Each result cited is universally quantified over the data in its own statement. The exponent of Continuous Periodic Functions are Power-Integrable and Dense on the Torus is taken to be p=2 throughout, and ΞΉ denotes the canonical map from N to R.
An enumeration of the index set. The set [2N+1]n is nonempty and finite by claim 3 of Finiteness of Cartesian Products, Tuple Sets, and Permutation Sets, as recorded in The Reproducing Identity for the Fejer Kernels of the Torus; being nonempty and finite, it has M elements for some MβN, unique by Uniqueness of the Number of Elements, and there is a bijection Ο:[M]β[2N+1]n. Fix one. By Sum over a Finite Index Set, for every map f:[2N+1]nβR,
aβ[2N+1]nββf(a)=j=1βMβf(Ο(j)).
For jβ[M] write kjβ=k(Ο(j))βZn, Wjβ=WN,Ο(j)β and u^jβ=β¨[uβ£Qβ],Ekjβββ©L2β. Applying the display to the map aβ¦WN,aββ¨[uβ£Qβ],Ek(a)ββ©L2βek(a)β(x) for each fixed x gives
ΟNβu(x)=j=1βMβ(Wjβu^jβ)ekjββ(x)(xβRn),
and each ekjββ lies in Cperβ by The Trigonometric System on the Torus is Orthonormal Β§classes.
Claim 1. By the last display, ΟNβu is the map of Finite Linear Combinations of Continuous Periodic Functions and Their Classes on the Torus formed with the coefficients cjβ=Wjβu^jβ and the maps gjβ=ekjββ, so ΟNβuβCperβ by Finite Linear Combinations of Continuous Periodic Functions and Their Classes on the Torus Β§member.
Claim 2. Let UβL2(Tn). With the same data, Finite Linear Combinations of Continuous Periodic Functions and Their Classes on the Torus Β§pairing gives
β¨U,[(ΟNβu)β£Qβ]β©L2β=j=1βMβWjβu^jββ¨U,Ekjβββ©L2β,
since [ekjβββ£Qβ]=Ekjββ. By the first display, applied to the map aβ¦WN,aββ¨[uβ£Qβ],Ek(a)ββ©L2ββ¨U,Ek(a)ββ©L2β, the right-hand side is the sum over [2N+1]n asserted in claim 2.
Claim 3. Fix xβRn and let yβRn. By The Reproducing Identity for the Fejer Kernels of the Torus Β§product, applied to the pair of points y,x, and the first display,
Ξ¦Nβ(yβx)=aβ[2N+1]nββWN,aβek(a)β(y)ek(a)β(x)=j=1βMβWjβekjββ(y)ekjββ(x).
Multiplying by the real number 1Qβ(y)u(y) and moving it inside the sum by the homogeneity of finite sums, claim 3 of Properties of Finite Sums, then rearranging each summand by the commutativity and associativity of multiplication, gives
1Qβ(y)Ξ¦Nβ(yβx)u(y)=j=1βMβΞ²jβhjβ(y),Ξ²jβ=Wjβekjββ(x),hjβ=1Qβekjββu,
where hjβ:RnβR is the pointwise product. For each jβ[M] the map ekjββu lies in Cperβ by Elementary Properties of Lattice-Periodic Functions Β§algebra, so by Continuous Periodic Functions are Power-Integrable and Dense on the Torus Β§integral the map hjβ=1Qβ(ekjββu) is measurable and integrable, and
β«RnβhjβdΞ»nβ=β«Tnβ(ekjββu)β£Qβdx.
The restriction (ekjββu)β£Qβ is the pointwise product of ekjβββ£Qβ and uβ£Qβ, both of which lie in L2(Tn) by Continuous Periodic Functions are Power-Integrable and Dense on the Torus Β§member; so by The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space Β§inner-product the right-hand side equals β¨Ekjββ,[uβ£Qβ]β©L2β, which is u^jβ by the symmetry of the inner product, condition (a) of Real Inner Product Space Β§inner-product. Now Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions, applied to the integrable maps hjβ and the coefficients Ξ²jβ, shows by its clause Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions Β§integrable that yβ¦1Qβ(y)Ξ¦Nβ(yβx)u(y) is measurable and integrable, and by Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions Β§linear that
β«Rnβ1Qβ(y)Ξ¦Nβ(yβx)u(y)dΞ»nβ(y)=j=1βMβΞ²jβu^jβ=j=1βMβ(Wjβu^jβ)ekjββ(x)=ΟNβu(x),
the middle equality by commutativity of multiplication and the last by the second display.
Claim 4. Let 0 denote the origin of Rn, all of whose coordinates are 0; it lies in Zn by Lattice-Periodic Functions and the Periodic Function Classes Β§lattice, since 0βZ by claim 2 of Arithmetic, Order and Discreteness of the Integers. By The Trigonometric System on the Torus Β§one-dimensional and The Trigonometric System on the Torus Β§system, e0β(y)=βi=1nβΟ0β(yiβ)=βi=1nβ1=1 for every yβRn, the last step by claim 3 of Properties of Finite Products applied with i=1 there, every factor other than the first being 1. Also e0ββCperβ by The Trigonometric System on the Torus is Orthonormal Β§classes.
Fix xβRn and apply claim 3 to u=e0β: the map yβ¦1Qβ(y)Ξ¦Nβ(yβx)e0β(y), which is yβ¦1Qβ(y)Ξ¦Nβ(yβx) because e0β(y)=1, is measurable and integrable, and its integral equals ΟNβe0β(x). It remains to show ΟNβe0β(x)=1.
Let a0β[2N+1]n be the tuple with ai0β=N+1 for every iβ[n]; here N+1β[2N+1] because N+1<(N+1)+N=N+(N+1)=2N+1 by claim 6 of Properties of the Order on the Natural Numbers and claim 4 of Arithmetic of Addition on the Natural Numbers, hence N+1β€2N+1 by claim 1 of the former. The summands of ΟNβe0β(x) involve β¨[e0ββ£Qβ],Ek(a)ββ©L2β=β¨E0β,Ek(a)ββ©L2β, since E0β=[e0ββ£Qβ] by The Trigonometric System on the Torus is Orthonormal Β§classes. For aβ[2N+1]n, by The Trigonometric System on the Torus is Orthonormal Β§orthonormal the number β¨E0β,Ek(a)ββ©L2β equals 1 if k(a)=0 and 0 otherwise. Now k(a)=0 holds exactly when k(a)iβ=0, that is ΞΉ(aiβ)=ΞΉ(N)+1=ΞΉ(N+1), for every iβ[n], by claim 1 of Euclidean Points as Tuples of Real Numbers and claim 1 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field; by the injectivity of ΞΉ, claim 7 of that lemma, this holds exactly when aiβ=N+1 for every iβ[n], that is, exactly when a=a0, two maps on [n] being equal when their values agree everywhere. Hence the summand WN,aββ¨E0β,Ek(a)ββ©L2βek(a)β(x) of ΟNβe0β(x) vanishes for every aξ =a0, and claims 4 and 1 of Peeling, Splitting, and Interchange for Sums over a Finite Index Set, applied with E={a0}, give
ΟNβe0β(x)=WN,a0ββ¨E0β,E0ββ©L2βe0β(x)=WN,a0β.
Finally, the integer attached to ai0β=N+1 in The Reproducing Identity for the Fejer Kernels of the Torus is ΞΉ(N+1)βΞΉ(N)β1=0, so wN,N+1β=1βNβ£0β£β=1 by Absolute Value in an Ordered Field, and WN,a0β=βi=1nβ1=1 by claim 3 of Properties of Finite Products as above. This proves claim 4.