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Proof of Gaussian Smoothing of a Kernel-Weighted Discrete Family with Countable Support: Joint Density, van Trees Regularity, and the Symmetrised Directional Score Bound

lemmalem:kernel-smoothing-score-bound-2026a
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Reason: First version: proof of lemma A' by differentiation under the counting-measure integral, reindexing along the moves, the averaging inequality for the main term and the Gaussian first-order remainder for the rest.

Proof

Preliminaries. We call The Gaussian Smoothing Weight: Normalization, Derivatives, Exponential Tilting, Moments, and First-Order Remainder the weight lemma and Weighted Cauchy-Schwarz Inequality on a Measure Space and the Symmetrised Score Functional: Bounds and Averaging the averaging lemma. Integrals of nonnegative functions are handled with claim 1 of Linearity and Monotonicity of the Lebesgue Integral (linearity, monotonicity), integrable functions with claim 2 there and Integrable Function and the Lebesgue Integral; the monotone convergence theorem (MCT) and the dominated convergence theorem (DCT) are used on the measure spaces (S,2S,c)(\mathsf{S},2^{\mathsf{S}},\mathsf{c}), (Rd,B(Rd),λd)(\mathbb{R}^d,\mathcal{B}(\mathbb{R}^d),\lambda_d), (R,R,ρ)(\mathsf{R},\mathcal{R},\rho) and the product (Rd×R,B(Rd)R,λdρ)(\mathbb{R}^d\times\mathsf{R},\mathcal{B}(\mathbb{R}^d)\otimes\mathcal{R},\lambda_d\otimes\rho); on the last, Tonelli and Fubini Theorems (Tonelli) applies, both factors being σ\sigma-finite. Sums, products, absolute values and pointwise limits of measurable real functions are measurable by Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions. Write d(,)d(\cdot,\cdot) for the Euclidean distance; d(θx,θx)=d(θ,θ)d(\theta-x,\theta'-x)=d(\theta,\theta') for all θ,θ,x\theta,\theta',x, so translates of sequentially continuous functions are sequentially continuous, and sequentially continuous functions on Rd\mathbb{R}^d are measurable by claim 3(a) of The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets.

(P1) Countable sums. Since S\mathsf{S} is countable, there is a sequence (xk)kN(x_k)_{k\in\mathbb{N}} in S\mathsf{S} whose set of values is S\mathsf{S} (a constant sequence if S\mathsf{S} is a single point; otherwise enumerate, repeating values if S\mathsf{S} is finite); put Fk={x1,,xk}F_k=\{x_1,\dots,x_k\}, a nondecreasing sequence of finite sets with union S\mathsf{S}, so that every finite subset of S\mathsf{S} is contained in some FkF_k. For h:S[0,]h:\mathsf{S}\to[0,\infty] the finite partial sums xFkh(x)=h1Fkdc\sum_{x\in F_k}h(x)=\int h\mathbf{1}_{F_k}\,d\mathsf{c} are nondecreasing in kk and cofinal among all finite partial sums, hence xSh(x)=supkxFkh(x)\sum_{x\in\mathsf{S}}h(x)=\sup_k\sum_{x\in F_k}h(x); for c\mathsf{c}-integrable real hh, DCT with the dominating function h|h| gives hdc=limkxFkh(x)\int h\,d\mathsf{c}=\lim_k\sum_{x\in F_k}h(x). Consequently a function on R\mathsf{R} (or on Rd×R\mathbb{R}^d\times\mathsf{R}) of the form rxSh(x,r)r\mapsto\sum_{x\in\mathsf{S}}h(x,r) with each h(x,)h(x,\cdot) measurable and nonnegative (resp. with h(,r)h(\cdot,r) c\mathsf{c}-integrable for every rr) is measurable, as a supremum (measurable by the MCT, which asserts measurability of the supremum) resp. a pointwise limit (claim 5 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions) of the measurable finite sums xFkh(x,)\sum_{x\in F_k}h(x,\cdot); and for such nonnegative hh, MCT on (R,ρ)(\mathsf{R},\rho) applied to the finite partial sums gives xSh(x,r)ρ(dr)=xSh(x,r)ρ(dr)\int\sum_{x\in\mathsf{S}}h(x,r)\,\rho(dr)=\sum_{x\in\mathsf{S}}\int h(x,r)\,\rho(dr), and likewise on (Rd,λd)(\mathbb{R}^d,\lambda_d) and on the product.

(P2) Reindexing along a move. Fix jj and let σj:SS\sigma_j:\mathsf{S}\to\mathsf{S}, σj(x)=x+aj\sigma_j(x)=x+a_j, which is injective with image Sj+={yS:yajS}\mathsf{S}_j^{+}=\{y\in\mathsf{S}:y-a_j\in\mathsf{S}\}. Let H:S[0,)H:\mathsf{S}\to[0,\infty) vanish off Sj+\mathsf{S}_j^{+}. For a finite FSF\subseteq\mathsf{S}, reindexing along the bijection σj:Fσj(F)\sigma_j:F\to\sigma_j(F) (claim 2 of Properties of a Sum over a Finite Index Set) gives xFH(x+aj)=yσj(F)H(y)\sum_{x\in F}H(x+a_j)=\sum_{y\in\sigma_j(F)}H(y); conversely, for a finite FSF'\subseteq\mathsf{S}, dropping the vanishing terms off Sj+\mathsf{S}_j^{+} (claims 3 and 4 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set) gives yFH(y)=yFSj+H(y)=xσj1(F)H(x+aj)\sum_{y\in F'}H(y)=\sum_{y\in F'\cap\mathsf{S}_j^{+}}H(y)=\sum_{x\in\sigma_j^{-1}(F')}H(x+a_j). So the two families of finite partial sums coincide, and

xSH(x+aj)=ySH(y).(R)\sum_{x\in\mathsf{S}}H(x+a_j)=\sum_{y\in\mathsf{S}}H(y).\tag{R}

(P3) Translations in θ\theta. For bRdb\in\mathbb{R}^d the map Tb(θ,r)=(θb,r)\mathsf{T}_b(\theta,r)=(\theta-b,r) is measurable on the product: the preimage of a rectangle A×BA\times B (AB(Rd)A\in\mathcal{B}(\mathbb{R}^d), BRB\in\mathcal{R}) is (A+b)×B(A+b)\times B, with A+bA+b Borel by claim 1 of Translation and Reflection Invariance of Lebesgue Measure on Rn\mathbb{R}^n, and such rectangles generate the product σ\sigma-algebra. For measurable F0F\ge0 on the product, Tonelli and claim 2 of Translation and Reflection Invariance of Lebesgue Measure on Rn\mathbb{R}^n applied to each section give FTbd(λdρ)=Fd(λdρ)\int F\circ\mathsf{T}_b\,d(\lambda_d\otimes\rho)=\int F\,d(\lambda_d\otimes\rho), and RdF(θb,r)λd(dθ)=RdF(θ,r)λd(dθ)\int_{\mathbb{R}^d}F(\theta-b,r)\,\lambda_d(d\theta)=\int_{\mathbb{R}^d}F(\theta,r)\,\lambda_d(d\theta) for every rr. In particular φη(θx)λd(dθ)=1\int\varphi_\eta(\theta-x)\,\lambda_d(d\theta)=1 (claim 1 of the weight lemma).

(P4) Cauchy-Schwarz on S\mathsf{S}. For α:SR\alpha:\mathsf{S}\to\mathbb{R} and β:S[0,)\beta:\mathsf{S}\to[0,\infty) with xβ(x)<\sum_x\beta(x)<\infty, α=0\alpha=0 where β=0\beta=0, and xα(x)2/β(x)<\sum_x\alpha(x)^{2}/\beta(x)<\infty (terms with β(x)=0\beta(x)=0 read as 00), claim 1 of the averaging lemma on (S,c)(\mathsf{S},\mathsf{c}) gives that α\alpha is c\mathsf{c}-integrable and (xα(x))2(xβ(x))(xα(x)2/β(x))(\sum_x\alpha(x))^{2}\le(\sum_x\beta(x))(\sum_x\alpha(x)^{2}/\beta(x)).

(P5) Sequential continuity implies continuity. Let G:RdRG:\mathbb{R}^d\to\mathbb{R} be sequentially continuous and θRd\theta\in\mathbb{R}^d. If GG were not continuous at θ\theta, there would be ε>0\varepsilon>0 such that for every natural kk some θk\theta^{k} has d(θk,θ)<1/kd(\theta^{k},\theta)<1/k and G(θk)G(θ)ε|G(\theta^{k})-G(\theta)|\ge\varepsilon (using Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field to pass between squared and unsquared inequalities); then d(θk,θ)0d(\theta^{k},\theta)\to0 while G(θk)↛G(θ)G(\theta^{k})\not\to G(\theta), a contradiction.

(P6) Vanishing off R+\mathsf{R}_{+}. If rR+r\notin \mathsf{R}_{+} then xp(x)f(x,r)=0\sum_xp(x)f(x,r)=0, so f(x,r)=0f(x,r)=0 for every xSx\in\mathsf{S} (each p(x)>0p(x)>0); hence every function below of the form xp(x)f(x,r)()\sum_xp(x)f(x,r)(\cdots) vanishes at such rr, in particular gg, gjg_j, gˉ\bar g, ig\partial_ig, A1A_1 and BjB_j.

Step 1: claim 1. S\mathsf{S} is nonempty, since otherwise the sum of pp over Rd\mathbb{R}^d would be 00 rather than 11. By (K2) and xp(x)=1\sum_xp(x)=1, fˉ(r)xp(x)M(r)=M(r)<\bar f(r)\le\sum_xp(x)M(r)=M(r)<\infty for every rr. For each xx, (θ,r)p(x)φη(θx)f(x,r)(\theta,r)\mapsto p(x)\varphi_\eta(\theta-x)f(x,r) is measurable on the product, being the product of the compositions of the measurable maps θφη(θx)\theta\mapsto\varphi_\eta(\theta-x) and rf(x,r)r\mapsto f(x,r) with the coordinate projections (whose preimages are rectangles); it is nonnegative and at most cηp(x)f(x,r)c_\eta p(x)f(x,r) (claim 1 of the weight lemma). By (P1), fˉ\bar f is R\mathcal{R}-measurable, gg is measurable on the product, and R+={fˉ>0}R\mathsf{R}_{+}=\{\bar f>0\}\in\mathcal{R}; monotonicity gives 0gcηfˉ(r)<0\le g\le c_\eta\bar f(r)<\infty, so gg is finite. For each xx and jj, the maps rp(x)f(x,r)r\mapsto p(x)f(x,r) and rpj(x)fj(x,r)r\mapsto p_j(x)f_j(x,r) are R\mathcal{R}-measurable (the latter is either 00 or p(xaj)f(xaj,)p(x-a_j)f(x-a_j,\cdot)), so rΦw(p(x)f(x,r),p1(x)f1(x,r),,pn(x)fn(x,r))r\mapsto\Phi_w(p(x)f(x,r),p_1(x)f_1(x,r),\dots,p_n(x)f_n(x,r)) is measurable by claim 2(a) of the averaging lemma and Sequentially Continuous Functions of Measurable Euclidean Maps are Measurable, and Jsym\mathsf{J}^{\mathrm{sym}} is well defined. For fixed rr, MCT on (Rd,λd)(\mathbb{R}^d,\lambda_d) applied to the finite partial sums, together with (P3) and linearity, gives g(θ,r)λd(dθ)=supkxFkp(x)f(x,r)=fˉ(r)\int g(\theta,r)\,\lambda_d(d\theta)=\sup_k\sum_{x\in F_k}p(x)f(x,r)=\bar f(r). Tonelli and (P1) then give gd(λdρ)=fˉdρ=xp(x)f(x,r)ρ(dr)=xp(x)=1\int g\,d(\lambda_d\otimes\rho)=\int\bar f\,d\rho=\sum_xp(x)\int f(x,r)\rho(dr)=\sum_xp(x)=1 by (K1) and the definition of a probability mass function (whose sum over Rd\mathbb{R}^d equals its sum over S\mathsf{S}, all other terms vanishing). Positivity: g(θ,r)>0g(\theta,r)>0 if and only if some summand is positive, if and only if f(x,r)>0f(x,r)>0 for some xx (as p>0p>0 on S\mathsf{S} and φη>0\varphi_\eta>0), if and only if fˉ(r)>0\bar f(r)>0. For gj=gTajg_j=g\circ\mathsf{T}_{a_j} the same statements follow from (P3) (measurability, invariance of the θ\theta-integral) and from gj(θ,r)>0    g(θaj,r)>0    rR+g_j(\theta,r)>0\iff g(\theta-a_j,r)>0\iff r\in \mathsf{R}_{+}; for gˉ\bar g, a convex combination of g,g1,,gng,g_1,\dots,g_n, they follow by linearity, and gˉ>0\bar g>0 exactly where g>0g>0.

Step 2: claim 2. Fix rRr\in\mathsf{R} and ii. Differentiation under the sum. Fix θRd\theta\in\mathbb{R}^d, let I=(θi1,θi+1)I=(\theta_i-1,\theta_i+1), and for tIt\in I let θ[t]\theta[t] be the point with iith coordinate tt and the other coordinates those of θ\theta. Define F:I×SRF:I\times\mathsf{S}\to\mathbb{R} by F(t,x)=p(x)f(x,r)φη(θ[t]x)F(t,x)=p(x)f(x,r)\varphi_\eta(\theta[t]-x). We verify the hypotheses of Differentiation under the Integral Sign on (S,2S,c)(\mathsf{S},2^{\mathsf{S}},\mathsf{c}): (i) for each tt, F(t,)cηp()f(,r)|F(t,\cdot)|\le c_\eta p(\cdot)f(\cdot,r), which is c\mathsf{c}-integrable with integral cηfˉ(r)<c_\eta\bar f(r)<\infty; (ii) for each xx and t0It_0\in I, the translate τx(θ)=φη(θx)\tau_x(\theta')=\varphi_\eta(\theta'-x) has, at θ[t0]\theta[t_0], exactly the difference quotients of φη\varphi_\eta at θ[t0]x\theta[t_0]-x in the iith variable, so by claim 2 of the weight lemma and Partial Derivative on a Euclidean Open Set its iith partial derivative at θ[t0]\theta[t_0] exists and equals iφη(θ[t0]x)\partial_i\varphi_\eta(\theta[t_0]-x); unwinding that definition (the point obtained from θ[t0]\theta[t_0] by increasing the iith coordinate by hh is θ[t0+h]\theta[t_0+h], which lies in the domain Rd\mathbb{R}^d, and t0+hIt_0+h\in I for h|h| small) says verbatim that tτx(θ[t])t\mapsto\tau_x(\theta[t]) is differentiable at t0t_0 with derivative iφη(θ[t0]x)\partial_i\varphi_\eta(\theta[t_0]-x), whence D1F(t0,x)=p(x)f(x,r)iφη(θ[t0]x)D_1F(t_0,x)=p(x)f(x,r)\,\partial_i\varphi_\eta(\theta[t_0]-x) by the constant-multiple rule (claim 2 of Sum, Constant Multiple, and Product Rules for One-Dimensional Derivatives); (iii) D1F(t,x)cη(2η)1/2p(x)f(x,r)|D_1F(t,x)|\le c_\eta(2\eta)^{-1/2}p(x)f(x,r) by claim 2 of the weight lemma, a c\mathsf{c}-integrable bound. Hence tF(t,x)c(dx)=g(θ[t],r)t\mapsto\int F(t,x)\,\mathsf{c}(dx)=g(\theta[t],r) is differentiable on II with derivative xp(x)f(x,r)iφη(θ[t]x)\sum_xp(x)f(x,r)\partial_i\varphi_\eta(\theta[t]-x), the summand being c\mathsf{c}-integrable. This function of tt is the slice function of g(,r)g(\cdot,r) at θ\theta in the iith variable with admissible radius 11 (claim 2 of Slice Function and the Partial Derivative, with II the interval so named there and Rd\mathbb{R}^d the open set), so ig(θ,r)\partial_ig(\theta,r) exists and equals the displayed formula at t=θit=\theta_i. The bound ig(θ,r)cη(2η)1/2fˉ(r)|\partial_ig(\theta,r)|\le c_\eta(2\eta)^{-1/2}\bar f(r) follows from (iii) and monotonicity.

Continuity. Let θkθ\theta^{k}\to\theta in Rd\mathbb{R}^d. For each xx, φη(θkx)φη(θx)\varphi_\eta(\theta^{k}-x)\to\varphi_\eta(\theta-x) and iφη(θkx)iφη(θx)\partial_i\varphi_\eta(\theta^{k}-x)\to\partial_i\varphi_\eta(\theta-x) by sequential continuity (claims 1 and 2 of the weight lemma), with the dominating functions cηp(x)f(x,r)c_\eta p(x)f(x,r) and cη(2η)1/2p(x)f(x,r)c_\eta(2\eta)^{-1/2}p(x)f(x,r); DCT on (S,c)(\mathsf{S},\mathsf{c}) gives g(θk,r)g(θ,r)g(\theta^{k},r)\to g(\theta,r) and ig(θk,r)ig(θ,r)\partial_ig(\theta^{k},r)\to\partial_ig(\theta,r). So g(,r)g(\cdot,r) and ig(,r)\partial_ig(\cdot,r) are sequentially continuous, hence continuous at every point by (P5). For rR+r\in \mathsf{R}_{+}, g(,r)>0g(\cdot,r)>0 by claim 1, and clauses 1 and 3 of C^k Maps on a Euclidean Open Set make g(,r)g(\cdot,r) of class C1C^1 on Rd\mathbb{R}^d.

Measurability and integrability of ig\partial_ig. By (P1) (integrable case), ig\partial_ig is the pointwise limit of the finite sums xFkp(x)iφη(θx)f(x,r)\sum_{x\in F_k}p(x)\partial_i\varphi_\eta(\theta-x)f(x,r), each measurable on the product as in Step 1, hence measurable. Next, with eie_i the iith unit vector, claim 2 of the weight lemma gives iφη(z)=Zei(z)φη(z)|\partial_i\varphi_\eta(z)|=|Z_{e_i}(z)|\varphi_\eta(z) with Zei(z)=zi/ηZ_{e_i}(z)=z_i/\eta and κei=1/η\kappa_{e_i}=1/\eta, so by claim 4 there, Zei2φηdλd=1/η\int Z_{e_i}^{2}\varphi_\eta\,d\lambda_d=1/\eta, and (P4)-type Cauchy-Schwarz (claim 1 of the averaging lemma on (Rd,λd)(\mathbb{R}^d,\lambda_d) with β=φη\beta=\varphi_\eta) gives Zeiφηdλd(φη)1/2(Zei2φη)1/2=η1/2\int|Z_{e_i}|\varphi_\eta\,d\lambda_d\le(\int\varphi_\eta)^{1/2}(\int Z_{e_i}^{2}\varphi_\eta)^{1/2}=\eta^{-1/2}; moreover zkiφη(z)=ηZek(z)Zei(z)φη(z)η2(Zek2+Zei2)φη(z)|z_k|\,|\partial_i\varphi_\eta(z)|=\eta\,|Z_{e_k}(z)Z_{e_i}(z)|\varphi_\eta(z)\le\tfrac{\eta}{2}(Z_{e_k}^{2}+Z_{e_i}^{2})\varphi_\eta(z), whose integral is at most 11. Since (θx)k+xk(θx)k+xk|(\theta-x)_k+x_k|\le|(\theta-x)_k|+|x_k| and xkx|x_k|\le\lVert x\rVert, (P3) yields for every xx

(1+k=1dθk)iφη(θx)λd(dθ)=(1+k=1dzk+xk)iφη(z)λd(dz)η1/2+d+dη1/2x=:C1+C2x.\int\Bigl(1+\sum_{k=1}^{d}|\theta_k|\Bigr)|\partial_i\varphi_\eta(\theta-x)|\,\lambda_d(d\theta)=\int\Bigl(1+\sum_{k=1}^{d}|z_k+x_k|\Bigr)|\partial_i\varphi_\eta(z)|\,\lambda_d(dz)\le\eta^{-1/2}+d+d\,\eta^{-1/2}\lVert x\rVert=:C_1+C_2\lVert x\rVert .

By monotonicity, ig(θ,r)xp(x)f(x,r)iφη(θx)|\partial_ig(\theta,r)|\le\sum_xp(x)f(x,r)|\partial_i\varphi_\eta(\theta-x)|, so by Tonelli, (P1) and (K1),

(1+kθk)igd(λdρ)xp(x)f(x,r)ρ(dr)(C1+C2x)=C1+C2xp(x)x<\int\Bigl(1+\sum_k|\theta_k|\Bigr)|\partial_ig|\,d(\lambda_d\otimes\rho)\le\sum_xp(x)\int f(x,r)\rho(dr)\,(C_1+C_2\lVert x\rVert)=C_1+C_2\sum_xp(x)\lVert x\rVert<\infty

by the first-moment condition. Finally, let h(v)=1/vh(v)=1/v for v>0v>0 and h(0)=0h(0)=0; as in the proof of claim 1 of the averaging lemma, hgh\circ g is measurable (a pointwise limit of g/(g2+1/k)g/(g^{2}+1/k)), so 1Rd×R+(ig)2/g=(ig)2(hg)\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}(\partial_ig)^{2}/g=(\partial_ig)^{2}\,(h\circ g) is measurable, the two sides agreeing also off Rd×R+\mathbb{R}^d\times \mathsf{R}_{+} by (P6) and claim 1. For rR+r\in \mathsf{R}_{+} and any θ\theta, apply (P4) with α(x)=p(x)f(x,r)iφη(θx)\alpha(x)=p(x)f(x,r)\partial_i\varphi_\eta(\theta-x) and β(x)=p(x)f(x,r)φη(θx)\beta(x)=p(x)f(x,r)\varphi_\eta(\theta-x) (so xβ=g(θ,r)>0\sum_x\beta=g(\theta,r)>0, α=0\alpha=0 where β=0\beta=0, and α2/β=p(x)f(x,r)Zei(θx)2φη(θx)\alpha^{2}/\beta=p(x)f(x,r)Z_{e_i}(\theta-x)^{2}\varphi_\eta(\theta-x) where β>0\beta>0):

ig(θ,r)2g(θ,r)xp(x)f(x,r)Zei(θx)2φη(θx),\frac{\partial_ig(\theta,r)^{2}}{g(\theta,r)}\le\sum_xp(x)f(x,r)\,Z_{e_i}(\theta-x)^{2}\varphi_\eta(\theta-x),

provided the right side is finite, and trivially otherwise. Integrating with Tonelli, (P1), (P3) and (K1), 1Rd×R+(ig)2/gd(λdρ)xp(x)1Zei2φηdλd=1/η\int\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}(\partial_ig)^{2}/g\,d(\lambda_d\otimes\rho)\le\sum_xp(x)\cdot1\cdot\int Z_{e_i}^{2}\varphi_\eta\,d\lambda_d=1/\eta.

Step 3: claim 3. Decomposition. By linearity of the c\mathsf{c}-integral, ug(θ,r)=xp(x)f(x,r)i=1duiiφη(θx)\partial_ug(\theta,r)=\sum_xp(x)f(x,r)\sum_{i=1}^{d}u_i\partial_i\varphi_\eta(\theta-x), and since u=jwjaju=\sum_jw_ja_j, the definition of RajR_{a_j} in claim 5 of the weight lemma gives iuiiφη(z)=jwj(Raj(z)+φη(z)φη(zaj))\sum_iu_i\partial_i\varphi_\eta(z)=\sum_jw_j\bigl(R_{a_j}(z)+\varphi_\eta(z)-\varphi_\eta(z-a_j)\bigr). Each RajR_{a_j} is bounded (by 2cη+cη(2η)1/2i(aj)i2c_\eta+c_\eta(2\eta)^{-1/2}\sum_i|(a_j)_i|), so all the resulting summands are c\mathsf{c}-integrable, and

ug=A1+j=1nwjBj,A1(θ,r)=j=1nwj(g(θ,r)gj(θ,r)),Bj(θ,r)=xp(x)f(x,r)Raj(θx),\partial_ug=A_1+\sum_{j=1}^{n}w_jB_j,\qquad A_1(\theta,r)=\sum_{j=1}^{n}w_j\bigl(g(\theta,r)-g_j(\theta,r)\bigr),\qquad B_j(\theta,r)=\sum_xp(x)f(x,r)R_{a_j}(\theta-x),

because xp(x)f(x,r)φη(θxaj)=g(θaj,r)=gj(θ,r)\sum_xp(x)f(x,r)\varphi_\eta(\theta-x-a_j)=g(\theta-a_j,r)=g_j(\theta,r) by definition. A1A_1 is measurable by Step 1, and BjB_j by (P1) (RajR_{a_j} is sequentially continuous, hence measurable, by claim 5 of the weight lemma).

Reindexing gjg_j. Fix (θ,r)(\theta,r) and jj, and put H(y)=φη(θy)pj(y)fj(y,r)H(y)=\varphi_\eta(\theta-y)\,p_j(y)f_j(y,r) for ySy\in\mathsf{S}; HH vanishes off Sj+\mathsf{S}_j^{+} (there pj(y)=p(yaj)=0p_j(y)=p(y-a_j)=0), and for xSx\in\mathsf{S}, H(x+aj)=φη(θxaj)p(x)f(x,r)H(x+a_j)=\varphi_\eta(\theta-x-a_j)p(x)f(x,r) since (x+aj)aj=xS(x+a_j)-a_j=x\in\mathsf{S}. By (R),

gj(θ,r)=xSH(x+aj)=ySφη(θy)pj(y)fj(y,r).g_j(\theta,r)=\sum_{x\in\mathsf{S}}H(x+a_j)=\sum_{y\in\mathsf{S}}\varphi_\eta(\theta-y)\,p_j(y)f_j(y,r).

The main term. Fix rR+r\in \mathsf{R}_{+} and θ\theta. On (S,c)(\mathsf{S},\mathsf{c}) put 0(y)=φη(θy)p(y)f(y,r)\ell_0(y)=\varphi_\eta(\theta-y)p(y)f(y,r) and j(y)=φη(θy)pj(y)fj(y,r)\ell_j(y)=\varphi_\eta(\theta-y)p_j(y)f_j(y,r), nonnegative with finite integrals 0dc=g(θ,r)\int\ell_0\,d\mathsf{c}=g(\theta,r) and jdc=gj(θ,r)\int\ell_j\,d\mathsf{c}=g_j(\theta,r) (by the reindexing). Since gˉ(θ,r)=D(g,g1,,gn)(θ,r)>0\bar g(\theta,r)=\mathsf{D}(g,g_1,\dots,g_n)(\theta,r)>0 and A1=Nw(g,g1,,gn)A_1=\mathsf{N}_w(g,g_1,\dots,g_n) in the notation of the averaging lemma, claim 3 there followed by claim 2(c) (homogeneity, with the factor φη(θy)>0\varphi_\eta(\theta-y)>0) gives

A1(θ,r)2gˉ(θ,r)=Φw(g,g1,,gn)(θ,r)ySφη(θy)Φw(p(y)f(y,r),p1(y)f1(y,r),,pn(y)fn(y,r)).\frac{A_1(\theta,r)^{2}}{\bar g(\theta,r)}=\Phi_w\bigl(g,g_1,\dots,g_n\bigr)(\theta,r)\le\sum_{y\in\mathsf{S}}\varphi_\eta(\theta-y)\,\Phi_w\bigl(p(y)f(y,r),p_1(y)f_1(y,r),\dots,p_n(y)f_n(y,r)\bigr).

For each yy, rΦw(p(y)f(y,r),)r\mapsto\Phi_w(p(y)f(y,r),\dots) is R\mathcal{R}-measurable by claim 3 of the averaging lemma (its arguments are measurable in rr), so the right side is a measurable nonnegative function on the product by (P1). Integrating over θ\theta first, with (P3) and φη(θy)λd(dθ)=1\int\varphi_\eta(\theta-y)\lambda_d(d\theta)=1, then over rr, using Tonelli and (P1),

1Rd×R+A12gˉd(λdρ)ySRΦw(p(y)f(y,r),p1(y)f1(y,r),,pn(y)fn(y,r))ρ(dr)=Jsym,\int\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}\frac{A_1^{2}}{\bar g}\,d(\lambda_d\otimes\rho)\le\sum_{y\in\mathsf{S}}\int_{\mathsf{R}}\Phi_w\bigl(p(y)f(y,r),p_1(y)f_1(y,r),\dots,p_n(y)f_n(y,r)\bigr)\rho(dr)=\mathsf{J}^{\mathrm{sym}} ,

where 1Rd×R+A12/gˉ=A12(hgˉ)\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}A_1^{2}/\bar g=A_1^{2}\,(h\circ\bar g) is measurable as in Step 2.

The remainder terms. Fix jj, rR+r\in \mathsf{R}_{+} and θ\theta. Since gˉ12g>0\bar g\ge\frac12g>0, Bj2/gˉ2Bj2/gB_j^{2}/\bar g\le2B_j^{2}/g. Apply (P4) with α(x)=p(x)f(x,r)Raj(θx)\alpha(x)=p(x)f(x,r)R_{a_j}(\theta-x) and β(x)=p(x)f(x,r)φη(θx)\beta(x)=p(x)f(x,r)\varphi_\eta(\theta-x): Bj(θ,r)2/g(θ,r)xp(x)f(x,r)Raj(θx)2/φη(θx)B_j(\theta,r)^{2}/g(\theta,r)\le\sum_xp(x)f(x,r)R_{a_j}(\theta-x)^{2}/\varphi_\eta(\theta-x) (trivially if the right side is infinite). Integrating with Tonelli, (P1), (P3) and claim 5 of the weight lemma (Raj2/φηdλd=exp(κj)1κj\int R_{a_j}^{2}/\varphi_\eta\,d\lambda_d=\exp(\kappa_j)-1-\kappa_j) and (K1),

1Rd×R+Bj2gˉd(λdρ)2xp(x)(exp(κj)1κj)=2(exp(κj)1κj).\int\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}\frac{B_j^{2}}{\bar g}\,d(\lambda_d\otimes\rho)\le2\sum_xp(x)\bigl(\exp(\kappa_j)-1-\kappa_j\bigr)=2\bigl(\exp(\kappa_j)-1-\kappa_j\bigr).

Conclusion. By claim 3 of Image Measures, Measures with Densities, and Change of Variables, ν(E)=1E1Rd×R+gˉd(λdρ)\nu(E)=\int\mathbf{1}_E\,\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}\,\bar g\,d(\lambda_d\otimes\rho) is a measure on the product σ\sigma-algebra with ν(Rd×R)=gˉd(λdρ)=1\nu(\mathbb{R}^d\times\mathsf{R})=\int\bar g\,d(\lambda_d\otimes\rho)=1 (as gˉ\bar g vanishes off Rd×R+\mathbb{R}^d\times \mathsf{R}_{+} by (P6)), so it makes the product a probability space, and F2dν=F21Rd×R+gˉd(λdρ)\int F^{2}\,d\nu=\int F^{2}\,\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}\,\bar g\,d(\lambda_d\otimes\rho) for measurable FF. For a measurable real AA on the product put FA=A(hgˉ)F_A=A\,(h\circ\bar g), measurable, equal to A/gˉA/\bar g on Rd×R+\mathbb{R}^d\times \mathsf{R}_{+} and to 00 elsewhere; then FA2dν=1Rd×R+A2/gˉd(λdρ)\int F_A^{2}\,d\nu=\int\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}A^{2}/\bar g\,d(\lambda_d\otimes\rho). Whenever this is finite, FAF_A is square-integrable under ν\nu with mean-square norm FA2\lVert F_A\rVert_2 equal to its square root; FA+A=FA+FAF_{A+A'}=F_A+F_{A'} and FcA=cFAF_{cA}=cF_A, so the triangle inequality (claim 2 of Cauchy-Schwarz and Triangle Inequalities for the Mean-Square Norm, extended to finitely many summands by induction) and the homogeneity cF2=cF2\lVert cF\rVert_2=|c|\lVert F\rVert_2 (immediate from Square-Integrable Random Variables and the Mean-Square Inner Product) apply. If Jsym=\mathsf{J}^{\mathrm{sym}}=\infty the claimed inequality holds trivially. Otherwise FA1F_{A_1} and every FBjF_{B_j} are square-integrable by the two bounds above, hence so is Fug=FA1+jwjFBjF_{\partial_ug}=F_{A_1}+\sum_jw_jF_{B_j}, and

(1Rd×R+(ug)2gˉd(λdρ))1/2=Fug2FA12+j=1nwjFBj2(Jsym)1/2+j=1nwj(2(exp(κj)1κj))1/2,\Bigl(\int\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}\frac{(\partial_ug)^{2}}{\bar g}\,d(\lambda_d\otimes\rho)\Bigr)^{1/2}=\lVert F_{\partial_ug}\rVert_2\le\lVert F_{A_1}\rVert_2+\sum_{j=1}^{n}|w_j|\,\lVert F_{B_j}\rVert_2\le(\mathsf{J}^{\mathrm{sym}})^{1/2}+\sum_{j=1}^{n}|w_j|\bigl(2(\exp(\kappa_j)-1-\kappa_j)\bigr)^{1/2},

the square root being increasing on [0,)[0,\infty) (Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field) and (2t)1/2=21/2t1/2(2t)^{1/2}=2^{1/2}t^{1/2} for t0t\ge0 (the right side is nonnegative with square 2t2t). This is claim 3; the measurability of 1Rd×R+(ug)2/gˉ=(ug)2(hgˉ)\mathbf{1}_{\mathbb{R}^d\times \mathsf{R}_{+}}(\partial_ug)^{2}/\bar g=(\partial_ug)^{2}(h\circ\bar g) was noted above. \blacksquare

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