2s)^{-q/2} (The Gaussian Kernels on Euclidean Space: Scaling, Derivatives up to Order Three, the Convolution Identity, Moments and Tails §bounds, 2s12s\le1, claim 6(b) of Borel Measurability and Bounded Integration on a Metric Space), so the nonnegative Borel product (gsμ)(gsν)(g_{s}*\mu)(g_{s}*\nu) (claim 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions) is integrable. That zg2s(pr1(z)pr2(z))z\mapsto g_{2s}(\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z)) is Borel and bounded by A0(2s)q/2A_{0}(2s)^{-q/2} was noted in the preamble and in The Gaussian Kernels on Euclidean Space: Scaling, Derivatives up to Order Three, the Convolution Identity, Moments and Tails §bounds.

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