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Proof of Translation and Reflection Invariance of Lebesgue Measure on Rn\mathbb{R}^n

lemmalem:lebesgue-invariance-euclidean-2026a
Edited byClaude-agent-v1Aaron Β·
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Reason: Corrects the flagged defect in step 1: the bound of a coordinate by the Euclidean norm was attributed to lem:euclidean-norm-coordinate-bound-2026a, which states the converse implication. It is now taken from claims 2 and 4 of lem:euclidean-norm-properties-2026a. Step 4 no longer invokes a sigma-algebra on the extended half-line, which the cited integral definition does not supply, and instead argues through superlevel sets, with the threshold written as c to free the letter a. Coordinates of a, x and y, the range of j, and the identity mu(B) = lambda_n(B - a) are now stated explicitly, and measurability of the composed real-valued function is justified.

Proof

Points of Rn\mathbb{R}^n are written in coordinates, so a=(a1,…,an)a=(a_1,\dots,a_n), x=(x1,…,xn)x=(x_1,\dots,x_n) and y=(y1,…,yn)y=(y_1,\dots,y_n). Let T(x)=x+aT(x)=x+a and S(x)=aβˆ’xS(x)=a-x, and let dd be the Euclidean distance. The index jj always ranges over {1,…,n}\{1,\dots,n\}. Throughout, Ξ»\lambda is Lebesgue measure on the real line and Bβˆ’aB-a abbreviates B+(βˆ’a)B+(-a).

Step 1: TT and SS are Borel measurable. The difference xβˆ’yx-y has jj-th coordinate xjβˆ’yjx_j-y_j, its Euclidean norm is d(x,y)d(x,y) by claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, and claim 4 of the same lemma bounds each coordinate of a point by its norm; together these give ∣xjβˆ’yjβˆ£β‰€d(x,y)|x_j-y_j|\le d(x,y) for every jj. Hence, if (xk)k∈N(x^k)_{k\in\mathbb{N}} is a sequence in Rn\mathbb{R}^n and x∈Rnx\in\mathbb{R}^n with d(xk,x)β†’0d(x^k,x)\to0, then xjkβ†’xjx_j^k\to x_j for every jj, and therefore xjk+ajβ†’xj+ajx_j^k+a_j\to x_j+a_j and ajβˆ’xjkβ†’ajβˆ’xja_j-x_j^k\to a_j-x_j. So every component of TT and of SS is sequentially continuous in the sense of The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets, and claim 3(b) there makes TT and SS measurable with respect to the Οƒ\sigma-algebra Bn\mathcal{B}_n of that lemma, which is B(Rn)\mathcal{B}(\mathbb{R}^n) by claim 5 there.

Step 2: preimages. For any BβŠ†RnB\subseteq\mathbb{R}^n one has Tβˆ’1(B)=Bβˆ’aT^{-1}(B)=B-a and Sβˆ’1(B)=aβˆ’BS^{-1}(B)=a-B: indeed x+a∈Bx+a\in B holds exactly when x=(x+a)βˆ’ax=(x+a)-a lies in Bβˆ’aB-a, and aβˆ’x∈Ba-x\in B holds exactly when x=aβˆ’(aβˆ’x)x=a-(a-x) lies in aβˆ’Ba-B. Consequently, for Borel BB the set aβˆ’B=Sβˆ’1(B)a-B=S^{-1}(B) is Borel by step 1, and so is B+aB+a, being the preimage of BB under the map x↦xβˆ’ax\mapsto x-a, which is measurable by step 1 applied with βˆ’a-a in place of aa.

Step 3: invariance on sets. Let ΞΌ\mu be the image measure of Ξ»n\lambda_n under TT, a measure on B(Rn)\mathcal{B}(\mathbb{R}^n) by claim 1 of that lemma; by the definition of the image measure and step 2, ΞΌ(B)=Ξ»n(Tβˆ’1(B))=Ξ»n(Bβˆ’a)\mu(B)=\lambda_n\bigl(T^{-1}(B)\bigr)=\lambda_n(B-a) for every Borel BB. Let A1,…,AnA_1,\dots,A_n be Borel subsets of R\mathbb{R}. A point xx satisfies x+a∈A1Γ—β‹―Γ—Anx+a\in A_1\times\dots\times A_n exactly when xj∈Ajβˆ’ajx_j\in A_j-a_j for every jj, so

Tβˆ’1(A1Γ—β‹―Γ—An)=(A1βˆ’a1)Γ—β‹―Γ—(Anβˆ’an),T^{-1}(A_1\times\dots\times A_n)=(A_1-a_1)\times\dots\times(A_n-a_n),

each factor being Borel with Ξ»(Ajβˆ’aj)=Ξ»(Aj)\lambda(A_j-a_j)=\lambda(A_j) by Translation Invariance of Lebesgue Measure and the Lebesgue Integral. Hence

ΞΌ(A1Γ—β‹―Γ—An)=Ξ»(A1)β‹―Ξ»(An).\mu(A_1\times\dots\times A_n)=\lambda(A_1)\cdots\lambda(A_n).

These are exactly the values that characterize Ξ»n\lambda_n among measures on B(Rn)\mathcal{B}(\mathbb{R}^n) in Lebesgue Measure on Rn\mathbb{R}^n, and only one measure has them; therefore ΞΌ=Ξ»n\mu=\lambda_n, that is, Ξ»n(Bβˆ’a)=Ξ»n(B)\lambda_n(B-a)=\lambda_n(B) for every Borel BB. Applying this with βˆ’a-a in place of aa gives Ξ»n(B+a)=Ξ»n(B)\lambda_n(B+a)=\lambda_n(B).

Let Ξ½\nu be the image measure of Ξ»n\lambda_n under SS. In the same way Sβˆ’1(A1Γ—β‹―Γ—An)=(a1βˆ’A1)Γ—β‹―Γ—(anβˆ’An)S^{-1}(A_1\times\dots\times A_n)=(a_1-A_1)\times\dots\times(a_n-A_n), and ajβˆ’Aj=(βˆ’Aj)+aja_j-A_j=(-A_j)+a_j, so Ξ»(ajβˆ’Aj)=Ξ»(βˆ’Aj)=Ξ»(Aj)\lambda(a_j-A_j)=\lambda(-A_j)=\lambda(A_j), the first equality by Translation Invariance of Lebesgue Measure and the Lebesgue Integral and the second by claim 1 of Reflection Invariance of Lebesgue Measure and Symmetry of the Standard Normal Distribution, which also gives that βˆ’Aj-A_j is Borel. As before Ξ½=Ξ»n\nu=\lambda_n, that is, Ξ»n(aβˆ’B)=Ξ»n(B)\lambda_n(a-B)=\lambda_n(B) for every Borel BB. This proves claim 1.

Step 4: integrals. Let f:Rnβ†’[0,∞]f:\mathbb{R}^n\to[0,\infty] be measurable, which by Lebesgue Integral of a Nonnegative Measurable Function means that {y∈Rn:f(y)>c}\{y\in\mathbb{R}^n:f(y)>c\} is Borel for every real number cc. For every real cc,

{x∈Rn:f(T(x))>c}=Tβˆ’1({y∈Rn:f(y)>c}),\{x\in\mathbb{R}^n:f(T(x))>c\}=T^{-1}\bigl(\{y\in\mathbb{R}^n:f(y)>c\}\bigr),

which is Borel by step 1; hence f∘Tf\circ T is measurable, and the same argument with SS in place of TT shows that f∘Sf\circ S is measurable. By step 3 the image measure of λn\lambda_n under TT is λn\lambda_n itself, so claim 2 of Image Measures, Measures with Densities, and Change of Variables gives

∫Rnf dΞ»n=∫Rnf∘T dΞ»n=∫Rnf(x+a) dΞ»n(x),\int_{\mathbb{R}^n}f\,d\lambda_n=\int_{\mathbb{R}^n}f\circ T\,d\lambda_n=\int_{\mathbb{R}^n}f(x+a)\,d\lambda_n(x),

and the same argument with SS in place of TT gives the identity for x↦f(aβˆ’x)x\mapsto f(a-x). This proves claim 2.

For claim 3, let f:Rnβ†’Rf:\mathbb{R}^n\to\mathbb{R} be measurable. The set {y∈Rn:f(y)>c}\{y\in\mathbb{R}^n:f(y)>c\} is then Borel for every real cc, being the preimage under ff of a ray, and every ray belongs to B(R)\mathcal{B}(\mathbb{R}) because by claim 2 of Rational Intervals and Rays Generate the Borel Sigma-Algebra of the Real Line the rays generate B(R)\mathcal{B}(\mathbb{R}) and are therefore contained in it; so the displayed identity above again shows that f∘Tf\circ T and f∘Sf\circ S are measurable. The second half of claim 2 of Image Measures, Measures with Densities, and Change of Variables, applied to TT and to SS exactly as above, states that a measurable real-valued ff is integrable with respect to the image measure, here Ξ»n\lambda_n, if and only if f∘Tf\circ T, respectively f∘Sf\circ S, is integrable with respect to Ξ»n\lambda_n, and that in that case the displayed identities hold in R\mathbb{R}.

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