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Proof of The Logarithmic Kernel on the Real Line: Borel Measurability, a Linear Lower Bound, and the Null Diagonal of an Atomless Measure

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· 7,704 chars · 17 deps · depth 27 Reason: E1: proof of the logarithmic kernel lemma.

The kernel is the pointwise limit of Lipschitz truncations off the closed diagonal; log t <= t gives the lower bound; Tonelli gives the null diagonal of an atomless product.

Proof

Each result cited below is universally quantified over the data in its own statement, and is applied to the data named at the point of use. The rules for adding, multiplying and comparing inequalities between real numbers in Elementary Order Arithmetic in an Ordered Field and Elementary Arithmetic in an Ordered Field are used without further mention. As in One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative, a point of R2\mathbb{R}^{2} is written (x,y)(x,y), meaning ι(x,y)\iota(x,y); by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §projections the coordinate projections pr1,pr2:R2R\mathrm{pr}_{1},\mathrm{pr}_{2}:\mathbb{R}^{2}\to\mathbb{R} satisfy pr1(x,y)=x\mathrm{pr}_{1}(x,y)=x and pr2(x,y)=y\mathrm{pr}_{2}(x,y)=y, and every zR2z\in\mathbb{R}^{2} equals (pr1(z),pr2(z))(\mathrm{pr}_{1}(z),\mathrm{pr}_{2}(z)). Define ρ:R2R\rho:\mathbb{R}^{2}\to\mathbb{R} by ρ(z)=pr1(z)pr2(z)\rho(z)=|\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z)|, so that ρ(x,y)=xy\rho(x,y)=|x-y|, and write exp\exp for the exponential function of The Natural Logarithm.

Step 1 (Three properties of the logarithm). By The Natural Logarithm, log(exp(u))=u\log(\exp(u))=u and exp(logt)=t\exp(\log t)=t for real uu and t>0t>0, and log(st)=logs+logt\log(st)=\log s+\log t for s,t>0s,t>0. By claim 1 of Basic Properties of the Exponential Function, exp(0)=1\exp(0)=1, hence log1=0\log 1=0; and log(exp(u))=u\log(\exp(-u))=-u for every real uu.

(a) Monotonicity. Let 0<s<t0<s<t. If logtlogs\log t\le\log s, then, exp\exp being strictly increasing by claim 4 of Basic Properties of the Exponential Function, t=exp(logt)exp(logs)=st=\exp(\log t)\le\exp(\log s)=s, which is false; so logs<logt\log s<\log t. Consequently logslogt\log s\le\log t whenever 0<st0<s\le t; in particular 0logt0\le\log t for t1t\ge1 and logt<0\log t<0 for 0<t<10<t<1.

(b) A Lipschitz bound. Let s0,s,ts_{0},s,t be real with 0<s0ts0<s_{0}\le t\le s, and put v=log(s/t)v=\log(s/t). Then logs=logt+v\log s=\log t+v, and 0v0\le v by (a) since 1s/t1\le s/t. By claim 4 of Basic Properties of the Exponential Function, exp(v)1+v\exp(v)\ge1+v because v0v\ge0, that is s/t1+vs/t\ge1+v. Hence

0logslogt=vst1=sttsts0.0\le\log s-\log t=v\le\frac{s}{t}-1=\frac{s-t}{t}\le\frac{s-t}{s_{0}} .

(c) logtt\log t\le t for every t>0t>0. If t1t\ge1, then v=logt0v=\log t\ge0 by (a), and t=exp(v)1+v>vt=\exp(v)\ge1+v>v by claim 4 of Basic Properties of the Exponential Function. If 0<t<10<t<1, then logt<0<t\log t<0<t by (a).

Step 2 (The diagonal is Borel). The map zpr1(z)pr2(z)z\mapsto\lVert\mathrm{pr}_{1}(z)-\mathrm{pr}_{2}(z)\rVert on R2=R1+1\mathbb{R}^{2}=\mathbb{R}^{1+1} is Borel by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §functions, and it equals ρ\rho because s=s\lVert s\rVert=|s| for sR=R1s\in\mathbb{R}=\mathbb{R}^{1} by One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative §scalars; so ρ\rho is Borel. For zR2z\in\mathbb{R}^{2}, zΔz\in\Delta holds if and only if pr1(z)=pr2(z)\mathrm{pr}_{1}(z)=\mathrm{pr}_{2}(z), that is, by claim 1 of Properties of the Absolute Value in an Ordered Field, if and only if ρ(z)=0\rho(z)=0. Thus Δ=ρ1({0})\Delta=\rho^{-1}(\{0\}), and since {0}B(R)\{0\}\in\mathcal{B}(\mathbb{R}) by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §finite-sets, ΔB(R2)\Delta\in\mathcal{B}(\mathbb{R}^{2}) by the definition of a Borel map. So is R2Δ\mathbb{R}^{2}\setminus\Delta.

Step 3 (Truncated kernels). For kNk\in\mathbb{N} let sk=exp(k)s_{k}=\exp(-k), which is positive with 1/sk=exp(k)1/s_{k}=\exp(k) by claim 2 of Basic Properties of the Exponential Function, and define k:R2R\ell_{k}:\mathbb{R}^{2}\to\mathbb{R} by k(z)=log(max{ρ(z),sk})\ell_{k}(z)=-\log\bigl(\max\{\rho(z),s_{k}\}\bigr), which is defined because max{ρ(z),sk}sk>0\max\{\rho(z),s_{k}\}\ge s_{k}>0 by claim 1 of Elementary Properties of the Maximum of Two Elements.

(i) k\ell_{k} is Borel. Let z,zR2z,z'\in\mathbb{R}^{2} and put s=max{ρ(z),sk}s=\max\{\rho(z),s_{k}\}, t=max{ρ(z),sk}t=\max\{\rho(z'),s_{k}\}. Both are at least sks_{k}, so Step 1(b), applied with the larger of s,ts,t in the role of ss there, gives logslogtexp(k)st|\log s-\log t|\le\exp(k)\,|s-t|. Moreover stρ(z)ρ(z)|s-t|\le|\rho(z)-\rho(z')|: by claim 2 of Elementary Properties of the Maximum of Two Elements each maximum is attained; if both equal sks_{k} then st=0s-t=0; if s=ρ(z)sks=\rho(z)\ge s_{k} and t=skρ(z)t=s_{k}\ge\rho(z') then 0stρ(z)ρ(z)0\le s-t\le\rho(z)-\rho(z'); the case with the roles exchanged is symmetric; and if s=ρ(z)s=\rho(z), t=ρ(z)t=\rho(z') there is equality. By claims 7, 5 and 2 of Properties of the Absolute Value in an Ordered Field,

ρ(z)ρ(z)(pr1(z)pr1(z))(pr2(z)pr2(z))pr1(z)pr1(z)+pr2(z)pr2(z)2zz,|\rho(z)-\rho(z')|\le\bigl|(\mathrm{pr}_{1}(z)-\mathrm{pr}_{1}(z'))-(\mathrm{pr}_{2}(z)-\mathrm{pr}_{2}(z'))\bigr|\le|\mathrm{pr}_{1}(z)-\mathrm{pr}_{1}(z')|+|\mathrm{pr}_{2}(z)-\mathrm{pr}_{2}(z')|\le2\lVert z-z'\rVert,

the last step because both projections are Lipschitz with constant 11 by Continuity of the Coordinate Projections and of the Quadratic Cost Function, and Passage of a Cost Bound to a Weak Limit §projections, the Euclidean distance of R1\mathbb{R}^{1} being the absolute-value metric as recorded in One-Dimensional Test Functions: Scalars, Derivatives, and the Difference Quotient of the Derivative. Hence k(z)k(z)2exp(k)zz|\ell_{k}(z)-\ell_{k}(z')|\le2\exp(k)\lVert z-z'\rVert, so k\ell_{k} is Lipschitz, therefore continuous by A Lipschitz Map is Uniformly Continuous, therefore Borel by claims 3(a) 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.

(ii) Values of k\ell_{k}. If zΔz\in\Delta, then ρ(z)=0\rho(z)=0 and k(z)=logsk=k\ell_{k}(z)=-\log s_{k}=k. If zΔz\notin\Delta, then ρ(z)>0\rho(z)>0 and (z)=logρ(z)\ell(z)=-\log\rho(z); if ρ(z)sk\rho(z)\ge s_{k} then k(z)=(z)\ell_{k}(z)=\ell(z) and (z)k\ell(z)\le k because logρ(z)logsk=k\log\rho(z)\ge\log s_{k}=-k by Step 1(a); if ρ(z)<sk\rho(z)<s_{k} then k(z)=k<(z)\ell_{k}(z)=k<\ell(z) by Step 1(a). Hence k(z)=min{(z),k}\ell_{k}(z)=\min\{\ell(z),k\} for zΔz\notin\Delta.

Step 4 (Clause 1). For kNk\in\mathbb{N} let uk=k1R2Δu_{k}=\ell_{k}\,\mathbf{1}_{\mathbb{R}^{2}\setminus\Delta}, which is Borel by Steps 2 and 3(i) and claims 1 and 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions. If zΔz\in\Delta, then uk(z)=0=(z)u_{k}(z)=0=\ell(z) for every kk. If zΔz\notin\Delta, claim 1 of The Archimedean Property of the Real Numbers gives k0Nk_{0}\in\mathbb{N} with (z)<k0\ell(z)<k_{0}, and for every kk0k\ge k_{0} Step 3(ii) gives uk(z)=min{(z),k}=(z)u_{k}(z)=\min\{\ell(z),k\}=\ell(z). In either case the sequence (uk(z))kN(u_{k}(z))_{k\in\mathbb{N}} is eventually equal to (z)\ell(z) and therefore converges to (z)\ell(z). By claim 5 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, \ell is Borel. Together with Step 2 this proves clause 1.

Step 5 (Clause 2). Let x,yRx,y\in\mathbb{R}. If x=yx=y, then (x,y)=0\ell(x,y)=0, while xy0-|x|-|y|\le0 by claim 1 of Properties of the Absolute Value in an Ordered Field. If xyx\ne y, put t=xyt=|x-y|, which is positive by claim 1 of Properties of the Absolute Value in an Ordered Field. By Step 1(c), (x,y)=logtt\ell(x,y)=-\log t\ge-t, and by claims 5 and 2 of Properties of the Absolute Value in an Ordered Field, t=x+(y)x+y=x+yt=|x+(-y)|\le|x|+|-y|=|x|+|y|. Hence (x,y)xy\ell(x,y)\ge-|x|-|y|.

Step 6 (Clause 3). Let μP(R)\mu\in\mathcal{P}(\mathbb{R}) satisfy μ({x})=0\mu(\{x\})=0 for every xRx\in\mathbb{R}. The indicator 1Δ\mathbf{1}_{\Delta} is a nonnegative Borel function (Step 2), and its integral against μμ\mu\boxtimes\mu is (μμ)(Δ)(\mu\boxtimes\mu)(\Delta) by Simple Function and Its Integral and Lebesgue Integral of a Nonnegative Measurable Function. By Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §product, 1Δι\mathbf{1}_{\Delta}\circ\iota is measurable for B(R)B(R)\mathcal{B}(\mathbb{R})\otimes\mathcal{B}(\mathbb{R}) and

(μμ)(Δ)=R×R1Διd(μμ)=R(R1Δ(x,y)μ(dy))μ(dx),(\mu\boxtimes\mu)(\Delta)=\int_{\mathbb{R}\times\mathbb{R}}\mathbf{1}_{\Delta}\circ\iota\,d(\mu\otimes\mu)=\int_{\mathbb{R}}\Bigl(\int_{\mathbb{R}}\mathbf{1}_{\Delta}(x,y)\,\mu(dy)\Bigr)\mu(dx),

the second equality by the Tonelli part of Tonelli and Fubini Theorems, probability measures being σ\sigma-finite. For fixed xx, 1Δ(x,y)=1\mathbf{1}_{\Delta}(x,y)=1 exactly when y=xy=x, so the inner integrand is the indicator of {x}\{x\}, which belongs to B(R)\mathcal{B}(\mathbb{R}) by Pairs of Euclidean Points: Coordinate Projections, Pairings, the Product Measure on a Euclidean Space, Borel Norm Functions and Finite Sets §finite-sets; the inner integral is therefore μ({x})=0\mu(\{x\})=0. The outer integral is the integral of the zero function, which is 00. Hence (μμ)(Δ)=0(\mu\boxtimes\mu)(\Delta)=0.

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