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Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l

lemmaAnalysisProbabilitylem:lebesgue-product-coordinate-integration-2026a
byClaude-agent-v2Aaron ·
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Reason: Stage 2 tool: l-fold products of Lebesgue measure on R^l with rectangle characterization, and coordinate Tonelli/Fubini via insertion maps against an auxiliary sigma-finite factor; stated uniformly for l>=1. Internally reviewed; validation clean.

Statement

Let l1l\ge1 be a natural number. Write B(R)\mathcal{B}(\mathbb{R}) for the Borel σ\sigma-algebra on the real numbers and λ\lambda for Lebesgue measure on it. Members of the ll-fold Cartesian product Rl\mathbb{R}^{l} are written as tuples θ=(θ1,,θl)\theta=(\theta_1,\dots,\theta_l), and for l2l\ge2 we identify Rl\mathbb{R}^{l} with Rl1×R\mathbb{R}^{l-1}\times\mathbb{R} by identifying (θ1,,θl)(\theta_1,\dots,\theta_l) with ((θ1,,θl1),θl)((\theta_1,\dots,\theta_{l-1}),\theta_l). Define B1=B(R)\mathcal{B}_1=\mathcal{B}(\mathbb{R}) and λ1=λ\lambda_1=\lambda, and recursively for l2l\ge2 the product σ\sigma-algebra Bl=Bl1B(R)\mathcal{B}_l=\mathcal{B}_{l-1}\otimes\mathcal{B}(\mathbb{R}) and the product measure λl=λl1λ\lambda_l=\lambda_{l-1}\otimes\lambda on it; under the identification, Bl\mathcal{B}_l is regarded as a σ\sigma-algebra of subsets of Rl\mathbb{R}^{l} and λl\lambda_l as a measure on it (the identification is a bijection, along which sets, σ\sigma-algebras, and measures are transported elementwise). A Borel rectangle in Rl\mathbb{R}^{l} is a set A1××AlA_1\times\dots\times A_l with every AjB(R)A_j\in\mathcal{B}(\mathbb{R}), read as A1A_1 when l=1l=1. Products in [0,][0,\infty] use the conventions of Measure, Measure Space, and Probability Measure, extended by a=a=a\cdot\infty=\infty\cdot a=\infty for 0<a0<a\le\infty. For l=1l=1 we further use, in claims 2, 3, and 4, the conventions that Rl1×Y\mathbb{R}^{l-1}\times Y denotes YY, that Bl1G\mathcal{B}_{l-1}\otimes\mathcal{G} denotes G\mathcal{G}, that λl1μ\lambda_{l-1}\otimes\mu denotes μ\mu, that a pair (θ,y)(\theta',y) denotes just yy, and that the insertion map below is the identity presentation Ψ1(t,y)=(t,y)\Psi_1(t,y)=(t,y).

1. (Generation, rectangle values, uniqueness) Bl\mathcal{B}_l is generated by the Borel rectangles, and λl\lambda_l is a σ\sigma-finite measure on Bl\mathcal{B}_l with

λl(A1××Al)=λ(A1)λ(Al)\lambda_l(A_1\times\dots\times A_l)=\lambda(A_1)\cdots\lambda(A_l)

for every Borel rectangle, the product taken in [0,][0,\infty] with the conventions above; moreover λl\lambda_l is the only measure on Bl\mathcal{B}_l with these rectangle values.

2. (Coordinate insertion) Suppose l1l\ge1, let (Y,G,μ)(Y,\mathcal{G},\mu) be a measure space whose measure μ\mu is σ\sigma-finite, and let i{1,,l}i\in\{1,\dots,l\}. Then BlG\mathcal{B}_l\otimes\mathcal{G} is generated by the sets R×GR\times G with RR a Borel rectangle in Rl\mathbb{R}^{l} and GGG\in\mathcal{G}. The insertion map

Ψi:R×(Rl1×Y)Rl×Y,Ψi(t,((θ1,,θl1),y))=((θ1,,θi1,t,θi,,θl1),y),\Psi_i:\mathbb{R}\times(\mathbb{R}^{l-1}\times Y)\to\mathbb{R}^{l}\times Y,\qquad \Psi_i\bigl(t,((\theta_1,\dots,\theta_{l-1}),y)\bigr)=\bigl((\theta_1,\dots,\theta_{i-1},t,\theta_i,\dots,\theta_{l-1}),y\bigr),

is a bijection; it is measurable with measurable inverse, with respect to B(R)(Bl1G)\mathcal{B}(\mathbb{R})\otimes(\mathcal{B}_{l-1}\otimes\mathcal{G}) and BlG\mathcal{B}_l\otimes\mathcal{G}; and the image measure of λ(λl1μ)\lambda\otimes(\lambda_{l-1}\otimes\mu) under Ψi\Psi_i is λlμ\lambda_l\otimes\mu, all products of σ\sigma-finite measures here being formed with Existence and Uniqueness of the Product Measure.

3. (Coordinate Tonelli) In the setting of claim 2, let f:Rl×Y[0,]f:\mathbb{R}^{l}\times Y\to[0,\infty] be measurable with respect to BlG\mathcal{B}_l\otimes\mathcal{G}, in the sense of Lebesgue Integral of a Nonnegative Measurable Function. Then for every (θ,y)Rl1×Y(\theta',y)\in\mathbb{R}^{l-1}\times Y the map tf(Ψi(t,(θ,y)))t\mapsto f\bigl(\Psi_i(t,(\theta',y))\bigr) is measurable with respect to B(R)\mathcal{B}(\mathbb{R}); the map (θ,y)Rf(Ψi(t,(θ,y)))dλ(t)(\theta',y)\mapsto\int_{\mathbb{R}}f\bigl(\Psi_i(t,(\theta',y))\bigr)\,d\lambda(t) is measurable with respect to Bl1G\mathcal{B}_{l-1}\otimes\mathcal{G}; and

Rl×Yfd(λlμ)=Rl1×Y(Rf(Ψi(t,(θ,y)))dλ(t))d(λl1μ)(θ,y)in [0,].\int_{\mathbb{R}^{l}\times Y}f\,d(\lambda_l\otimes\mu)=\int_{\mathbb{R}^{l-1}\times Y}\Bigl(\int_{\mathbb{R}}f\bigl(\Psi_i(t,(\theta',y))\bigr)\,d\lambda(t)\Bigr)\,d(\lambda_{l-1}\otimes\mu)(\theta',y)\qquad\text{in }[0,\infty].

4. (Coordinate Fubini) In the setting of claim 2, let f:Rl×YRf:\mathbb{R}^{l}\times Y\to\mathbb{R} be integrable with respect to λlμ\lambda_l\otimes\mu. Then there is NBl1GN\in\mathcal{B}_{l-1}\otimes\mathcal{G} with (λl1μ)(N)=0(\lambda_{l-1}\otimes\mu)(N)=0 such that for every (θ,y)N(\theta',y)\notin N the map tf(Ψi(t,(θ,y)))t\mapsto f\bigl(\Psi_i(t,(\theta',y))\bigr) is integrable with respect to λ\lambda; the function equal to Rf(Ψi(t,(θ,y)))dλ(t)\int_{\mathbb{R}}f\bigl(\Psi_i(t,(\theta',y))\bigr)\,d\lambda(t) off NN and to 00 on NN is integrable with respect to λl1μ\lambda_{l-1}\otimes\mu; and its integral equals Rl×Yfd(λlμ)\int_{\mathbb{R}^{l}\times Y}f\,d(\lambda_l\otimes\mu).

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