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Proof of Mollifying a Probability Measure on Euclidean Space: Kernel Bounds, the Translation Estimate, the Mollified Density and Its Cost

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The kernel facts come from the scaling lemma, the test-function gradient bound and a coordinate-by-coordinate mean value argument; the translation estimate splits into far and near translations, the latter using the Lipschitz bound on a ball of radius 2 eps; the density facts come from the convolution lemma and Tonelli's theorem with translation invariance; the cost bound is the composition clause of the Jensen lemma.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied to the data named here. The field axioms and the rules for adding inequalities, for multiplying or dividing them by positive real numbers, for multiplying them by nonnegative real numbers, and for handling absolute values, from Elementary Order Arithmetic in an Ordered Field, Elementary Arithmetic in an Ordered Field and Properties of the Absolute Value in an Ordered Field, are used without further mention; so are the power rules c1=cc^{1}=c, cn+1=cncc^{n+1}=c^{n}c, (cc′)n=cnc′n(cc')^{n}=c^{n}c'^{n} and 1n=11^{n}=1 of claims 1, 3 and 2 of Properties of Natural Number Powers in a Field, and the fact that 0<cn0<c^{n} for real c>0c>0 (claims 5 and 4 there). Points of Rd\mathbb{R}^{d} are dd-tuples of reals by Euclidean Points as Tuples of Real Numbers; sums, negatives and differences of points are formed coordinatewise, and the laws of the real vector space Rd\mathbb{R}^{d} are used without mention. For the Euclidean norm we use ∥x−y∥=dE(x,y)=dE(y,x)\lVert x-y\rVert=d_{E}(x,y)=d_{E}(y,x) (claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n and Euclidean Distance is a Metric on Rn\mathbb{R}^n), the coordinate bound ∣xi∣≤∥x∥|x_{i}|\le\lVert x\rVert (claim 4 there), homogeneity ∥tx∥=∣t∣ ∥x∥\lVert tx\rVert=|t|\,\lVert x\rVert (claim 5) and the triangle inequality (claim 6). Throughout, cε=(ε−1)dc_{\varepsilon}=(\varepsilon^{-1})^{d}, a positive real number, since 0<ε−10<\varepsilon^{-1}.

Step 1 (Claim 1).

(1a) Scaling. By Rescaling a Mollifier Kernel, applied with n=dn=d, the kernel η\eta of radius δ=1\delta=1 and the given ε\varepsilon, the function ηε\eta_{\varepsilon} is a mollifier kernel of radius ε⋅1=ε\varepsilon\cdot1=\varepsilon. Hence, by conditions 1 to 4 of Mollifier Kernel of Radius δ\delta on Rn\mathbb{R}^n: η\eta and ηε\eta_{\varepsilon} are smooth on Rd\mathbb{R}^{d} and nonnegative; η(z)=0\eta(z)=0 whenever 1<∥z∥1<\lVert z\rVert and ηε(z)=0\eta_{\varepsilon}(z)=0 whenever ε<∥z∥\varepsilon<\lVert z\rVert; and both are integrable with respect to λd\lambda_{d} with integral 11.

(1b) Continuity. Rd\mathbb{R}^{d} is open in itself by claim 1 of Euclidean Space is Open in Itself, and CkC^k Maps are Continuous, so claim 3 of that lemma (with U=RdU=\mathbb{R}^{d}, m=1m=1, in its version for smooth maps) shows that η\eta and ηε\eta_{\varepsilon} are continuous relative to Rd\mathbb{R}^{d} at every point, as maps into (R,dR)(\mathbb{R},d_{\mathbb{R}}) with the absolute-value metric; this is continuity in the sense of Differential Calculus and Convexity on Euclidean Open Sets: Standing Notation §extrema, and also continuity into R\mathbb{R} with its Euclidean distance, which is dRd_{\mathbb{R}} by The Euclidean Distance on the Real Line is the Absolute Value Metric. Both functions are therefore Borel by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps.

(1c) Test function. As η(z)=0\eta(z)=0 whenever 1<∥z∥1<\lVert z\rVert, claim 2 of Compact Support on Rn\mathbb{R}^n Means Vanishing Outside a Bounded Set (with R=1R=1) shows that η\eta is compactly supported for the topology of open subsets of (Rd,dE)(\mathbb{R}^{d},d_{E}), which is the topology of Test Functions on Euclidean Space, Their Gradient Maps and Laplacians §space by Euclidean Openness Agrees with Metric Openness on Rn\mathbb{R}^n. Being smooth, η\eta is a test function.

(1d) The bound SS. By claim 1 of A Continuous Compactly Supported Function on Rn\mathbb{R}^n is Bounded and Integrable, which applies by (1b) and (1c), η\eta is bounded: there is a real M≥0M\ge0 with ∣η(z)∣≤M|\eta(z)|\le M for all zz (Bounded Real-Valued Function on a Set). Then S=M+1S=M+1 is positive and η(z)≤∣η(z)∣≤M<S\eta(z)\le|\eta(z)|\le M<S for every zz. Now let SS be any real number with η(z)≤S\eta(z)\le S for all zz. For z∈Rdz\in\mathbb{R}^{d}, (1a) gives 0≤ηε(z)0\le\eta_{\varepsilon}(z), and ηε(z)=cε η(ε−1z)≤cεS\eta_{\varepsilon}(z)=c_{\varepsilon}\,\eta(\varepsilon^{-1}z)\le c_{\varepsilon}S because 0<cε0<c_{\varepsilon}.

(1e) The bound DD. By The Gradient of a Test Function is Bounded and Square-Integrable, and Its Laplacian Bounded and Integrable, Against Every Probability Measure §gradient, applied with q=dq=d and ψ=η\psi=\eta, there is a real K≥0K\ge0 with ∥∇η(z)∥≤K\lVert\nabla\eta(z)\rVert\le K for every zz; the iith coordinate of ∇η(z)\nabla\eta(z) is ∂iη(z)\partial_{i}\eta(z) by Test Functions on Euclidean Space, Their Gradient Maps and Laplacians §gradient, so ∣∂iη(z)∣≤∥∇η(z)∥≤K|\partial_{i}\eta(z)|\le\lVert\nabla\eta(z)\rVert\le K by the coordinate bound. Thus D=KD=K has the required property.

(1f) Lipschitz bounds. Let DD be any real number with ∣∂iη(z)∣≤D|\partial_{i}\eta(z)|\le D for all z∈Rdz\in\mathbb{R}^{d} and i∈[d]i\in[d], and let z,z′∈Rdz,z'\in\mathbb{R}^{d}. By Test Functions on Euclidean Space, Their Gradient Maps and Laplacians §gradient, η\eta is of class C1C^{1} on Rd\mathbb{R}^{d}, so by clause 1 of C^k Maps on a Euclidean Open Set (read through its scalar convention, clause 3) the partial derivative ∂iη(p)\partial_{i}\eta(p) exists at every p∈Rdp\in\mathbb{R}^{d} for every i∈[d]i\in[d]. Put w0=zw^{0}=z, and for j∈[d]j\in[d] let wj∈Rdw^{j}\in\mathbb{R}^{d} have iith coordinate zi′z'_{i} for i≤ji\le j and ziz_{i} for j<ij<i; thus wd=z′w^{d}=z', and for j∈[d]j\in[d] the points wj−1w^{j-1} and wjw^{j} have the same coordinates except the jjth, which is zjz_{j} for wj−1w^{j-1} and zj′z'_{j} for wjw^{j}.

Claim (∗)(\ast): for every j∈[d]j\in[d], ∣η(wj)−η(wj−1)∣≤D ∣zj′−zj∣|\eta(w^{j})-\eta(w^{j-1})|\le D\,|z'_{j}-z_{j}|. If zj=zj′z_{j}=z'_{j} then wj=wj−1w^{j}=w^{j-1} and there is nothing to prove. Otherwise let α<β\alpha<\beta be the smaller and the larger of zj,zj′z_{j},z'_{j}. For s∈Rs\in\mathbb{R} let a[s]∈Rda[s]\in\mathbb{R}^{d} be the point with jjth coordinate ss and all other coordinates those of wj−1w^{j-1}, so a[zj]=wj−1a[z_{j}]=w^{j-1} and a[zj′]=wja[z'_{j}]=w^{j}, and let g:R→Rg:\mathbb{R}\to\mathbb{R}, g(s)=η(a[s])g(s)=\eta(a[s]). Fix s∈Rs\in\mathbb{R} and apply Slice Function and the Partial Derivative with n=dn=d, U=RdU=\mathbb{R}^{d}, f=ηf=\eta, the point a[s]a[s] and i=ji=j: the points obtained from a[s]a[s] by replacing its jjth coordinate by s′s' are the points a[s′]a[s'], which lie in U=RdU=\mathbb{R}^{d}, so ρ=1\rho=1 is admissible in its claim 1, and the slice function of its claim 2 is the restriction of gg to I={s′∈R:s−1<s′<s+1}I=\{s'\in\mathbb{R}:s-1<s'<s+1\}. Since ∂jη(a[s])\partial_{j}\eta(a[s]) exists, claim 2 there shows that g∣Ig|_{I} is differentiable at ss with derivative ∂jη(a[s])\partial_{j}\eta(a[s]). Now II is an interval with ss as an interior point by Basic Facts about Intervals of the Real Line and Their Interior Points §open-interval, R\mathbb{R} is an interval with ss as an interior point by Basic Facts about Intervals of the Real Line and Their Interior Points §whole-line, and {s′∈R:∣s′−s∣<1}=I\{s'\in\mathbb{R}:|s'-s|<1\}=I; so Differentiability at an Interior Point is a Local Property §local shows that gg is differentiable at ss with g′(s)=∂jη(a[s])g'(s)=\partial_{j}\eta(a[s]), whence ∣g′(s)∣≤D|g'(s)|\le D, and Differentiability at an Interior Point Implies Continuity There shows that gg is continuous at ss relative to R\mathbb{R}. The closed interval [α,β][\alpha,\beta] is an interval of which every point of (α,β)(\alpha,\beta) is an interior point (Basic Facts about Intervals of the Real Line and Their Interior Points §closed-interval); by claim 1 of Restriction Stability of Continuity and of the Derivative the restriction g∣[α,β]g|_{[\alpha,\beta]} is continuous on [α,β][\alpha,\beta], and by claim 2 there it is differentiable at every point of (α,β)(\alpha,\beta), with the derivative of gg. By Mean Value Theorem on a Closed Real Interval there is c∈(α,β)c\in(\alpha,\beta) with g(β)−g(α)=g′(c)(β−α)g(\beta)-g(\alpha)=g'(c)(\beta-\alpha). Hence ∣η(wj)−η(wj−1)∣=∣g(β)−g(α)∣=∣g′(c)∣(β−α)≤D ∣zj′−zj∣|\eta(w^{j})-\eta(w^{j-1})|=|g(\beta)-g(\alpha)|=|g'(c)|(\beta-\alpha)\le D\,|z'_{j}-z_{j}|, proving (∗)(\ast).

Claim (∗∗)(\ast\ast): for every j∈[d]j\in[d], ∣η(wj)−η(z)∣≤j D ∥z′−z∥|\eta(w^{j})-\eta(z)|\le j\,D\,\lVert z'-z\rVert. For every j∈[d]j\in[d], ∣zj′−zj∣≤∥z′−z∥|z'_{j}-z_{j}|\le\lVert z'-z\rVert by the coordinate bound, so (∗)(\ast) gives ∣η(wj)−η(wj−1)∣≤D∥z′−z∥|\eta(w^{j})-\eta(w^{j-1})|\le D\lVert z'-z\rVert; for j=1j=1 this is (∗∗)(\ast\ast), as w0=zw^{0}=z. If (∗∗)(\ast\ast) holds for some jj with j+1∈[d]j+1\in[d], then

∣η(wj+1)−η(z)∣≤∣η(wj+1)−η(wj)∣+∣η(wj)−η(z)∣≤D∥z′−z∥+j D∥z′−z∥=(j+1) D∥z′−z∥,|\eta(w^{j+1})-\eta(z)|\le|\eta(w^{j+1})-\eta(w^{j})|+|\eta(w^{j})-\eta(z)|\le D\lVert z'-z\rVert+j\,D\lVert z'-z\rVert=(j+1)\,D\lVert z'-z\rVert ,

the image of j+1j+1 in R\mathbb{R} being that of jj plus 11 by claim 1 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field. By induction on jj (Natural Numbers), (∗∗)(\ast\ast) holds for every j∈[d]j\in[d]; with j=dj=d and wd=z′w^{d}=z' it gives ∣η(z)−η(z′)∣≤d D ∥z−z′∥|\eta(z)-\eta(z')|\le d\,D\,\lVert z-z'\rVert.

For the rescaled kernel, ηε(z)−ηε(z′)=cε(η(ε−1z)−η(ε−1z′))\eta_{\varepsilon}(z)-\eta_{\varepsilon}(z')=c_{\varepsilon}\bigl(\eta(\varepsilon^{-1}z)-\eta(\varepsilon^{-1}z')\bigr) and ∥ε−1z−ε−1z′∥=∥ε−1(z−z′)∥=ε−1∥z−z′∥\lVert\varepsilon^{-1}z-\varepsilon^{-1}z'\rVert=\lVert\varepsilon^{-1}(z-z')\rVert=\varepsilon^{-1}\lVert z-z'\rVert by homogeneity, so the bound just proved gives ∣ηε(z)−ηε(z′)∣≤cε d D ε−1∥z−z′∥=(ε−1)d+1d D ∥z−z′∥|\eta_{\varepsilon}(z)-\eta_{\varepsilon}(z')|\le c_{\varepsilon}\,d\,D\,\varepsilon^{-1}\lVert z-z'\rVert=(\varepsilon^{-1})^{d+1}d\,D\,\lVert z-z'\rVert.

(1g) Borel compositions. Let mm be a natural number and u,v:Rm→Rdu,v:\mathbb{R}^{m}\to\mathbb{R}^{d} Borel. By the componentwise criterion recorded in Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps (claim 2 of The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets), the components ui,viu_{i},v_{i} are Borel; the iith component of w↦v(w)−u(w)w\mapsto v(w)-u(w) is vi−uiv_{i}-u_{i}, which is Borel by claim 2 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions; so w↦v(w)−u(w)w\mapsto v(w)-u(w) is Borel by the same criterion, and its composition with the Borel map ηε\eta_{\varepsilon} of (1b) is Borel, a composition of Borel maps being Borel (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps). We shall use this with maps built from the identity of Rd\mathbb{R}^{d} and constant maps, which are Borel by the same criterion, their components being coordinate projections (claims 1 and 5 of The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets), respectively constants (claim 1 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions), and with the coordinate projections of Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §projections.

(1h) Unit mass of translates. Let x∈Rdx\in\mathbb{R}^{d}. By (1g) with m=dm=d, vv the identity and uu constant equal to xx, the function y↦ηε(y−x)y\mapsto\eta_{\varepsilon}(y-x) is Borel; it is nonnegative by (1a). Since y+(−x)=y−xy+(-x)=y-x, claim 2 of Translation and Reflection Invariance of Lebesgue Measure on Rn\mathbb{R}^n, applied with n=dn=d, a=−xa=-x and the nonnegative measurable function ηε\eta_{\varepsilon}, gives ∫Rdηε(y−x) λd(dy)=∫Rdηε dλd\int_{\mathbb{R}^{d}}\eta_{\varepsilon}(y-x)\,\lambda_{d}(dy)=\int_{\mathbb{R}^{d}}\eta_{\varepsilon}\,d\lambda_{d} in [0,∞][0,\infty]. For a nonnegative integrable function the integral in [0,∞][0,\infty] equals the real integral, its positive part being the function and its negative part 00 (Integrable Function and the Lebesgue Integral); so by (1a) both sides equal 11, and y↦ηε(y−x)y\mapsto\eta_{\varepsilon}(y-x) is integrable by the criterion of Measure Spaces and the Lebesgue Integral: Standing Notation §integral. This completes the proof of claim 1.

Step 2 (Claim 2). Let DD be as in claim 1, let x,x′∈Rdx,x'\in\mathbb{R}^{d}, put δ=∥x−x′∥\delta=\lVert x-x'\rVert, and let f(y)=∣ηε(y−x)−ηε(y−x′)∣f(y)=|\eta_{\varepsilon}(y-x)-\eta_{\varepsilon}(y-x')|. By (1h) and claims 2 and 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, ff is Borel, and it is nonnegative. Put K0=ε−1(2+2dd κdD)K_{0}=\varepsilon^{-1}(2+2^{d}d\,\kappa_{d}D); here 0<κd0<\kappa_{d} by The Lebesgue Measure of a Closed Ball in Rn\mathbb{R}^n §constant, so 2dd κdD≥02^{d}d\,\kappa_{d}D\ge0.

Since both kernels are nonnegative, f(y)≤ηε(y−x)+ηε(y−x′)f(y)\le\eta_{\varepsilon}(y-x)+\eta_{\varepsilon}(y-x'), so claim 1 of Linearity and Monotonicity of the Lebesgue Integral and (1h) give ∫Rdf dλd≤1+1=2\int_{\mathbb{R}^{d}}f\,d\lambda_{d}\le1+1=2.

Case ε≤δ\varepsilon\le\delta. Then 2=2ε−1ε≤2ε−1δ≤K0 δ2=2\varepsilon^{-1}\varepsilon\le2\varepsilon^{-1}\delta\le K_{0}\,\delta.

Case δ<ε\delta<\varepsilon. Let B=Bˉ(x,2ε)B=\bar{B}(x,2\varepsilon); by The Lebesgue Measure of a Closed Ball in Rn\mathbb{R}^n §borel and The Lebesgue Measure of a Closed Ball in Rn\mathbb{R}^n §value it is Borel with λd(B)=κd(2ε)d\lambda_{d}(B)=\kappa_{d}(2\varepsilon)^{d}. If y∉By\notin B, then 2ε<dE(x,y)=∥y−x∥2\varepsilon<d_{E}(x,y)=\lVert y-x\rVert, and the triangle inequality applied to y−x=(y−x′)+(x′−x)y-x=(y-x')+(x'-x), with ∥x′−x∥=δ\lVert x'-x\rVert=\delta, gives ∥y−x′∥≥∥y−x∥−δ>2ε−ε=ε\lVert y-x'\rVert\ge\lVert y-x\rVert-\delta>2\varepsilon-\varepsilon=\varepsilon; since also ε<2ε<∥y−x∥\varepsilon<2\varepsilon<\lVert y-x\rVert, (1a) gives ηε(y−x)=ηε(y−x′)=0\eta_{\varepsilon}(y-x)=\eta_{\varepsilon}(y-x')=0, so f(y)=0f(y)=0. If y∈By\in B, then, as (y−x)−(y−x′)=x′−x(y-x)-(y-x')=x'-x has norm δ\delta, (1f) gives f(y)≤(ε−1)d+1d D δf(y)\le(\varepsilon^{-1})^{d+1}d\,D\,\delta. Hence f≤(ε−1)d+1d D δ 1Bf\le(\varepsilon^{-1})^{d+1}d\,D\,\delta\,\mathbf{1}_{B} pointwise, and by claim 1 of Linearity and Monotonicity of the Lebesgue Integral and The Integral of an Indicator Function is the Measure of the Set,

∫Rdf dλd≤(ε−1)d+1d D δ κd(2ε)d=2dd κdD ε−1δ≤K0 δ,\int_{\mathbb{R}^{d}}f\,d\lambda_{d}\le(\varepsilon^{-1})^{d+1}d\,D\,\delta\,\kappa_{d}(2\varepsilon)^{d}=2^{d}d\,\kappa_{d}D\,\varepsilon^{-1}\delta\le K_{0}\,\delta ,

using (ε−1)d+1(2ε)d=ε−1 2d (ε−1ε)d=2dε−1(\varepsilon^{-1})^{d+1}(2\varepsilon)^{d}=\varepsilon^{-1}\,2^{d}\,(\varepsilon^{-1}\varepsilon)^{d}=2^{d}\varepsilon^{-1}. In both cases ∫f dλd≤K0 δ\int f\,d\lambda_{d}\le K_{0}\,\delta, which is claim 2.

Step 3 (Claim 3). Let μ∈P(Rd)\mu\in\mathcal{P}(\mathbb{R}^{d}), and fix a positive S0S_{0} with η≤S0\eta\le S_{0} as in (1d). The function ηε\eta_{\varepsilon} is continuous by (1b) and satisfies ∣ηε(z)∣=ηε(z)≤cεS0|\eta_{\varepsilon}(z)|=\eta_{\varepsilon}(z)\le c_{\varepsilon}S_{0} for all zz by (1d). Hence The Convolution of a Bounded Continuous Function with a Probability Measure on Euclidean Space: Continuity, Boundedness and Differentiation Under the Integral §continuous, applied with q=dq=d, H=ηεH=\eta_{\varepsilon} and C=cεS0C=c_{\varepsilon}S_{0}, shows: for every yy the function x↦ηε(y−x)x\mapsto\eta_{\varepsilon}(y-x) is Borel and integrable with respect to μ\mu, and it is bounded by cεS0c_{\varepsilon}S_{0}; the function ηε∗μ\eta_{\varepsilon}*\mu, which is the function H∗μH*\mu of that lemma, is continuous; and so it is Borel by Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps.

Let SS be any real with η≤S\eta\le S. For y∈Rdy\in\mathbb{R}^{d} we have 0≤ηε(y−x)≤cεS0\le\eta_{\varepsilon}(y-x)\le c_{\varepsilon}S for every xx by (1d). As μ\mu is a Borel measure with μ(Rd)=1\mu(\mathbb{R}^{d})=1 (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §measures), the constant functions 00 and cεSc_{\varepsilon}S are integrable with integrals 00 and cεSc_{\varepsilon}S by claim 6(a) of Borel Measurability and Bounded Integration on a Metric Space; the monotonicity statement in claim 2 of Linearity and Monotonicity of the Lebesgue Integral gives 0≤(ηε∗μ)(y)≤cεS0\le(\eta_{\varepsilon}*\mu)(y)\le c_{\varepsilon}S.

Unit mass. Let k:Rd+d→Rk:\mathbb{R}^{d+d}\to\mathbb{R}, k(w)=ηε(pr2(w)−pr1(w))k(w)=\eta_{\varepsilon}(\mathrm{pr}_{2}(w)-\mathrm{pr}_{1}(w)), with the coordinate projections of Probability Measures on Euclidean Space and Random Vectors: Standing Notation §pairs; it is Borel by (1g) (with m=d+dm=d+d, u=pr1u=\mathrm{pr}_{1}, v=pr2v=\mathrm{pr}_{2}) and nonnegative. By Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §product the concatenation ι:Rd×Rd→Rd+d\iota:\mathbb{R}^{d}\times\mathbb{R}^{d}\to\mathbb{R}^{d+d} is measurable with respect to B(Rd)⊗B(Rd)\mathcal{B}(\mathbb{R}^{d})\otimes\mathcal{B}(\mathbb{R}^{d}) and B(Rd+d)\mathcal{B}(\mathbb{R}^{d+d}), the latter being the Borel σ\sigma-algebra of (Rd+d,dE)(\mathbb{R}^{d+d},d_{E}) (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §spaces); so k^=k∘ι\hat{k}=k\circ\iota is measurable with respect to the product σ\sigma-algebra by claim 4 of Borel Measurability and Bounded Integration on a Metric Space, and k^(x,y)=ηε(y−x)\hat{k}(x,y)=\eta_{\varepsilon}(y-x) by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §projections. The measure μ\mu is finite and λd\lambda_{d} is σ\sigma-finite by Lebesgue Measure on Euclidean Space is Sigma-Finite §sigma-finite, so the Tonelli statement of Tonelli and Fubini Theorems, applied to the measure spaces (Rd,B(Rd),μ)(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}),\mu) and (Rd,B(Rd),λd)(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}),\lambda_{d}) and the function k^\hat{k}, gives

∫Rd(∫Rdηε(y−x) μ(dx))λd(dy)=∫Rd(∫Rdηε(y−x) λd(dy))μ(dx)in [0,∞].\int_{\mathbb{R}^{d}}\Bigl(\int_{\mathbb{R}^{d}}\eta_{\varepsilon}(y-x)\,\mu(dx)\Bigr)\lambda_{d}(dy)=\int_{\mathbb{R}^{d}}\Bigl(\int_{\mathbb{R}^{d}}\eta_{\varepsilon}(y-x)\,\lambda_{d}(dy)\Bigr)\mu(dx)\qquad\text{in }[0,\infty].

By (1h) the inner integral on the right is 11 for every xx, so the right side is ∫Rd1Rd dμ=μ(Rd)=1\int_{\mathbb{R}^{d}}\mathbf{1}_{\mathbb{R}^{d}}\,d\mu=\mu(\mathbb{R}^{d})=1 by The Integral of an Indicator Function is the Measure of the Set. On the left, the inner integral of the nonnegative integrable function x↦ηε(y−x)x\mapsto\eta_{\varepsilon}(y-x) equals its real integral (ηε∗μ)(y)(\eta_{\varepsilon}*\mu)(y), as in (1h). Hence the nonnegative Borel function ηε∗μ\eta_{\varepsilon}*\mu has integral 11 in [0,∞][0,\infty]; by the criterion of Measure Spaces and the Lebesgue Integral: Standing Notation §integral it is integrable with respect to λd\lambda_{d}, and its real integral is 11, as in (1h). This proves claim 3.

Step 4 (Claim 4). Let μ\mu, LL and Φ\Phi be as in claim 4. By claim 3, h=ηε∗μh=\eta_{\varepsilon}*\mu is a Borel, nonnegative function, integrable with respect to λd\lambda_{d} with integral 11. The composition clause Supporting Lines, Composition and Jensen's Inequality for a Convex Lipschitz Integrand §composition, applied to the measure space (Rd,B(Rd),λd)(\mathbb{R}^{d},\mathcal{B}(\mathbb{R}^{d}),\lambda_{d}), whose measurable real functions are the Borel ones (Probability Measures on Euclidean Space and Random Vectors: Standing Notation §borel-maps), and to hh, shows that Φ∘h\Phi\circ h is Borel, that 0≤Φ(h(y))≤L h(y)0\le\Phi(h(y))\le L\,h(y) for every yy, and that Φ∘h\Phi\circ h is integrable with 0≤∫Φ∘h dλd≤L∫h dλd=L0\le\int\Phi\circ h\,d\lambda_{d}\le L\int h\,d\lambda_{d}=L. This proves claim 4.

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