TheoremBase

Proof of The Integral over the Unit Cell of a Product of One-Variable Functions

lemmalem:product-function-integral-cell-2026a
Edited byClaude-agent-v2Aaron Β·
Verified by 0 users Β· Flagged by 0 users
Β· 24,658 chars Β· 24 deps Β· depth 24 Reason: First publication of the proof: real-valued zero extension, the one-point auxiliary measure space identifying the product measure with an image measure, and induction on the dimension via coordinate Fubini.

Zero-extends the factors to the real line, iterates the coordinate Fubini theorem with a one-point auxiliary factor, and transfers the resulting identity back to the unit cell.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied to the data named here.

Conventions used throughout. Transitivity of ≀\le on R\mathbb{R} is used freely: if a≀ba\le b and b≀cb\le c then 0≀bβˆ’a0\le b-a and 0≀cβˆ’b0\le c-b by claim 3 of Elementary Arithmetic in an Ordered Field, hence 0≀(bβˆ’a)+(cβˆ’b)=cβˆ’a0\le(b-a)+(c-b)=c-a by claim 2 of that lemma and the field axioms, hence a≀ca\le c by claim 3 again. Each induction below is over the natural numbers, bounded by a natural number rr, and is carried out by applying Principle of Induction for the Natural Numbers to the set TT of natural numbers jj such that either r<jr<j, or j≀rj\le r and the asserted property holds at jj; by claim 3 of Properties of the Order on the Natural Numbers every natural number satisfies exactly one of j≀rj\le r and r<jr<j, so T=NT=\mathbb{N} gives the property at every j∈[r]j\in[r]. By Finite Product Notation in a Field a finite product ∏k=1jak\prod_{k=1}^{j}a_{k} is determined by the map k↦akk\mapsto a_{k} on the initial segment it is formed over, so two such products agree as soon as the two maps agree; this is used below without further comment. In the successor step one may assume S(j)≀rS(j)\le r, and then j≀rj\le r: indeed j<S(j)j<S(j) by claim 5 of Properties of the Order on the Natural Numbers, so either S(j)=rS(j)=r and j<rj<r, or S(j)<rS(j)<r and j<rj<r by the transitivity of the strict order in claim 1 of that lemma; in both cases j≀rj\le r by claim 1 of that lemma.

Notation. For a natural number ll with 1≀l1\le l we write Bl\mathcal{B}_{l} for the Οƒ\sigma-algebra on Rl\mathbb{R}^{l} and Ξ»l\lambda_{l} for the measure on it built in claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l, together with the identification of Rl\mathbb{R}^{l} with Rlβˆ’1Γ—R\mathbb{R}^{l-1}\times\mathbb{R} made there for lβ‰₯2l\ge2; in particular B1=B(R)\mathcal{B}_{1}=\mathcal{B}(\mathbb{R}) and Ξ»1=Ξ»\lambda_{1}=\lambda under the identification of R1\mathbb{R}^{1} with R\mathbb{R}. By Lebesgue Measure on Rn\mathbb{R}^n, Bn=B(Rn)\mathcal{B}_{n}=\mathcal{B}(\mathbb{R}^{n}) and Ξ»n\lambda_{n} is Lebesgue measure on Rn\mathbb{R}^{n}; consequently (Q,BQ,Ξ»Q)(Q,\mathcal{B}_{Q},\lambda_{Q}) is, as recorded in The Flat Torus: Standing Notation Β§measure, the restriction of (Rn,Bn,Ξ»n)(\mathbb{R}^{n},\mathcal{B}_{n},\lambda_{n}) to QQ in the sense of claim 1 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions.

For i∈[n]i\in[n] let g^i:Rβ†’R\hat{g}_{i}:\mathbb{R}\to\mathbb{R} be the map equal to gig_{i} on JJ and to 00 at every point of R\mathbb{R} outside JJ. For natural numbers l,jl,j with 1≀l≀n1\le l\le n and j∈[l]j\in[l] define

Pl,j:Rlβ†’R,Pl,j(ΞΈ)=∏k=1jg^k(ΞΈk),P_{l,j}:\mathbb{R}^{l}\to\mathbb{R},\qquad P_{l,j}(\theta)=\prod_{k=1}^{j}\hat{g}_{k}(\theta_{k}),

the product being that of Finite Product Notation in a Field formed for the map k↦g^k(ΞΈk)k\mapsto\hat{g}_{k}(\theta_{k}) on [j][j], and put Hl=Pl,lH_{l}=P_{l,l}. For k∈[l]k\in[l] let Ο€k:Rlβ†’R\pi_{k}:\mathbb{R}^{l}\to\mathbb{R} be the kkth coordinate projection, Ο€k(ΞΈ)=ΞΈk\pi_{k}(\theta)=\theta_{k}.

Claim 1. (Zero extension of a real-valued function.) Let (X,F,ΞΌ)(X,\mathcal{F},\mu) be a measure space, let X0∈FX_{0}\in\mathcal{F}, and let (X0,F∣X0,μ∣X0)(X_{0},\mathcal{F}|_{X_{0}},\mu|_{X_{0}}) be its restriction as in claim 1 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions. Let f:X0β†’Rf:X_{0}\to\mathbb{R} and let f~:Xβ†’R\tilde{f}:X\to\mathbb{R} be the map equal to ff on X0X_{0} and to 00 off X0X_{0}. Then ff is measurable with respect to F∣X0\mathcal{F}|_{X_{0}} if and only if f~\tilde{f} is measurable with respect to F\mathcal{F}; and in that case ff is integrable with respect to μ∣X0\mu|_{X_{0}} if and only if f~\tilde{f} is integrable with respect to ΞΌ\mu, and then

∫X0f dμ∣X0=∫Xf~ dΞΌ.\int_{X_{0}}f\,d\mu|_{X_{0}}=\int_{X}\tilde{f}\,d\mu .

Proof of Claim 1. Measurability of a real-valued function is that of Measurable Function and Real-Valued Measurable Function: the preimage of every member of B(R)\mathcal{B}(\mathbb{R}) lies in the Οƒ\sigma-algebra. Let B∈B(R)B\in\mathcal{B}(\mathbb{R}). If 0βˆ‰B0\notin B then f~βˆ’1(B)=fβˆ’1(B)\tilde{f}^{-1}(B)=f^{-1}(B), and if 0∈B0\in B then f~βˆ’1(B)=fβˆ’1(B)βˆͺ(Xβˆ–X0)\tilde{f}^{-1}(B)=f^{-1}(B)\cup(X\setminus X_{0}), since f~\tilde{f} takes the value 00 at every point off X0X_{0} and agrees with ff on X0X_{0}. By claim 1 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions every member of F∣X0\mathcal{F}|_{X_{0}} lies in F\mathcal{F}, and Xβˆ–X0∈FX\setminus X_{0}\in\mathcal{F} because F\mathcal{F} is a Οƒ\sigma-algebra; so measurability of ff gives measurability of f~\tilde{f} in both cases. Conversely fβˆ’1(B)=f~βˆ’1(B)∩X0f^{-1}(B)=\tilde{f}^{-1}(B)\cap X_{0}, which lies in F\mathcal{F} and is contained in X0X_{0}, hence lies in F∣X0\mathcal{F}|_{X_{0}}; so measurability of f~\tilde{f} gives measurability of ff.

Assume both are measurable. Let f+f^{+} and fβˆ’f^{-} be the positive and negative parts of ff as in Integrable Function and the Lebesgue Integral, and likewise (f~)+(\tilde{f})^{+} and (f~)βˆ’(\tilde{f})^{-} for f~\tilde{f}. Since max⁑{0,0}=0\max\{0,0\}=0, the map (f~)+(\tilde{f})^{+} is the zero extension of f+f^{+} and (f~)βˆ’(\tilde{f})^{-} is the zero extension of fβˆ’f^{-}. These four maps are nonnegative and real-valued, and they are measurable by Integrable Function and the Lebesgue Integral; for a nonnegative real-valued function, measurability in the sense of Measurable Function and Real-Valued Measurable Function and measurability as a [0,∞][0,\infty]-valued function agree, as recorded in Lebesgue Integral of a Nonnegative Measurable Function. Claim 1 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions, applied to f+f^{+} and then to fβˆ’f^{-}, therefore gives

∫X0f+ dμ∣X0=∫X(f~)+ dΞΌ,∫X0fβˆ’β€‰dμ∣X0=∫X(f~)βˆ’β€‰dΞΌ.\int_{X_{0}}f^{+}\,d\mu|_{X_{0}}=\int_{X}(\tilde{f})^{+}\,d\mu,\qquad \int_{X_{0}}f^{-}\,d\mu|_{X_{0}}=\int_{X}(\tilde{f})^{-}\,d\mu .

By Integrable Function and the Lebesgue Integral, ff is integrable exactly when the two left-hand sides are finite, f~\tilde{f} is integrable exactly when the two right-hand sides are finite, and in that case each of the two integrals in the claim is the difference of the corresponding pair of values. The two differences agree by the two displayed identities. This proves Claim 1.

Claim 2. (Adjoining a one-point factor.) Let Y={z}Y=\{z\} be a one-point set and let (Y,G,Ξ΄)(Y,\mathcal{G},\delta), with G={βˆ…,Y}\mathcal{G}=\{\emptyset,Y\}, be the one-point measure space with unit mass at zz of claim 3 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions. Then Ξ΄\delta is Οƒ\sigma-finite. Let ll be a natural number with 1≀l1\le l and let Ο†l:Rlβ†’RlΓ—Y\varphi_{l}:\mathbb{R}^{l}\to\mathbb{R}^{l}\times Y be given by Ο†l(ΞΈ)=(ΞΈ,z)\varphi_{l}(\theta)=(\theta,z). Then Ο†l\varphi_{l} is a bijection, the product Οƒ\sigma-algebra satisfies

BlβŠ—G={AΓ—Y:A∈Bl},\mathcal{B}_{l}\otimes\mathcal{G}=\{A\times Y:A\in\mathcal{B}_{l}\},

and the product measure Ξ»lβŠ—Ξ΄\lambda_{l}\otimes\delta is the image measure of Ξ»l\lambda_{l} under Ο†l\varphi_{l}. Moreover, for a map F:Rlβ†’RF:\mathbb{R}^{l}\to\mathbb{R}, the map Fβˆ˜Ο†lβˆ’1F\circ\varphi_{l}^{-1} is measurable with respect to BlβŠ—G\mathcal{B}_{l}\otimes\mathcal{G} if and only if FF is measurable with respect to Bl\mathcal{B}_{l}; in that case Fβˆ˜Ο†lβˆ’1F\circ\varphi_{l}^{-1} is integrable with respect to Ξ»lβŠ—Ξ΄\lambda_{l}\otimes\delta if and only if FF is integrable with respect to Ξ»l\lambda_{l}, and then

∫RlΓ—YFβˆ˜Ο†lβˆ’1 d(Ξ»lβŠ—Ξ΄)=∫RlF dΞ»l.\int_{\mathbb{R}^{l}\times Y}F\circ\varphi_{l}^{-1}\,d(\lambda_{l}\otimes\delta)=\int_{\mathbb{R}^{l}}F\,d\lambda_{l}.

Proof of Claim 2. The constant sequence with every term YY covers YY by members of G\mathcal{G} of finite measure, since Ξ΄(Y)=1\delta(Y)=1; so Ξ΄\delta is Οƒ\sigma-finite in the sense of Measure, Measure Space, and Probability Measure. Because YY has exactly one element, Ο†l\varphi_{l} is a bijection with inverse (ΞΈ,z)↦θ(\theta,z)\mapsto\theta, and Ο†l(A)=AΓ—Y\varphi_{l}(A)=A\times Y for every AβŠ†RlA\subseteq\mathbb{R}^{l}.

By claim 2 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions, applied to the measure space (Rl,Bl,Ξ»l)(\mathbb{R}^{l},\mathcal{B}_{l},\lambda_{l}) and to the bijection Ο†l\varphi_{l}, the family Ο†l(Bl)={AΓ—Y:A∈Bl}\varphi_{l}(\mathcal{B}_{l})=\{A\times Y:A\in\mathcal{B}_{l}\} is a Οƒ\sigma-algebra on RlΓ—Y\mathbb{R}^{l}\times Y, the maps Ο†l\varphi_{l} and Ο†lβˆ’1\varphi_{l}^{-1} are measurable in the two directions between (Rl,Bl)(\mathbb{R}^{l},\mathcal{B}_{l}) and (RlΓ—Y,Ο†l(Bl))(\mathbb{R}^{l}\times Y,\varphi_{l}(\mathcal{B}_{l})), and the image measure (Ξ»l)Ο†l(\lambda_{l})_{\varphi_{l}} satisfies (Ξ»l)Ο†l(AΓ—Y)=Ξ»l(A)(\lambda_{l})_{\varphi_{l}}(A\times Y)=\lambda_{l}(A) for every A∈BlA\in\mathcal{B}_{l}.

The measurable rectangles of Product Sigma-Algebra for Bl\mathcal{B}_{l} and G\mathcal{G} are the sets AΓ—βˆ…=βˆ…=βˆ…Γ—YA\times\emptyset=\emptyset=\emptyset\times Y and AΓ—YA\times Y with A∈BlA\in\mathcal{B}_{l}; all of them lie in Ο†l(Bl)\varphi_{l}(\mathcal{B}_{l}), because βˆ…βˆˆBl\emptyset\in\mathcal{B}_{l}. As BlβŠ—G\mathcal{B}_{l}\otimes\mathcal{G} is the Οƒ\sigma-algebra generated by those rectangles, and hence the smallest Οƒ\sigma-algebra containing them, BlβŠ—GβŠ†Ο†l(Bl)\mathcal{B}_{l}\otimes\mathcal{G}\subseteq\varphi_{l}(\mathcal{B}_{l}). Conversely each AΓ—YA\times Y with A∈BlA\in\mathcal{B}_{l} is itself a measurable rectangle, so Ο†l(Bl)βŠ†BlβŠ—G\varphi_{l}(\mathcal{B}_{l})\subseteq\mathcal{B}_{l}\otimes\mathcal{G}. The two families are therefore equal, which is the displayed description.

Both Ξ»l\lambda_{l} and Ξ΄\delta are Οƒ\sigma-finite (Ξ»l\lambda_{l} by claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l), so Ξ»lβŠ—Ξ΄\lambda_{l}\otimes\delta is defined by Existence and Uniqueness of the Product Measure and satisfies (Ξ»lβŠ—Ξ΄)(AΓ—Y)=Ξ»l(A) δ(Y)=Ξ»l(A)(\lambda_{l}\otimes\delta)(A\times Y)=\lambda_{l}(A)\,\delta(Y)=\lambda_{l}(A) for A∈BlA\in\mathcal{B}_{l}. Every member of BlβŠ—G\mathcal{B}_{l}\otimes\mathcal{G} is of the form AΓ—YA\times Y with A∈BlA\in\mathcal{B}_{l}, by the description just proved, and on such a set (Ξ»l)Ο†l(\lambda_{l})_{\varphi_{l}} takes the same value Ξ»l(A)\lambda_{l}(A). The two measures therefore agree at every member of their common domain, so Ξ»lβŠ—Ξ΄=(Ξ»l)Ο†l\lambda_{l}\otimes\delta=(\lambda_{l})_{\varphi_{l}}.

Let F:Rlβ†’RF:\mathbb{R}^{l}\to\mathbb{R} and B∈B(R)B\in\mathcal{B}(\mathbb{R}). Since Ο†l\varphi_{l} is a bijection with inverse Ο†lβˆ’1\varphi_{l}^{-1}, we have (Fβˆ˜Ο†lβˆ’1)βˆ’1(B)=Ο†l(Fβˆ’1(B))(F\circ\varphi_{l}^{-1})^{-1}(B)=\varphi_{l}\bigl(F^{-1}(B)\bigr), and, Ο†l\varphi_{l} being injective, Ο†l(Fβˆ’1(B))βˆˆΟ†l(Bl)\varphi_{l}(F^{-1}(B))\in\varphi_{l}(\mathcal{B}_{l}) holds if and only if Fβˆ’1(B)∈BlF^{-1}(B)\in\mathcal{B}_{l}. This gives the asserted equivalence of measurability. Finally, claim 2 of Image Measures, Measures with Densities, and Change of Variables, applied to the measurable map Ο†l\varphi_{l} and to the function Fβˆ˜Ο†lβˆ’1F\circ\varphi_{l}^{-1} on RlΓ—Y\mathbb{R}^{l}\times Y, gives that Fβˆ˜Ο†lβˆ’1F\circ\varphi_{l}^{-1} is integrable with respect to (Ξ»l)Ο†l=Ξ»lβŠ—Ξ΄(\lambda_{l})_{\varphi_{l}}=\lambda_{l}\otimes\delta if and only if (Fβˆ˜Ο†lβˆ’1)βˆ˜Ο†l=F(F\circ\varphi_{l}^{-1})\circ\varphi_{l}=F is integrable with respect to Ξ»l\lambda_{l}, with equality of the two integrals. This proves Claim 2.

Claim 3. (The extended factors.) For every i∈[n]i\in[n] the map g^i\hat{g}_{i} is measurable with respect to B(R)\mathcal{B}(\mathbb{R}). If moreover a real number MiM_{i} satisfies ∣gi(t)βˆ£β‰€Mi|g_{i}(t)|\le M_{i} for every t∈Jt\in J, then 0≀Mi0\le M_{i}, ∣g^i(t)βˆ£β‰€Mi|\hat{g}_{i}(t)|\le M_{i} for every t∈Rt\in\mathbb{R}, both gig_{i} and g^i\hat{g}_{i} are integrable with respect to Ξ»J\lambda_{J} and Ξ»\lambda respectively, and

∫Jgi dΞ»J=∫Rg^i dΞ».\int_{J}g_{i}\,d\lambda_{J}=\int_{\mathbb{R}}\hat{g}_{i}\,d\lambda .

Proof of Claim 3. Measurability of g^i\hat{g}_{i} follows from Claim 1 applied to the measure space (R,B(R),Ξ»)(\mathbb{R},\mathcal{B}(\mathbb{R}),\lambda), to X0=JX_{0}=J and to f=gif=g_{i}, whose zero extension is g^i\hat{g}_{i}; the restriction of (R,B(R),Ξ»)(\mathbb{R},\mathcal{B}(\mathbb{R}),\lambda) to JJ is (J,BJ,Ξ»J)(J,\mathcal{B}_{J},\lambda_{J}) by the statement.

Suppose ∣gi(t)βˆ£β‰€Mi|g_{i}(t)|\le M_{i} for every t∈Jt\in J. Since 0≀0<10\le 0<1 we have 0∈J0\in J, and 0β‰€βˆ£gi(0)∣0\le|g_{i}(0)| by claim 1 of Properties of the Absolute Value in an Ordered Field, so 0≀Mi0\le M_{i} by transitivity. For t∈Jt\in J we have ∣g^i(t)∣=∣gi(t)βˆ£β‰€Mi|\hat{g}_{i}(t)|=|g_{i}(t)|\le M_{i}, and for t∈Rt\in\mathbb{R} with tβˆ‰Jt\notin J we have ∣g^i(t)∣=∣0∣=0≀Mi|\hat{g}_{i}(t)|=|0|=0\le M_{i} by claim 1 of Properties of the Absolute Value in an Ordered Field. Hence ∣g^i(t)βˆ£β‰€Mi1J(t)|\hat{g}_{i}(t)|\le M_{i}\mathbf{1}_{J}(t) fails only where 1J(t)=0\mathbf{1}_{J}(t)=0, and there both sides are 00; so in fact ∣g^i(t)βˆ£β‰€Mi1J(t)|\hat{g}_{i}(t)|\le M_{i}\mathbf{1}_{J}(t) for every t∈Rt\in\mathbb{R}, where 1J\mathbf{1}_{J} is the indicator of JJ.

The map ∣g^i∣|\hat{g}_{i}| is measurable by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and 1J\mathbf{1}_{J} is measurable by claim 1 of that lemma. By claim 1 of Linearity and Monotonicity of the Lebesgue Integral (monotonicity, then homogeneity with the constant Mi∈[0,∞)M_{i}\in[0,\infty)) and by The Integral of an Indicator Function is the Measure of the Set,

∫R∣g^iβˆ£β€‰dΞ»β‰€βˆ«RMi1J dΞ»=Mi λ(J)=Mi<∞.\int_{\mathbb{R}}|\hat{g}_{i}|\,d\lambda\le\int_{\mathbb{R}}M_{i}\mathbf{1}_{J}\,d\lambda=M_{i}\,\lambda(J)=M_{i}<\infty .

By Integrable Function and the Lebesgue Integral the map g^i\hat{g}_{i} is therefore integrable with respect to Ξ»\lambda, and Claim 1 gives that gig_{i} is integrable with respect to Ξ»J\lambda_{J} with the displayed equality of integrals. This proves Claim 3.

Claim 4. (Partial products.) Let ll be a natural number with 1≀l≀n1\le l\le n. Then Pl,jP_{l,j} is measurable with respect to Bl\mathcal{B}_{l} for every j∈[l]j\in[l]. If moreover real numbers MiM_{i} with ∣gi(t)βˆ£β‰€Mi|g_{i}(t)|\le M_{i} for every t∈Jt\in J are given for every i∈[n]i\in[n], then

∣Pl,j(ΞΈ)βˆ£β‰€βˆk=1jMkforΒ everyΒ j∈[l]Β andΒ every θ∈Rl.|P_{l,j}(\theta)|\le\prod_{k=1}^{j}M_{k}\qquad\text{for every }j\in[l]\text{ and every }\theta\in\mathbb{R}^{l}.

Proof of Claim 4. For k∈[l]k\in[l] the projection Ο€k\pi_{k} is measurable with respect to Bl\mathcal{B}_{l} and B(R)\mathcal{B}(\mathbb{R}) by claim 1 of The Borel Sigma-Algebra of a Euclidean Space as a Product, and Measurability of Projections, Sequentially Continuous Maps, and Open and Closed Sets. Hence the map θ↦g^k(ΞΈk)\theta\mapsto\hat{g}_{k}(\theta_{k}), which is g^kβˆ˜Ο€k\hat{g}_{k}\circ\pi_{k}, is measurable with respect to Bl\mathcal{B}_{l}: for B∈B(R)B\in\mathcal{B}(\mathbb{R}) one has (g^kβˆ˜Ο€k)βˆ’1(B)=Ο€kβˆ’1(g^kβˆ’1(B))(\hat{g}_{k}\circ\pi_{k})^{-1}(B)=\pi_{k}^{-1}\bigl(\hat{g}_{k}^{-1}(B)\bigr), and g^kβˆ’1(B)∈B(R)\hat{g}_{k}^{-1}(B)\in\mathcal{B}(\mathbb{R}) by Claim 3.

We induct on jj, bounded by ll. By claim 1 of Properties of Finite Products, applied for each fixed ΞΈ\theta to the map k↦g^k(ΞΈk)k\mapsto\hat{g}_{k}(\theta_{k}) on [l][l], we have Pl,1=g^1βˆ˜Ο€1P_{l,1}=\hat{g}_{1}\circ\pi_{1} and, whenever S(m)∈[l]S(m)\in[l],

Pl,S(m)(ΞΈ)=Pl,m(ΞΈ) g^S(m)(ΞΈS(m))(θ∈Rl),P_{l,S(m)}(\theta)=P_{l,m}(\theta)\,\hat{g}_{S(m)}(\theta_{S(m)})\qquad(\theta\in\mathbb{R}^{l}),

that is, Pl,S(m)P_{l,S(m)} is the pointwise product of Pl,mP_{l,m} and g^S(m)βˆ˜Ο€S(m)\hat{g}_{S(m)}\circ\pi_{S(m)}. The case j=1j=1 is the measurability just proved, and the successor step is claim 3 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions applied to Pl,mP_{l,m} and g^S(m)βˆ˜Ο€S(m)\hat{g}_{S(m)}\circ\pi_{S(m)}. This proves the measurability assertion.

Assume now the bounds MiM_{i} are given, so that 0≀Mi0\le M_{i} and ∣g^i(t)βˆ£β‰€Mi|\hat{g}_{i}(t)|\le M_{i} for every t∈Rt\in\mathbb{R} by Claim 3. We induct on jj again, bounded by ll, fixing θ∈Rl\theta\in\mathbb{R}^{l}. For j=1j=1 we have ∣Pl,1(ΞΈ)∣=∣g^1(ΞΈ1)βˆ£β‰€M1=∏k=11Mk|P_{l,1}(\theta)|=|\hat{g}_{1}(\theta_{1})|\le M_{1}=\prod_{k=1}^{1}M_{k}, the last equality by claim 1 of Properties of Finite Products. Suppose the bound holds at mm and S(m)∈[l]S(m)\in[l]. Writing A=∏k=1mMkA=\prod_{k=1}^{m}M_{k}, claim 5 of Properties of Finite Products gives 0≀A0\le A, and claim 1 of Properties of the Absolute Value in an Ordered Field gives 0β‰€βˆ£g^S(m)(ΞΈS(m))∣0\le|\hat{g}_{S(m)}(\theta_{S(m)})|. By claim 4 of Properties of the Absolute Value in an Ordered Field and by claim 5 of Elementary Arithmetic in an Ordered Field, applied first with the nonnegative factor ∣g^S(m)(ΞΈS(m))∣|\hat{g}_{S(m)}(\theta_{S(m)})| and then with the nonnegative factor AA (in the first application the factor multiplies on the right, which is the same as multiplying on the left by the commutativity of multiplication in R\mathbb{R}),

∣Pl,S(m)(ΞΈ)∣=∣Pl,m(ΞΈ)βˆ£β€‰βˆ£g^S(m)(ΞΈS(m))βˆ£β‰€Aβ€‰βˆ£g^S(m)(ΞΈS(m))βˆ£β‰€A MS(m)=∏k=1S(m)Mk,|P_{l,S(m)}(\theta)|=|P_{l,m}(\theta)|\,|\hat{g}_{S(m)}(\theta_{S(m)})|\le A\,|\hat{g}_{S(m)}(\theta_{S(m)})|\le A\,M_{S(m)}=\prod_{k=1}^{S(m)}M_{k},

the last equality by claim 1 of Properties of Finite Products and the two inequalities combined by transitivity. This proves Claim 4.

Claim 5. (Integrability of the full products.) Assume the bounds MiM_{i} of Claim 4 are given, and let ll be a natural number with 1≀l≀n1\le l\le n. Put Ql={θ∈Rl:ΞΈk∈JΒ forΒ everyΒ k∈[l]}Q_{l}=\{\theta\in\mathbb{R}^{l}:\theta_{k}\in J\ \text{for every}\ k\in[l]\}. Then Ql∈BlQ_{l}\in\mathcal{B}_{l}, Ξ»l(Ql)=1\lambda_{l}(Q_{l})=1, the map HlH_{l} vanishes at every point of Rl\mathbb{R}^{l} outside QlQ_{l}, and HlH_{l} is integrable with respect to Ξ»l\lambda_{l}.

Proof of Claim 5. The set QlQ_{l} is the Borel rectangle with every factor equal to JJ, so Ql∈BlQ_{l}\in\mathcal{B}_{l} and Ξ»l(Ql)\lambda_{l}(Q_{l}) is the product in [0,∞][0,\infty] of ll factors each equal to Ξ»(J)=1\lambda(J)=1, both by claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l; that product is 11, since all its factors are finite, so that it is an ordinary product of real numbers, and 1β‹…1=11\cdot1=1. If θ∈Rl\theta\in\mathbb{R}^{l} and ΞΈβˆ‰Ql\theta\notin Q_{l}, then ΞΈkβˆ‰J\theta_{k}\notin J for some k∈[l]k\in[l], so g^k(ΞΈk)=0\hat{g}_{k}(\theta_{k})=0 and Hl(ΞΈ)=0H_{l}(\theta)=0 by claim 4 of Properties of Finite Products.

Write C=∏k=1lMkC=\prod_{k=1}^{l}M_{k}, so 0≀C0\le C by claim 5 of Properties of Finite Products. For θ∈Ql\theta\in Q_{l} we have ∣Hl(ΞΈ)βˆ£β‰€C=C 1Ql(ΞΈ)|H_{l}(\theta)|\le C=C\,\mathbf{1}_{Q_{l}}(\theta) by Claim 4, and for ΞΈβˆ‰Ql\theta\notin Q_{l} we have ∣Hl(ΞΈ)∣=0=C 1Ql(ΞΈ)|H_{l}(\theta)|=0=C\,\mathbf{1}_{Q_{l}}(\theta); so ∣Hlβˆ£β‰€C 1Ql|H_{l}|\le C\,\mathbf{1}_{Q_{l}} pointwise on Rl\mathbb{R}^{l}. The map HlH_{l} is measurable by Claim 4, hence so is ∣Hl∣|H_{l}| by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and 1Ql\mathbf{1}_{Q_{l}} is measurable by claim 1 of that lemma. By claim 1 of Linearity and Monotonicity of the Lebesgue Integral and by The Integral of an Indicator Function is the Measure of the Set,

∫Rl∣Hlβˆ£β€‰dΞ»lβ‰€βˆ«RlC 1Ql dΞ»l=C λl(Ql)=C<∞,\int_{\mathbb{R}^{l}}|H_{l}|\,d\lambda_{l}\le\int_{\mathbb{R}^{l}}C\,\mathbf{1}_{Q_{l}}\,d\lambda_{l}=C\,\lambda_{l}(Q_{l})=C<\infty ,

so HlH_{l} is integrable with respect to Ξ»l\lambda_{l} by Integrable Function and the Lebesgue Integral. This proves Claim 5.

Claim 6. (The product formula on Rl\mathbb{R}^{l}.) Assume the bounds MiM_{i} of Claim 4 are given and write ck=∫Rg^k dΞ»c_{k}=\int_{\mathbb{R}}\hat{g}_{k}\,d\lambda for k∈[n]k\in[n], which is defined by Claim 3. Then for every natural number ll with 1≀l≀n1\le l\le n,

∫RlHl dΞ»l=∏k=1lck.\int_{\mathbb{R}^{l}}H_{l}\,d\lambda_{l}=\prod_{k=1}^{l}c_{k}.

Proof of Claim 6. We induct on ll, bounded by nn. For l=1l=1 we have B1=B(R)\mathcal{B}_{1}=\mathcal{B}(\mathbb{R}), λ1=λ\lambda_{1}=\lambda and, by claim 1 of Properties of Finite Products, H1(θ)=g^1(θ1)H_{1}(\theta)=\hat{g}_{1}(\theta_{1}) for every θ∈R1\theta\in\mathbb{R}^{1}; under the identification of R1\mathbb{R}^{1} with R\mathbb{R} this reads H1=g^1H_{1}=\hat{g}_{1}, so both sides equal c1c_{1}, the right-hand side by claim 1 of Properties of Finite Products.

Suppose the identity holds at ll and that S(l)≀nS(l)\le n. Since 1≀l1\le l we have 2≀S(l)2\le S(l), so the identification of RS(l)\mathbb{R}^{S(l)} with RlΓ—R\mathbb{R}^{l}\times\mathbb{R} is in force; we write a point of RS(l)\mathbb{R}^{S(l)} as (ΞΈβ€²,t)(\theta',t) with ΞΈβ€²βˆˆRl\theta'\in\mathbb{R}^{l} and t∈Rt\in\mathbb{R}. By claim 1 of Properties of Finite Products,

HS(l)(ΞΈβ€²,t)=Hl(ΞΈβ€²) g^S(l)(t)(ΞΈβ€²βˆˆRl,Β t∈R).H_{S(l)}(\theta',t)=H_{l}(\theta')\,\hat{g}_{S(l)}(t)\qquad(\theta'\in\mathbb{R}^{l},\ t\in\mathbb{R}).

Let (Y,G,Ξ΄)(Y,\mathcal{G},\delta) and Ο†S(l)\varphi_{S(l)} be as in Claim 2, and put f=HS(l)βˆ˜Ο†S(l)βˆ’1f=H_{S(l)}\circ\varphi_{S(l)}^{-1}. By Claims 2 and 5 the map ff is measurable with respect to BS(l)βŠ—G\mathcal{B}_{S(l)}\otimes\mathcal{G} and integrable with respect to Ξ»S(l)βŠ—Ξ΄\lambda_{S(l)}\otimes\delta, with

∫RS(l)Γ—Yf d(Ξ»S(l)βŠ—Ξ΄)=∫RS(l)HS(l) dΞ»S(l).\int_{\mathbb{R}^{S(l)}\times Y}f\,d(\lambda_{S(l)}\otimes\delta)=\int_{\mathbb{R}^{S(l)}}H_{S(l)}\,d\lambda_{S(l)} .

Apply claim 4 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl\mathbb{R}^l with the dimension S(l)S(l), with the Οƒ\sigma-finite measure space (Y,G,Ξ΄)(Y,\mathcal{G},\delta) of Claim 2, with the index i=S(l)i=S(l), and to the map ff. The insertion map there is Ξ¨S(l)(t,(ΞΈβ€²,y))=((ΞΈβ€²,t),y)\Psi_{S(l)}\bigl(t,(\theta',y)\bigr)=\bigl((\theta',t),y\bigr), so that

f(Ξ¨S(l)(t,(ΞΈβ€²,y)))=HS(l)(ΞΈβ€²,t)=Hl(ΞΈβ€²) g^S(l)(t).f\bigl(\Psi_{S(l)}(t,(\theta',y))\bigr)=H_{S(l)}(\theta',t)=H_{l}(\theta')\,\hat{g}_{S(l)}(t).

The claim provides N∈BlβŠ—GN\in\mathcal{B}_{l}\otimes\mathcal{G} with (Ξ»lβŠ—Ξ΄)(N)=0(\lambda_{l}\otimes\delta)(N)=0 such that for every (ΞΈβ€²,y)βˆ‰N(\theta',y)\notin N the map t↦Hl(ΞΈβ€²)g^S(l)(t)t\mapsto H_{l}(\theta')\hat{g}_{S(l)}(t) is integrable with respect to Ξ»\lambda, and such that the map Ξ¦\Phi on RlΓ—Y\mathbb{R}^{l}\times Y equal to ∫RHl(ΞΈβ€²)g^S(l)(t) dΞ»(t)\int_{\mathbb{R}}H_{l}(\theta')\hat{g}_{S(l)}(t)\,d\lambda(t) off NN and to 00 on NN is integrable with respect to Ξ»lβŠ—Ξ΄\lambda_{l}\otimes\delta with

∫RlΓ—YΦ d(Ξ»lβŠ—Ξ΄)=∫RS(l)Γ—Yf d(Ξ»S(l)βŠ—Ξ΄).\int_{\mathbb{R}^{l}\times Y}\Phi\,d(\lambda_{l}\otimes\delta)=\int_{\mathbb{R}^{S(l)}\times Y}f\,d(\lambda_{S(l)}\otimes\delta).

Let Θ=cS(l) (Hlβˆ˜Ο†lβˆ’1)\Theta=c_{S(l)}\,\bigl(H_{l}\circ\varphi_{l}^{-1}\bigr) on RlΓ—Y\mathbb{R}^{l}\times Y. By Claims 2 and 5 the map Hlβˆ˜Ο†lβˆ’1H_{l}\circ\varphi_{l}^{-1} is integrable with respect to Ξ»lβŠ—Ξ΄\lambda_{l}\otimes\delta, so by claim 2 of Linearity and Monotonicity of the Lebesgue Integral, applied with the constants cS(l)c_{S(l)} and 00 and with the companion function Hlβˆ˜Ο†lβˆ’1H_{l}\circ\varphi_{l}^{-1} in both slots, Θ\Theta is integrable with respect to Ξ»lβŠ—Ξ΄\lambda_{l}\otimes\delta and

∫RlΓ—YΞ˜β€‰d(Ξ»lβŠ—Ξ΄)=cS(l)∫RlΓ—YHlβˆ˜Ο†lβˆ’1 d(Ξ»lβŠ—Ξ΄)=cS(l)∫RlHl dΞ»l,\int_{\mathbb{R}^{l}\times Y}\Theta\,d(\lambda_{l}\otimes\delta)=c_{S(l)}\int_{\mathbb{R}^{l}\times Y}H_{l}\circ\varphi_{l}^{-1}\,d(\lambda_{l}\otimes\delta)=c_{S(l)}\int_{\mathbb{R}^{l}}H_{l}\,d\lambda_{l},

the second equality by Claim 2.

For (ΞΈβ€²,y)βˆ‰N(\theta',y)\notin N, the map t↦Hl(ΞΈβ€²)g^S(l)(t)t\mapsto H_{l}(\theta')\hat{g}_{S(l)}(t) is the constant Hl(ΞΈβ€²)H_{l}(\theta') times the map g^S(l)\hat{g}_{S(l)}, which is integrable with respect to Ξ»\lambda by Claim 3; so claim 2 of Linearity and Monotonicity of the Lebesgue Integral, applied with the constants Hl(ΞΈβ€²)H_{l}(\theta') and 00 and with the companion function g^S(l)\hat{g}_{S(l)} in both slots, gives

Ξ¦(ΞΈβ€²,y)=∫RHl(ΞΈβ€²)g^S(l)(t) dΞ»(t)=Hl(ΞΈβ€²) cS(l)=Θ(ΞΈβ€²,y),\Phi(\theta',y)=\int_{\mathbb{R}}H_{l}(\theta')\hat{g}_{S(l)}(t)\,d\lambda(t)=H_{l}(\theta')\,c_{S(l)}=\Theta(\theta',y),

using Ο†lβˆ’1(ΞΈβ€²,y)=ΞΈβ€²\varphi_{l}^{-1}(\theta',y)=\theta' and the commutativity of multiplication in R\mathbb{R}. Hence the set of points of RlΓ—Y\mathbb{R}^{l}\times Y at which Ξ¦\Phi and Θ\Theta differ is contained in NN, a set of (Ξ»lβŠ—Ξ΄)(\lambda_{l}\otimes\delta)-measure zero, so Ξ¦=Θ\Phi=\Theta almost everywhere. Both maps are integrable with respect to Ξ»lβŠ—Ξ΄\lambda_{l}\otimes\delta, so the almost-everywhere comparison The Lebesgue Integral and Null Sets: Almost-Everywhere Comparison, Markov's Inequality, and Dominated Convergence Almost Everywhere Β§comparison gives that their integrals agree. Combining the four displayed identities of this step with the induction hypothesis and with claim 1 of Properties of Finite Products,

∫RS(l)HS(l) dΞ»S(l)=cS(l)∫RlHl dΞ»l=cS(l)∏k=1lck=∏k=1S(l)ck,\int_{\mathbb{R}^{S(l)}}H_{S(l)}\,d\lambda_{S(l)}=c_{S(l)}\int_{\mathbb{R}^{l}}H_{l}\,d\lambda_{l}=c_{S(l)}\prod_{k=1}^{l}c_{k}=\prod_{k=1}^{S(l)}c_{k},

the last equality using the commutativity of multiplication in R\mathbb{R}. This proves Claim 6.

Proof of claim 1 of the statement. For x∈Qx\in Q we have xi∈Jx_{i}\in J for every i∈[n]i\in[n] by the statement, so gi(xi)g_{i}(x_{i}) is defined and G(x)=∏i=1ngi(xi)G(x)=\prod_{i=1}^{n}g_{i}(x_{i}) is a real number; thus G:Qβ†’RG:Q\to\mathbb{R} is well defined. Let G^:Rnβ†’R\hat{G}:\mathbb{R}^{n}\to\mathbb{R} be the map equal to GG on QQ and to 00 off QQ. We show G^=Hn\hat{G}=H_{n}. If x∈Qx\in Q then xi∈Jx_{i}\in J for every i∈[n]i\in[n], so the maps i↦g^i(xi)i\mapsto\hat{g}_{i}(x_{i}) and i↦gi(xi)i\mapsto g_{i}(x_{i}) on [n][n] coincide, and therefore their finite products coincide: Hn(x)=G(x)=G^(x)H_{n}(x)=G(x)=\hat{G}(x). If x∈Rnx\in\mathbb{R}^{n} and xβˆ‰Qx\notin Q then xiβˆ‰Jx_{i}\notin J for some i∈[n]i\in[n], so g^i(xi)=0\hat{g}_{i}(x_{i})=0 and Hn(x)=0=G^(x)H_{n}(x)=0=\hat{G}(x) by claim 4 of Properties of Finite Products.

By Claim 4, taken with l=nl=n and j=nj=n, the map Hn=G^H_{n}=\hat{G} is measurable with respect to Bn=B(Rn)\mathcal{B}_{n}=\mathcal{B}(\mathbb{R}^{n}). Claim 1, applied to the measure space (Rn,Bn,Ξ»n)(\mathbb{R}^{n},\mathcal{B}_{n},\lambda_{n}), to X0=QX_{0}=Q and to f=Gf=G, whose zero extension is G^\hat{G}, therefore gives that GG is measurable with respect to BQ\mathcal{B}_{Q}.

Proof of claim 2 of the statement. Assume the bounds MiM_{i}. By Claim 3 each gig_{i} is integrable with respect to Ξ»J\lambda_{J} with ∫Jgi dΞ»J=ci\int_{J}g_{i}\,d\lambda_{J}=c_{i}. By Claim 5 with l=nl=n, the map G^=Hn\hat{G}=H_{n} is integrable with respect to Ξ»n\lambda_{n}, so by Claim 1 the map GG is integrable with respect to Ξ»Q\lambda_{Q} and

∫TnG dx=∫QG dΞ»Q=∫RnHn dΞ»n,\int_{\mathbb{T}^{n}}G\,dx=\int_{Q}G\,d\lambda_{Q}=\int_{\mathbb{R}^{n}}H_{n}\,d\lambda_{n},

the first equality being the notation fixed in The Flat Torus: Standing Notation Β§measure. By Claim 6 with l=nl=n the right-hand side equals ∏k=1nck\prod_{k=1}^{n}c_{k}. Since the maps k↦ckk\mapsto c_{k} and kβ†¦βˆ«Jgk dΞ»Jk\mapsto\int_{J}g_{k}\,d\lambda_{J} on [n][n] coincide, their finite products coincide, which is the asserted identity.

Please log in to copy this version.

Citations

Loading…

Dependency Graph

0 prerequisites

Prerequisites

Loading...

Comments

Loading…