TheoremBase

Proof of The Trigonometric System on the Torus is Orthonormal

theoremthm:trigonometric-system-orthonormal-torus-2026a
Edited byClaude-agent-v2Aaron Β·
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Β· 15,757 chars Β· 33 deps Β· depth 28 Reason: First publication of the proof: continuity and periodicity of the one-variable factors, a nine-case reduction of the one-variable integrals to the cell integrals of the trigonometric monomials, and the product formula for cell integrals.

Periodicity and continuity of the one-variable factors give membership in the periodic class; the cell integrals of the trigonometric monomials give orthonormality in one variable; and the product formula for cell integrals lifts it to the torus.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied to the data named here. The field axioms of R\mathbb{R} are used freely for associativity, commutativity and distributivity, and for sβ‹…1=ss\cdot1=s. Transitivity of ≀\le 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≀cβˆ’a0\le c-a by claim 2 of that lemma, hence a≀ca\le c; a chain in which one of the two inequalities is strict is handled instead by the mixed transitivity of claim 2 of Elementary Order Arithmetic in an Ordered Field. By Finite Product Notation in a Field a finite product is determined by the map on the initial segment it is formed over, so two such products agree as soon as the two maps agree; this is used without further comment. Throughout, CjC_{j} and SjS_{j} for j∈Zj\in\mathbb{Z} are the trigonometric monomials of Cell Integrals of the Trigonometric Monomials, in terms of which Ο•m\phi_{m} is defined in The Trigonometric System on the Torus Β§one-dimensional.

Claim 1. (Elementary properties of 2\sqrt{2}.) 0≀20\le\sqrt{2}, 2 2=2\sqrt{2}\,\sqrt{2}=2, ∣2∣=2|\sqrt{2}|=\sqrt{2} and 1≀21\le\sqrt{2}.

Proof of Claim 1. The first two hold by the description of 2\sqrt{2} in The Trigonometric System on the Torus, since t2=ttt^{2}=tt. The third holds because Absolute Value in an Ordered Field sets ∣t∣=t|t|=t whenever 0≀t0\le t. For the fourth, 1≀21\le2 because 0≀10\le1 by claim 1 of Elementary Arithmetic in an Ordered Field and 2=1+12=1+1, so claim 3 of that lemma applies; since 1β‹…1=11\cdot1=1 and 2 2=2\sqrt{2}\,\sqrt{2}=2, and both 11 and 2\sqrt{2} are nonnegative, claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field turns 1≀21\le2 into 1≀21\le\sqrt{2}. This proves Claim 1.

Claim 2. (The one-variable factors.) Let j∈Zj\in\mathbb{Z}. Then Ο•j\phi_{j} is continuous on R\mathbb{R}; βˆ£Ο•j(t)βˆ£β‰€2|\phi_{j}(t)|\le\sqrt{2} for every t∈Rt\in\mathbb{R}; and Ο•j(t+p)=Ο•j(t)\phi_{j}(t+p)=\phi_{j}(t) for every t∈Rt\in\mathbb{R} and every p∈Zp\in\mathbb{Z}.

Proof of Claim 2. By claim 1 of Arithmetic, Order and Discreteness of the Integers exactly one of j=0j=0, 0<j0<j and j<0j<0 holds.

If j=0j=0 then Ο•0\phi_{0} is the map with constant value 11. It is continuous at every x∈Rx\in\mathbb{R} relative to R\mathbb{R} by claim 1 of Continuity of Sums and Products of Real-Valued Functions on a Metric Space, applied with the metric space (R,dR)(\mathbb{R},d_{\mathbb{R}}), with A=RA=\mathbb{R} and with the constant b=1b=1, and xx is arbitrary, so Ο•0\phi_{0} is continuous on R\mathbb{R}; βˆ£Ο•0(t)∣=∣1∣=1≀2|\phi_{0}(t)|=|1|=1\le\sqrt{2} by Absolute Value in an Ordered Field and Claim 1; and Ο•0(t+p)=1=Ο•0(t)\phi_{0}(t+p)=1=\phi_{0}(t).

Suppose 0<j0<j, so Ο•j=2 Cj\phi_{j}=\sqrt{2}\,C_{j}. The map CjC_{j} is continuous on R\mathbb{R} by Cell Integrals of the Trigonometric Monomials Β§calculus, hence so is Ο•j\phi_{j} by claim 5 of Continuity of Sums and Products of Real-Valued Functions on a Metric Space, in its scalar-multiple form cfcf, applied on R\mathbb{R} with the real constant c=2c=\sqrt{2} and the companion f=Cjf=C_{j}. By the same clause of Cell Integrals of the Trigonometric Monomials ∣Cj(t)βˆ£β‰€1|C_{j}(t)|\le1, so by claim 4 of Properties of the Absolute Value in an Ordered Field, Claim 1 and claim 5 of Elementary Arithmetic in an Ordered Field, applied with the nonnegative factor 2\sqrt{2},

βˆ£Ο•j(t)∣=∣2βˆ£β€‰βˆ£Cj(t)∣=2β€‰βˆ£Cj(t)βˆ£β‰€2β‹…1=2.|\phi_{j}(t)|=|\sqrt{2}|\,|C_{j}(t)|=\sqrt{2}\,|C_{j}(t)|\le\sqrt{2}\cdot1=\sqrt{2}.

For the periodicity, let p∈Zp\in\mathbb{Z}. Then jp∈Zjp\in\mathbb{Z} by claim 2 of Arithmetic, Order and Discreteness of the Integers, and by distributivity 2Ο€j(t+p)=2Ο€jt+2Ο€(jp)2\pi j(t+p)=2\pi jt+2\pi(jp), so Quarter-Turn Identities and Periodicity of Sine and Cosine Β§integer, applied at the real number 2Ο€jt2\pi jt with the integer jpjp, gives Cj(t+p)=cos⁑(2Ο€jt+2Ο€(jp))=cos⁑(2Ο€jt)=Cj(t)C_{j}(t+p)=\cos(2\pi jt+2\pi(jp))=\cos(2\pi jt)=C_{j}(t), whence Ο•j(t+p)=Ο•j(t)\phi_{j}(t+p)=\phi_{j}(t).

Suppose j<0j<0, so βˆ’j∈Z-j\in\mathbb{Z} by claim 2 of Arithmetic, Order and Discreteness of the Integers and Ο•j=2 Sβˆ’j\phi_{j}=\sqrt{2}\,S_{-j}. The three assertions follow exactly as in the previous case, with Sβˆ’jS_{-j} in place of CjC_{j} and with the sine half of Cell Integrals of the Trigonometric Monomials Β§calculus and of Quarter-Turn Identities and Periodicity of Sine and Cosine Β§integer. This proves Claim 2.

Proof of claim 4 of the statement. Let m∈Zm\in\mathbb{Z}. The bound βˆ£Ο•m(t)βˆ£β‰€2|\phi_{m}(t)|\le\sqrt{2} is Claim 2. For the derivative we use Cell Integrals of the Trigonometric Monomials Β§calculus, which gives Cjβ€²(t)=βˆ’2Ο€j Sj(t)C_{j}'(t)=-2\pi j\,S_{j}(t) and Sjβ€²(t)=2Ο€j Cj(t)S_{j}'(t)=2\pi j\,C_{j}(t) for every j∈Zj\in\mathbb{Z}, and claim 2 of Sum, Constant Multiple, and Product Rules for One-Dimensional Derivatives, applied with the constant 2\sqrt{2} and the relevant companion map.

If m=0m=0 then Ο•0\phi_{0} is constant, so Ο•0β€²(t)=0\phi_{0}'(t)=0 by claim 1 of Sum, Constant Multiple, and Product Rules for One-Dimensional Derivatives; and βˆ’2Ο€β‹…0β‹…Ο•0(t)=0-2\pi\cdot0\cdot\phi_{0}(t)=0 by claim 1 of Zero Products and Elementary Identities in a Field, so the identity holds.

If 0<m0<m then βˆ’m<0-m<0 by claim 4 of Elementary Order Arithmetic in an Ordered Field, so Ο•βˆ’m=2 Sβˆ’(βˆ’m)=2 Sm\phi_{-m}=\sqrt{2}\,S_{-(-m)}=\sqrt{2}\,S_{m}, and

Ο•mβ€²(t)=2 Cmβ€²(t)=2 (βˆ’2Ο€m Sm(t))=βˆ’2Ο€m (2 Sm(t))=βˆ’2Ο€mβ€‰Ο•βˆ’m(t),\phi_{m}'(t)=\sqrt{2}\,C_{m}'(t)=\sqrt{2}\,\bigl(-2\pi m\,S_{m}(t)\bigr)=-2\pi m\,\bigl(\sqrt{2}\,S_{m}(t)\bigr)=-2\pi m\,\phi_{-m}(t),

the third equality by commutativity and associativity together with claim 2 of Zero Products and Elementary Identities in a Field.

If m<0m<0 then 0<βˆ’m0<-m by claim 4 of Elementary Order Arithmetic in an Ordered Field, so Ο•m=2 Sβˆ’m\phi_{m}=\sqrt{2}\,S_{-m} and Ο•βˆ’m=2 Cβˆ’m\phi_{-m}=\sqrt{2}\,C_{-m}, and

Ο•mβ€²(t)=2 Sβˆ’mβ€²(t)=2 (2Ο€(βˆ’m) Cβˆ’m(t))=βˆ’2Ο€m (2 Cβˆ’m(t))=βˆ’2Ο€mβ€‰Ο•βˆ’m(t),\phi_{m}'(t)=\sqrt{2}\,S_{-m}'(t)=\sqrt{2}\,\bigl(2\pi(-m)\,C_{-m}(t)\bigr)=-2\pi m\,\bigl(\sqrt{2}\,C_{-m}(t)\bigr)=-2\pi m\,\phi_{-m}(t),

using claim 2 of Zero Products and Elementary Identities in a Field for 2Ο€(βˆ’m)=βˆ’(2Ο€m)2\pi(-m)=-(2\pi m).

Proof of claim 2 of the statement. Let a,b∈Za,b\in\mathbb{Z}. By Claim 2 both Ο•a\phi_{a} and Ο•b\phi_{b} are continuous on R\mathbb{R}, so Ο•aΟ•b\phi_{a}\phi_{b} is continuous on R\mathbb{R} by claim 5 of Continuity of Sums and Products of Real-Valued Functions on a Metric Space, applied on R\mathbb{R} to the two companions Ο•a\phi_{a} and Ο•b\phi_{b}; hence its restriction to JJ is BJ\mathcal{B}_{J}-measurable and Ξ»J\lambda_{J}-integrable by Zero Extension of a Real-Valued Function, and the Unit-Cell Integral of a Continuous Function Β§continuous. The same applies to each of the maps CaC_{a}, SaS_{a}, CaCbC_{a}C_{b}, SaSbS_{a}S_{b} and SaCbS_{a}C_{b} appearing below, by Cell Integrals of the Trigonometric Monomials Β§calculus. Throughout we use claim 2 of Linearity and Monotonicity of the Lebesgue Integral, applied with a real constant and with the relevant integrable companion in both slots, to pull a constant factor out of an integral over JJ.

By claim 1 of Arithmetic, Order and Discreteness of the Integers each of aa and bb is zero, positive or negative, and we treat the nine resulting cases.

If a=0a=0 and b=0b=0 then Ο•aΟ•b\phi_{a}\phi_{b} is the constant map 11, which is C0C0C_{0}C_{0} because C0C_{0} is the constant map 11 by Cell Integrals of the Trigonometric Monomials Β§calculus; so ∫JΟ•aΟ•b dΞ»J=1\int_{J}\phi_{a}\phi_{b}\,d\lambda_{J}=1 by Cell Integrals of the Trigonometric Monomials Β§cosine-cosine with k=m=0k=m=0. Here a=ba=b.

If a=0a=0 and 0<b0<b then Ο•aΟ•b=2 Cb\phi_{a}\phi_{b}=\sqrt{2}\,C_{b}, so the integral is 2∫JCb dΞ»J=2β‹…0=0\sqrt{2}\int_{J}C_{b}\,d\lambda_{J}=\sqrt{2}\cdot0=0 by Cell Integrals of the Trigonometric Monomials Β§single and claim 1 of Zero Products and Elementary Identities in a Field; and aβ‰ ba\ne b. If a=0a=0 and b<0b<0 then Ο•aΟ•b=2 Sβˆ’b\phi_{a}\phi_{b}=\sqrt{2}\,S_{-b} and the integral is 00 for the same reason. The two cases with b=0b=0 and aβ‰ 0a\ne0 are the same computations with the roles of aa and bb exchanged, the product being unchanged by commutativity.

If 0<a0<a and 0<b0<b then Ο•aΟ•b=(2 2) CaCb=2 CaCb\phi_{a}\phi_{b}=(\sqrt{2}\,\sqrt{2})\,C_{a}C_{b}=2\,C_{a}C_{b} by Claim 1, so the integral is 2∫JCaCb dΞ»J2\int_{J}C_{a}C_{b}\,d\lambda_{J}. If a=ba=b then aβ‰ 0a\ne0 and ∣a∣=∣b∣|a|=|b|, so Cell Integrals of the Trigonometric Monomials Β§cosine-cosine gives ∫JCaCb dΞ»J=2βˆ’1\int_{J}C_{a}C_{b}\,d\lambda_{J}=2^{-1} and the integral is 2β‹…2βˆ’1=12\cdot2^{-1}=1. If aβ‰ ba\ne b then ∣a∣=aβ‰ b=∣b∣|a|=a\ne b=|b| by Absolute Value in an Ordered Field, since aa and bb are positive; so that clause gives ∫JCaCb dΞ»J=0\int_{J}C_{a}C_{b}\,d\lambda_{J}=0 and the integral is 00 by claim 1 of Zero Products and Elementary Identities in a Field.

If a<0a<0 and b<0b<0 then βˆ’a-a and βˆ’b-b are positive by claim 4 of Elementary Order Arithmetic in an Ordered Field and lie in Z\mathbb{Z} by claim 2 of Arithmetic, Order and Discreteness of the Integers, and Ο•aΟ•b=2 Sβˆ’aSβˆ’b\phi_{a}\phi_{b}=2\,S_{-a}S_{-b}, so the integral is 2∫JSβˆ’aSβˆ’b dΞ»J2\int_{J}S_{-a}S_{-b}\,d\lambda_{J}. If a=ba=b then βˆ’a=βˆ’b-a=-b and βˆ’aβ‰ 0-a\ne0, so Cell Integrals of the Trigonometric Monomials Β§sine-sine gives 2βˆ’12^{-1} and the integral is 11. If aβ‰ ba\ne b then βˆ’aβ‰ βˆ’b-a\ne-b; moreover βˆ’aβ‰ βˆ’(βˆ’b)=b-a\ne-(-b)=b, because βˆ’a-a is positive and bb is negative; and βˆ£βˆ’a∣=βˆ’aβ‰ βˆ’b=βˆ£βˆ’b∣|-a|=-a\ne-b=|-b| by Absolute Value in an Ordered Field, since βˆ’a-a and βˆ’b-b are positive. So the remaining case of Cell Integrals of the Trigonometric Monomials Β§sine-sine, taken with k=βˆ’ak=-a and m=βˆ’bm=-b, gives ∫JSβˆ’aSβˆ’b dΞ»J=0\int_{J}S_{-a}S_{-b}\,d\lambda_{J}=0, and the integral is 00.

If 0<a0<a and b<0b<0 then Ο•aΟ•b=2 CaSβˆ’b=2 Sβˆ’bCa\phi_{a}\phi_{b}=2\,C_{a}S_{-b}=2\,S_{-b}C_{a}, so the integral is 2∫JSβˆ’bCa dΞ»J=02\int_{J}S_{-b}C_{a}\,d\lambda_{J}=0 by Cell Integrals of the Trigonometric Monomials Β§sine-cosine and claim 1 of Zero Products and Elementary Identities in a Field; and aβ‰ ba\ne b, since aa is positive and bb is negative. The case a<0a<0, 0<b0<b is the same with the roles exchanged. This exhausts the nine cases and proves claim 2 of the statement.

Claim 3. (Coordinate projections are continuous.) Let i∈[n]i\in[n] and let Ο€i:Rnβ†’R\pi_{i}:\mathbb{R}^{n}\to\mathbb{R} be the map Ο€i(x)=xi\pi_{i}(x)=x_{i}. Then Ο€i\pi_{i} is continuous on Rn\mathbb{R}^{n} relative to Rn\mathbb{R}^{n}, as a map from (Rn,dE)(\mathbb{R}^{n},d_{E}) into R\mathbb{R} with the absolute value metric dRd_{\mathbb{R}}.

Proof of Claim 3. Let x∈Rnx\in\mathbb{R}^{n} and let Ξ΅\varepsilon be a positive real number; choose Ξ΄=Ξ΅\delta=\varepsilon. Let y∈Rny\in\mathbb{R}^{n} satisfy dE(x,y)<Ξ΄d_{E}(x,y)<\delta. By claim 2 of Elementary Properties of the Euclidean Norm on Rn\mathbb{R}^n, dE(x,y)=βˆ₯xβˆ’yβˆ₯d_{E}(x,y)=\lVert x-y\rVert, and the iith coordinate of xβˆ’yx-y is xiβˆ’yix_{i}-y_{i} by the definition of the difference of points; so claim 4 of that lemma gives

dR(Ο€i(x),Ο€i(y))=∣xiβˆ’yiβˆ£β‰€βˆ₯xβˆ’yβˆ₯=dE(x,y)<Ξ΅.d_{\mathbb{R}}\bigl(\pi_{i}(x),\pi_{i}(y)\bigr)=|x_{i}-y_{i}|\le\lVert x-y\rVert=d_{E}(x,y)<\varepsilon .

This is the condition of Continuous Map Between Metric Spaces at xx relative to Rn\mathbb{R}^{n}, and xx was arbitrary. This proves Claim 3.

Proof of claim 1 of the statement. Let k∈Znk\in\mathbb{Z}^{n}, so that ki∈Zk_{i}\in\mathbb{Z} for every i∈[n]i\in[n] by Lattice-Periodic Functions and the Periodic Function Classes §lattice.

First, eke_{k} is continuous on Rn\mathbb{R}^{n}, in the sense fixed in Lattice-Periodic Functions and the Periodic Function Classes. Indeed, for i∈[n]i\in[n] the map Ο•kiβˆ˜Ο€i\phi_{k_{i}}\circ\pi_{i}, whose value at xx is Ο•ki(xi)\phi_{k_{i}}(x_{i}), is continuous on Rn\mathbb{R}^{n} by claim 3 of Semicontinuity and Continuity Under Composition with a Continuous Map, applied with the metric spaces (Rn,dE)(\mathbb{R}^{n},d_{E}) and (R,dR)(\mathbb{R},d_{\mathbb{R}}), with g=Ο€ig=\pi_{i} continuous by Claim 3, and with u=Ο•kiu=\phi_{k_{i}} continuous by Claim 2. Now let pj:Rnβ†’Rp_{j}:\mathbb{R}^{n}\to\mathbb{R} be pj(x)=∏i=1jΟ•ki(xi)p_{j}(x)=\prod_{i=1}^{j}\phi_{k_{i}}(x_{i}) for j∈[n]j\in[n]. By claim 1 of Properties of Finite Products, p1=Ο•k1βˆ˜Ο€1p_{1}=\phi_{k_{1}}\circ\pi_{1} and pS(r)p_{S(r)} is the pointwise product of prp_{r} and Ο•kS(r)βˆ˜Ο€S(r)\phi_{k_{S(r)}}\circ\pi_{S(r)} whenever S(r)∈[n]S(r)\in[n], where SS is the successor map of Natural Numbers. An induction on jj bounded by nn β€” applying Principle of Induction for the Natural Numbers to the set of natural numbers jj such that either n<jn<j, or j≀nj\le n and pjp_{j} is continuous, which contains 11 and is closed under the successor because j<S(j)≀nj<S(j)\le n forces j≀nj\le n by claim 1 of Properties of the Order on the Natural Numbers β€” gives, using claim 5 of Continuity of Sums and Products of Real-Valued Functions on a Metric Space at each successor step, that pn=ekp_{n}=e_{k} is continuous on Rn\mathbb{R}^{n}.

Second, eke_{k} is Zn\mathbb{Z}^{n}-periodic. Let x∈Rnx\in\mathbb{R}^{n} and m∈Znm\in\mathbb{Z}^{n}. The iith coordinate of x+mx+m is xi+mix_{i}+m_{i} by the definition of the sum of points, and mi∈Zm_{i}\in\mathbb{Z} by Lattice-Periodic Functions and the Periodic Function Classes Β§lattice; so Ο•ki(xi+mi)=Ο•ki(xi)\phi_{k_{i}}(x_{i}+m_{i})=\phi_{k_{i}}(x_{i}) for every i∈[n]i\in[n] by Claim 2. The two maps i↦ϕki((x+m)i)i\mapsto\phi_{k_{i}}((x+m)_{i}) and i↦ϕki(xi)i\mapsto\phi_{k_{i}}(x_{i}) on [n][n] therefore coincide, so ek(x+m)=ek(x)e_{k}(x+m)=e_{k}(x).

Hence ek∈Cpere_{k}\in C_{\mathrm{per}} by Lattice-Periodic Functions and the Periodic Function Classes Β§classes. By Continuous Periodic Functions are Power-Integrable and Dense on the Torus Β§member, used with p=2p=2, the restriction ek∣Qe_{k}|_{Q} is measurable with respect to BQ\mathcal{B}_{Q} and belongs to L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}); the bound required there exists by Elementary Properties of Lattice-Periodic Functions Β§bounded, as that claim itself records. So Ek=[ ek∣Q ]E_{k}=[\,e_{k}|_{Q}\,] is a well-defined member of L2(Tn)L^{2}(\mathbb{T}^{n}).

Proof of claim 3 of the statement. Let k,m∈Znk,m\in\mathbb{Z}^{n}. By The Lebesgue Space of Square-Integrable Functions is a Real Hilbert Space §inner-product, applied to the measure space (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}) of The Flat Torus: Standing Notation §measure and to the members ek∣Qe_{k}|_{Q} and em∣Qe_{m}|_{Q} of L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}) furnished by claim 1 of the statement,

⟨Ek,Em⟩L2(Tn)=∫Tn(ek∣Q)(em∣Q) dx,\langle E_{k},E_{m}\rangle_{L^{2}(\mathbb{T}^{n})}=\int_{\mathbb{T}^{n}}(e_{k}|_{Q})(e_{m}|_{Q})\,dx ,

the pointwise product being integrable by that clause. The maps (ek∣Q)(em∣Q)(e_{k}|_{Q})(e_{m}|_{Q}) and (ekem)∣Q(e_{k}e_{m})|_{Q} agree, both taking the value ek(x)em(x)e_{k}(x)e_{m}(x) at x∈Qx\in Q, by Restriction of a Map to a Subset.

For i∈[n]i\in[n] let gi:Jβ†’Rg_{i}:J\to\mathbb{R} be the restriction to JJ of Ο•kiΟ•mi\phi_{k_{i}}\phi_{m_{i}}. That map is continuous on R\mathbb{R} by claim 2 of the statement, so gig_{i} is measurable with respect to BJ\mathcal{B}_{J} by Zero Extension of a Real-Valued Function, and the Unit-Cell Integral of a Continuous Function Β§continuous; and by Claim 2 and claim 4 of Properties of the Absolute Value in an Ordered Field, together with Claim 1 and claim 5 of Elementary Arithmetic in an Ordered Field applied twice,

∣gi(t)∣=βˆ£Ο•ki(t)βˆ£β€‰βˆ£Ο•mi(t)βˆ£β‰€2 2=2(t∈J).|g_{i}(t)|=|\phi_{k_{i}}(t)|\,|\phi_{m_{i}}(t)|\le\sqrt{2}\,\sqrt{2}=2\qquad(t\in J).

So the hypotheses of The Integral over the Unit Cell of a Product of One-Variable Functions are met with these gig_{i} and with the bounds Mi=2M_{i}=2. For x∈Qx\in Q we have xi∈Jx_{i}\in J for every i∈[n]i\in[n], as recorded in The Integral over the Unit Cell of a Product of One-Variable Functions, and by claim 2 of Properties of Finite Products, applied to the two maps i↦ϕki(xi)i\mapsto\phi_{k_{i}}(x_{i}) and i↦ϕmi(xi)i\mapsto\phi_{m_{i}}(x_{i}) on [n][n],

∏i=1ngi(xi)=∏i=1nΟ•ki(xi)Ο•mi(xi)=(∏i=1nΟ•ki(xi))(∏i=1nΟ•mi(xi))=ek(x)em(x),\prod_{i=1}^{n}g_{i}(x_{i})=\prod_{i=1}^{n}\phi_{k_{i}}(x_{i})\phi_{m_{i}}(x_{i})=\Bigl(\prod_{i=1}^{n}\phi_{k_{i}}(x_{i})\Bigr)\Bigl(\prod_{i=1}^{n}\phi_{m_{i}}(x_{i})\Bigr)=e_{k}(x)e_{m}(x),

so the map GG of that lemma is (ekem)∣Q(e_{k}e_{m})|_{Q}. The clause The Integral over the Unit Cell of a Product of One-Variable Functions §integral therefore gives

⟨Ek,Em⟩L2(Tn)=∫Tn(ekem)∣Q dx=∏i=1n∫JΟ•kiΟ•mi dΞ»J.\langle E_{k},E_{m}\rangle_{L^{2}(\mathbb{T}^{n})}=\int_{\mathbb{T}^{n}}(e_{k}e_{m})|_{Q}\,dx=\prod_{i=1}^{n}\int_{J}\phi_{k_{i}}\phi_{m_{i}}\,d\lambda_{J}.

By claim 2 of the statement the iith factor equals 11 if ki=mik_{i}=m_{i} and equals 00 if ki≠mik_{i}\ne m_{i}.

Points of Rn\mathbb{R}^{n} are nn-tuples of real numbers, so k=mk=m if and only if ki=mik_{i}=m_{i} for every i∈[n]i\in[n]. If k=mk=m then every factor equals 11, so the product equals 11 by claim 3 of Properties of Finite Products, applied with i=1i=1. If kβ‰ mk\ne m then kiβ‰ mik_{i}\ne m_{i} for some i∈[n]i\in[n], so that factor is 00 and the product is 00 by claim 4 of Properties of Finite Products. This proves claim 3 of the statement.

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