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 β€ on R is used freely: if aβ€b and bβ€c then 0β€bβa and 0β€cβb by claim 3 of Elementary Arithmetic in an Ordered Field, hence 0β€(bβa)+(cβb)=cβa by claim 2 of that lemma and the field axioms, hence aβ€c by claim 3 again. Each induction below is over the natural numbers, bounded by a natural number r, and is carried out by applying Principle of Induction for the Natural Numbers to the set T of natural numbers j such that either r<j, or jβ€r and the asserted property holds at j; by claim 3 of Properties of the Order on the Natural Numbers every natural number satisfies exactly one of jβ€r and r<j, so T=N gives the property at every jβ[r]. By Finite Product Notation in a Field a finite product βk=1jβakβ is determined by the map kβ¦akβ 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)β€r, and then jβ€r: indeed j<S(j) by claim 5 of Properties of the Order on the Natural Numbers, so either S(j)=r and j<r, or S(j)<r and j<r by the transitivity of the strict order in claim 1 of that lemma; in both cases jβ€r by claim 1 of that lemma.
Notation. For a natural number l with 1β€l we write Blβ for the Ο-algebra on Rl and Ξ»lβ for the measure on it built in claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl, together with the identification of Rl with Rlβ1ΓR made there for lβ₯2; in particular B1β=B(R) and Ξ»1β=Ξ» under the identification of R1 with R. By Lebesgue Measure on Rn, Bnβ=B(Rn) and Ξ»nβ is Lebesgue measure on Rn; consequently (Q,BQβ,Ξ»Qβ) is, as recorded in The Flat Torus: Standing Notation Β§measure, the restriction of (Rn,Bnβ,Ξ»nβ) to Q in the sense of claim 1 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions.
For iβ[n] let g^βiβ:RβR be the map equal to giβ on J and to 0 at every point of R outside J. For natural numbers l,j with 1β€lβ€n and jβ[l] define
Pl,jβ:RlβR,Pl,jβ(ΞΈ)=k=1βjβg^βkβ(ΞΈkβ),
the product being that of Finite Product Notation in a Field formed for the map kβ¦g^βkβ(ΞΈkβ) on [j], and put Hlβ=Pl,lβ. For kβ[l] let Οkβ:RlβR be the kth coordinate projection, Οkβ(ΞΈ)=ΞΈkβ.
Claim 1. (Zero extension of a real-valued function.) Let (X,F,ΞΌ) be a measure space, let X0ββF, and let (X0β,Fβ£X0ββ,ΞΌβ£X0ββ) be its restriction as in claim 1 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions. Let f:X0ββR and let f~β:XβR be the map equal to f on X0β and to 0 off X0β. Then f is measurable with respect to Fβ£X0ββ if and only if f~β is measurable with respect to F; and in that case f is integrable with respect to ΞΌβ£X0ββ if and only if f~β is integrable with respect to ΞΌ, and then
β«X0ββfdΞΌβ£X0ββ=β«Xβf~βdΞΌ.
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) lies in the Ο-algebra. Let BβB(R). If 0β/B then f~ββ1(B)=fβ1(B), and if 0βB then f~ββ1(B)=fβ1(B)βͺ(XβX0β), since f~β takes the value 0 at every point off X0β and agrees with f on X0β. By claim 1 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions every member of Fβ£X0ββ lies in F, and XβX0ββF because F is a Ο-algebra; so measurability of f gives measurability of f~β in both cases. Conversely fβ1(B)=f~ββ1(B)β©X0β, which lies in F and is contained in X0β, hence lies in Fβ£X0ββ; so measurability of f~β gives measurability of f.
Assume both are measurable. Let f+ and fβ be the positive and negative parts of f as in Integrable Function and the Lebesgue Integral, and likewise (f~β)+ and (f~β)β for f~β. Since max{0,0}=0, the map (f~β)+ is the zero extension of f+ and (f~β)β is the zero extension of fβ. 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,β]-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+ and then to fβ, therefore gives
β«X0ββf+dΞΌβ£X0ββ=β«Xβ(f~β)+dΞΌ,β«X0ββfβdΞΌβ£X0ββ=β«Xβ(f~β)βdΞΌ.
By Integrable Function and the Lebesgue Integral, f is integrable exactly when the two left-hand sides are finite, f~β 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} be a one-point set and let (Y,G,Ξ΄), with G={β
,Y}, be the one-point measure space with unit mass at z of claim 3 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions. Then Ξ΄ is Ο-finite. Let l be a natural number with 1β€l and let Οlβ:RlβRlΓY be given by Οlβ(ΞΈ)=(ΞΈ,z). Then Οlβ is a bijection, the product Ο-algebra satisfies
BlββG={AΓY:AβBlβ},
and the product measure Ξ»lββΞ΄ is the image measure of Ξ»lβ under Οlβ. Moreover, for a map F:RlβR, the map FβΟlβ1β is measurable with respect to BlββG if and only if F is measurable with respect to Blβ; in that case FβΟlβ1β is integrable with respect to Ξ»lββΞ΄ if and only if F is integrable with respect to Ξ»lβ, and then
β«RlΓYβFβΟlβ1βd(Ξ»lββΞ΄)=β«RlβFdΞ»lβ.
Proof of Claim 2. The constant sequence with every term Y covers Y by members of G of finite measure, since Ξ΄(Y)=1; so Ξ΄ is Ο-finite in the sense of Measure, Measure Space, and Probability Measure. Because Y has exactly one element, Οlβ is a bijection with inverse (ΞΈ,z)β¦ΞΈ, and Οlβ(A)=AΓY for every AβRl.
By claim 2 of Assembly of Measure Spaces: Restriction, Transport, One-Point Spaces, and Countable Disjoint Unions, applied to the measure space (Rl,Blβ,Ξ»lβ) and to the bijection Οlβ, the family Οlβ(Blβ)={AΓY:AβBlβ} is a Ο-algebra on RlΓY, the maps Οlβ and Οlβ1β are measurable in the two directions between (Rl,Blβ) and (RlΓY,Οlβ(Blβ)), and the image measure (Ξ»lβ)Οlββ satisfies (Ξ»lβ)Οlββ(AΓY)=Ξ»lβ(A) for every AβBlβ.
The measurable rectangles of Product Sigma-Algebra for Blβ and G are the sets AΓβ
=β
=β
ΓY and AΓY with AβBlβ; all of them lie in Οlβ(Blβ), because β
βBlβ. As BlββG is the Ο-algebra generated by those rectangles, and hence the smallest Ο-algebra containing them, BlββGβΟlβ(Blβ). Conversely each AΓY with AβBlβ is itself a measurable rectangle, so Οlβ(Blβ)βBlββG. The two families are therefore equal, which is the displayed description.
Both Ξ»lβ and Ξ΄ are Ο-finite (Ξ»lβ by claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl), so Ξ»lββΞ΄ is defined by Existence and Uniqueness of the Product Measure and satisfies (Ξ»lββΞ΄)(AΓY)=Ξ»lβ(A)Ξ΄(Y)=Ξ»lβ(A) for AβBlβ. Every member of BlββG is of the form AΓY with AβBlβ, by the description just proved, and on such a set (Ξ»lβ)Οlββ takes the same value Ξ»lβ(A). The two measures therefore agree at every member of their common domain, so Ξ»lββΞ΄=(Ξ»lβ)Οlββ.
Let F:RlβR and BβB(R). Since Οlβ is a bijection with inverse Οlβ1β, we have (FβΟlβ1β)β1(B)=Οlβ(Fβ1(B)), and, Οlβ being injective, Οlβ(Fβ1(B))βΟlβ(Blβ) holds if and only if Fβ1(B)βBlβ. 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 Οlβ and to the function FβΟlβ1β on RlΓY, gives that FβΟlβ1β is integrable with respect to (Ξ»lβ)Οlββ=Ξ»lββΞ΄ if and only if (FβΟlβ1β)βΟlβ=F is integrable with respect to Ξ»lβ, with equality of the two integrals. This proves Claim 2.
Claim 3. (The extended factors.) For every iβ[n] the map g^βiβ is measurable with respect to B(R). If moreover a real number Miβ satisfies β£giβ(t)β£β€Miβ for every tβJ, then 0β€Miβ, β£g^βiβ(t)β£β€Miβ for every tβR, both giβ and g^βiβ are integrable with respect to Ξ»Jβ and Ξ» respectively, and
β«JβgiβdΞ»Jβ=β«Rβg^βiβdΞ».
Proof of Claim 3. Measurability of g^βiβ follows from Claim 1 applied to the measure space (R,B(R),Ξ»), to X0β=J and to f=giβ, whose zero extension is g^βiβ; the restriction of (R,B(R),Ξ») to J is (J,BJβ,Ξ»Jβ) by the statement.
Suppose β£giβ(t)β£β€Miβ for every tβJ. Since 0β€0<1 we have 0βJ, and 0β€β£giβ(0)β£ by claim 1 of Properties of the Absolute Value in an Ordered Field, so 0β€Miβ by transitivity. For tβJ we have β£g^βiβ(t)β£=β£giβ(t)β£β€Miβ, and for tβR with tβ/J we have β£g^βiβ(t)β£=β£0β£=0β€Miβ by claim 1 of Properties of the Absolute Value in an Ordered Field. Hence β£g^βiβ(t)β£β€Miβ1Jβ(t) fails only where 1Jβ(t)=0, and there both sides are 0; so in fact β£g^βiβ(t)β£β€Miβ1Jβ(t) for every tβR, where 1Jβ is the indicator of J.
The map β£g^βiββ£ is measurable by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and 1Jβ 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 Miββ[0,β)) and by The Integral of an Indicator Function is the Measure of the Set,
β«Rββ£g^βiββ£dΞ»β€β«RβMiβ1JβdΞ»=MiβΞ»(J)=Miβ<β.
By Integrable Function and the Lebesgue Integral the map g^βiβ is therefore integrable with respect to Ξ», and Claim 1 gives that giβ is integrable with respect to Ξ»Jβ with the displayed equality of integrals. This proves Claim 3.
Claim 4. (Partial products.) Let l be a natural number with 1β€lβ€n. Then Pl,jβ is measurable with respect to Blβ for every jβ[l]. If moreover real numbers Miβ with β£giβ(t)β£β€Miβ for every tβJ are given for every iβ[n], then
β£Pl,jβ(ΞΈ)β£β€k=1βjβMkβforΒ everyΒ jβ[l]Β andΒ everyΒ ΞΈβRl.
Proof of Claim 4. For kβ[l] the projection Οkβ is measurable with respect to Blβ and B(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 ΞΈβ¦g^βkβ(ΞΈkβ), which is g^βkββΟkβ, is measurable with respect to Blβ: for BβB(R) one has (g^βkββΟkβ)β1(B)=Οkβ1β(g^βkβ1β(B)), and g^βkβ1β(B)βB(R) by Claim 3.
We induct on j, bounded by l. By claim 1 of Properties of Finite Products, applied for each fixed ΞΈ to the map kβ¦g^βkβ(ΞΈkβ) on [l], we have Pl,1β=g^β1ββΟ1β and, whenever S(m)β[l],
Pl,S(m)β(ΞΈ)=Pl,mβ(ΞΈ)g^βS(m)β(ΞΈS(m)β)(ΞΈβRl),
that is, Pl,S(m)β is the pointwise product of Pl,mβ and g^βS(m)ββΟS(m)β. The case j=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,mβ and g^βS(m)ββΟS(m)β. This proves the measurability assertion.
Assume now the bounds Miβ are given, so that 0β€Miβ and β£g^βiβ(t)β£β€Miβ for every tβR by Claim 3. We induct on j again, bounded by l, fixing ΞΈβRl. For j=1 we have β£Pl,1β(ΞΈ)β£=β£g^β1β(ΞΈ1β)β£β€M1β=βk=11βMkβ, the last equality by claim 1 of Properties of Finite Products. Suppose the bound holds at m and S(m)β[l]. Writing A=βk=1mβMkβ, claim 5 of Properties of Finite Products gives 0β€A, and claim 1 of Properties of the Absolute Value in an Ordered Field gives 0β€β£g^βS(m)β(ΞΈS(m)β)β£. 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 β£g^βS(m)β(ΞΈS(m)β)β£ and then with the nonnegative factor A (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),
β£Pl,S(m)β(ΞΈ)β£=β£Pl,mβ(ΞΈ)β£β£g^βS(m)β(ΞΈS(m)β)β£β€Aβ£g^βS(m)β(ΞΈS(m)β)β£β€AMS(m)β=k=1βS(m)βMkβ,
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 Miβ of Claim 4 are given, and let l be a natural number with 1β€lβ€n. Put Qlβ={ΞΈβRl:ΞΈkββJΒ forΒ everyΒ kβ[l]}. Then QlββBlβ, Ξ»lβ(Qlβ)=1, the map Hlβ vanishes at every point of Rl outside Qlβ, and Hlβ is integrable with respect to Ξ»lβ.
Proof of Claim 5. The set Qlβ is the Borel rectangle with every factor equal to J, so QlββBlβ and Ξ»lβ(Qlβ) is the product in [0,β] of l factors each equal to Ξ»(J)=1, both by claim 1 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl; that product is 1, since all its factors are finite, so that it is an ordinary product of real numbers, and 1β
1=1. If ΞΈβRl and ΞΈβ/Qlβ, then ΞΈkββ/J for some kβ[l], so g^βkβ(ΞΈkβ)=0 and Hlβ(ΞΈ)=0 by claim 4 of Properties of Finite Products.
Write C=βk=1lβMkβ, so 0β€C by claim 5 of Properties of Finite Products. For ΞΈβQlβ we have β£Hlβ(ΞΈ)β£β€C=C1Qlββ(ΞΈ) by Claim 4, and for ΞΈβ/Qlβ we have β£Hlβ(ΞΈ)β£=0=C1Qlββ(ΞΈ); so β£Hlββ£β€C1Qlββ pointwise on Rl. The map Hlβ is measurable by Claim 4, hence so is β£Hlββ£ by claim 4 of Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions, and 1Qlββ 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,
β«Rlββ£Hlββ£dΞ»lββ€β«RlβC1QlββdΞ»lβ=CΞ»lβ(Qlβ)=C<β,
so Hlβ is integrable with respect to Ξ»lβ by Integrable Function and the Lebesgue Integral. This proves Claim 5.
Claim 6. (The product formula on Rl.) Assume the bounds Miβ of Claim 4 are given and write ckβ=β«Rβg^βkβdΞ» for kβ[n], which is defined by Claim 3. Then for every natural number l with 1β€lβ€n,
β«RlβHlβdΞ»lβ=k=1βlβckβ.
Proof of Claim 6. We induct on l, bounded by n. For l=1 we have B1β=B(R), Ξ»1β=Ξ» and, by claim 1 of Properties of Finite Products, H1β(ΞΈ)=g^β1β(ΞΈ1β) for every ΞΈβR1; under the identification of R1 with R this reads H1β=g^β1β, so both sides equal c1β, the right-hand side by claim 1 of Properties of Finite Products.
Suppose the identity holds at l and that S(l)β€n. Since 1β€l we have 2β€S(l), so the identification of RS(l) with RlΓR is in force; we write a point of RS(l) as (ΞΈβ²,t) with ΞΈβ²βRl and tβR. By claim 1 of Properties of Finite Products,
HS(l)β(ΞΈβ²,t)=Hlβ(ΞΈβ²)g^βS(l)β(t)(ΞΈβ²βRl,Β tβR).
Let (Y,G,Ξ΄) and ΟS(l)β be as in Claim 2, and put f=HS(l)ββΟS(l)β1β. By Claims 2 and 5 the map f is measurable with respect to BS(l)ββG and integrable with respect to Ξ»S(l)ββΞ΄, with
β«RS(l)ΓYβfd(Ξ»S(l)ββΞ΄)=β«RS(l)βHS(l)βdΞ»S(l)β.
Apply claim 4 of Finite Products of Lebesgue Measure and Coordinate Integration on Rl with the dimension S(l), with the Ο-finite measure space (Y,G,Ξ΄) of Claim 2, with the index i=S(l), and to the map f. The insertion map there is Ξ¨S(l)β(t,(ΞΈβ²,y))=((ΞΈβ²,t),y), so that
f(Ξ¨S(l)β(t,(ΞΈβ²,y)))=HS(l)β(ΞΈβ²,t)=Hlβ(ΞΈβ²)g^βS(l)β(t).
The claim provides NβBlββG with (Ξ»lββΞ΄)(N)=0 such that for every (ΞΈβ²,y)β/N the map tβ¦Hlβ(ΞΈβ²)g^βS(l)β(t) is integrable with respect to Ξ», and such that the map Ξ¦ on RlΓY equal to β«RβHlβ(ΞΈβ²)g^βS(l)β(t)dΞ»(t) off N and to 0 on N is integrable with respect to Ξ»lββΞ΄ with
β«RlΓYβΞ¦d(Ξ»lββΞ΄)=β«RS(l)ΓYβfd(Ξ»S(l)ββΞ΄).
Let Ξ=cS(l)β(HlββΟlβ1β) on RlΓY. By Claims 2 and 5 the map HlββΟlβ1β is integrable with respect to Ξ»lββΞ΄, so by claim 2 of Linearity and Monotonicity of the Lebesgue Integral, applied with the constants cS(l)β and 0 and with the companion function HlββΟlβ1β in both slots, Ξ is integrable with respect to Ξ»lββΞ΄ and
β«RlΓYβΞd(Ξ»lββΞ΄)=cS(l)ββ«RlΓYβHlββΟlβ1βd(Ξ»lββΞ΄)=cS(l)ββ«RlβHlβdΞ»lβ,
the second equality by Claim 2.
For (ΞΈβ²,y)β/N, the map tβ¦Hlβ(ΞΈβ²)g^βS(l)β(t) is the constant Hlβ(ΞΈβ²) times the map g^βS(l)β, which is integrable with respect to Ξ» by Claim 3; so claim 2 of Linearity and Monotonicity of the Lebesgue Integral, applied with the constants Hlβ(ΞΈβ²) and 0 and with the companion function g^βS(l)β in both slots, gives
Ξ¦(ΞΈβ²,y)=β«RβHlβ(ΞΈβ²)g^βS(l)β(t)dΞ»(t)=Hlβ(ΞΈβ²)cS(l)β=Ξ(ΞΈβ²,y),
using Οlβ1β(ΞΈβ²,y)=ΞΈβ² and the commutativity of multiplication in R. Hence the set of points of RlΓY at which Ξ¦ and Ξ differ is contained in N, a set of (Ξ»lββΞ΄)-measure zero, so Ξ¦=Ξ almost everywhere. Both maps are integrable with respect to Ξ»lββΞ΄, 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,
β«RS(l)βHS(l)βdΞ»S(l)β=cS(l)ββ«RlβHlβdΞ»lβ=cS(l)βk=1βlβckβ=k=1βS(l)βckβ,
the last equality using the commutativity of multiplication in R. This proves Claim 6.
Proof of claim 1 of the statement. For xβQ we have xiββJ for every iβ[n] by the statement, so giβ(xiβ) is defined and G(x)=βi=1nβgiβ(xiβ) is a real number; thus G:QβR is well defined. Let G^:RnβR be the map equal to G on Q and to 0 off Q. We show G^=Hnβ. If xβQ then xiββJ for every iβ[n], so the maps iβ¦g^βiβ(xiβ) and iβ¦giβ(xiβ) on [n] coincide, and therefore their finite products coincide: Hnβ(x)=G(x)=G^(x). If xβRn and xβ/Q then xiββ/J for some iβ[n], so g^βiβ(xiβ)=0 and Hnβ(x)=0=G^(x) by claim 4 of Properties of Finite Products.
By Claim 4, taken with l=n and j=n, the map Hnβ=G^ is measurable with respect to Bnβ=B(Rn). Claim 1, applied to the measure space (Rn,Bnβ,Ξ»nβ), to X0β=Q and to f=G, whose zero extension is G^, therefore gives that G is measurable with respect to BQβ.
Proof of claim 2 of the statement. Assume the bounds Miβ. By Claim 3 each giβ is integrable with respect to Ξ»Jβ with β«JβgiβdΞ»Jβ=ciβ. By Claim 5 with l=n, the map G^=Hnβ is integrable with respect to Ξ»nβ, so by Claim 1 the map G is integrable with respect to Ξ»Qβ and
β«TnβGdx=β«QβGdΞ»Qβ=β«RnβHnβdΞ»nβ,
the first equality being the notation fixed in The Flat Torus: Standing Notation Β§measure. By Claim 6 with l=n the right-hand side equals βk=1nβckβ. Since the maps kβ¦ckβ and kβ¦β«JβgkβdΞ»Jβ on [n] coincide, their finite products coincide, which is the asserted identity.