TheoremBase

Along a coordinate slice the product collapses to a constant multiple of a single one-variable factor, so the partial derivative is read off from the one-variable derivative rule; the weak derivative then agrees with the classical one, and orthogonality follows from orthonormality of the system.

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, for s⋅1=ss\cdot1=s, and for the injectivity of the additive inverse, that is, −s=−t-s=-t implies s=ts=t. 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, ϕm\phi_{m} for m∈Zm\in\mathbb{Z} are the one-dimensional maps of The Trigonometric System on the Torus (i), so that ek(x)=∏j=1nϕkj(xj)e_{k}(x)=\prod_{j=1}^{n}\phi_{k_{j}}(x_{j}).

Claim 1. (The flipped index.) Let k∈Znk\in\mathbb{Z}^{n} and i∈[n]i\in[n]. Then k(i)∈Znk^{(i)}\in\mathbb{Z}^{n}.

Proof of Claim 1. Every coordinate of kk lies in Z\mathbb{Z} by Lattice-Periodic Functions and the Periodic Function Classes (i), and −ki∈Z-k_{i}\in\mathbb{Z} by claim 2 of Arithmetic, Order, Discreteness and Intervals of the Integers; so every coordinate of k(i)k^{(i)} lies in Z\mathbb{Z}, and k(i)∈Znk^{(i)}\in\mathbb{Z}^{n} by the same clause of Lattice-Periodic Functions and the Periodic Function Classes. This proves Claim 1.

Claim 2. (The slice of the product.) Let k∈Znk\in\mathbb{Z}^{n}, let i∈[n]i\in[n] and let a∈Rna\in\mathbb{R}^{n}. For s∈Rs\in\mathbb{R} let a[s]a[s] denote the point of Rn\mathbb{R}^{n} whose iith coordinate is ss and whose jjth coordinate is aja_{j} for every j∈[n]j\in[n] with j≠ij\ne i. Let c∈Rc\in\mathbb{R} be the finite product of the map [n]→R[n]\to\mathbb{R} taking the value 11 at ii and the value ϕkj(aj)\phi_{k_{j}}(a_{j}) at every j≠ij\ne i. Then

ek(a[s])=c ϕki(s)for every s∈R,andek(i)(a)=c ϕ−ki(ai).e_{k}(a[s])=c\,\phi_{k_{i}}(s)\quad\text{for every }s\in\mathbb{R}, \qquad\text{and}\qquad e_{k^{(i)}}(a)=c\,\phi_{-k_{i}}(a_{i}).

Proof of Claim 2. Write u:[n]→Ru:[n]\to\mathbb{R} for the map just described, so that c=∏j=1nujc=\prod_{j=1}^{n}u_{j}. Fix s∈Rs\in\mathbb{R} and let v:[n]→Rv:[n]\to\mathbb{R} take the value ϕki(s)\phi_{k_{i}}(s) at ii and the value 11 at every j≠ij\ne i. Then ujvj=ϕkj(a[s]j)u_{j}v_{j}=\phi_{k_{j}}(a[s]_{j}) for every j∈[n]j\in[n]: at j=ij=i both sides are ϕki(s)\phi_{k_{i}}(s), and at j≠ij\ne i both sides are ϕkj(aj)\phi_{k_{j}}(a_{j}), since a[s]j=aja[s]_{j}=a_{j} there. Hence by claim 2 of Properties of Finite Products,

ek(a[s])=∏j=1nujvj=(∏j=1nuj)(∏j=1nvj)=c ϕki(s),e_{k}(a[s])=\prod_{j=1}^{n}u_{j}v_{j}=\Bigl(\prod_{j=1}^{n}u_{j}\Bigr)\Bigl(\prod_{j=1}^{n}v_{j}\Bigr)=c\,\phi_{k_{i}}(s),

the last equality by claim 3 of Properties of Finite Products, applied with the index ii, since vj=1v_{j}=1 for every j≠ij\ne i.

The second identity is the same computation with w:[n]→Rw:[n]\to\mathbb{R} taking the value ϕ−ki(ai)\phi_{-k_{i}}(a_{i}) at ii and 11 elsewhere: then ujwj=ϕkj(i)(aj)u_{j}w_{j}=\phi_{k^{(i)}_{j}}(a_{j}) for every j∈[n]j\in[n], because the iith coordinate of k(i)k^{(i)} is −ki-k_{i} and its other coordinates agree with those of kk; so ek(i)(a)=c ϕ−ki(ai)e_{k^{(i)}}(a)=c\,\phi_{-k_{i}}(a_{i}) by the same two clauses. This proves Claim 2.

Proof of claim 1 of the statement. Fix k∈Znk\in\mathbb{Z}^{n}; Claim 1 gives k(i)∈Znk^{(i)}\in\mathbb{Z}^{n} for every i∈[n]i\in[n].

The partial derivatives exist and have the stated values. Let i∈[n]i\in[n] and a∈Rna\in\mathbb{R}^{n}, and let a[s]a[s] and cc be as in Claim 2. Apply Slice Function and the Partial Derivative with the open set Rn\mathbb{R}^{n}, the map eke_{k}, the point aa and the index ii: claim 1 there provides a positive real ρ\rho, and claim 2 there introduces the slice function gg on the interval I={s∈R:ai−ρ<s<ai+ρ}I=\{s\in\mathbb{R}:a_{i}-\rho<s<a_{i}+\rho\} given by g(s)=ek(a[s])g(s)=e_{k}(a[s]), and states that the partial derivative of eke_{k} with respect to the iith variable exists at aa if and only if gg is differentiable at aia_{i}, in which case ∂iek(a)=g′(ai)\partial_{i}e_{k}(a)=g'(a_{i}).

By Claim 2 the map s↦c ϕki(s)s\mapsto c\,\phi_{k_{i}}(s) on R\mathbb{R} agrees with gg on II. That map is differentiable at every point of R\mathbb{R} with derivative c ϕki′c\,\phi_{k_{i}}' there, by The Trigonometric System on the Torus is Orthonormal (iv) and claim 2 of Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers, applied on the interval R\mathbb{R} with the constant cc and the companion ϕki\phi_{k_{i}}; every point of R\mathbb{R} is an interior point of R\mathbb{R} by Basic Facts about Intervals of the Real Line (i), so that claim applies at each of them. The point aia_{i} is an interior point of II by Basic Facts about Intervals of the Real Line (iv), and I⊆RI\subseteq\mathbb{R}, so claim 2 of Restriction Stability of Continuity and of the Derivative gives that gg is differentiable at aia_{i} with

g′(ai)=c ϕki′(ai)=c (−2πki ϕ−ki(ai))=−2πki (c ϕ−ki(ai))=−2πki ek(i)(a),g'(a_{i})=c\,\phi_{k_{i}}'(a_{i})=c\,\bigl(-2\pi k_{i}\,\phi_{-k_{i}}(a_{i})\bigr)=-2\pi k_{i}\,\bigl(c\,\phi_{-k_{i}}(a_{i})\bigr)=-2\pi k_{i}\,e_{k^{(i)}}(a),

using The Trigonometric System on the Torus is Orthonormal (iv) for the second equality, commutativity and associativity together with claim 2 of Zero Products and Elementary Identities in a Field for the third, and Claim 2 for the fourth. Hence ∂iek(a)\partial_{i}e_{k}(a) exists and equals −2πki ek(i)(a)-2\pi k_{i}\,e_{k^{(i)}}(a), which is the displayed identity.

Class C1C^{1}. By The Trigonometric System on the Torus is Orthonormal (i) the map eke_{k} lies in CperC_{\mathrm{per}}, hence is continuous on Rn\mathbb{R}^{n} relative to Rn\mathbb{R}^{n} in the sense fixed in Lattice-Periodic Functions and the Periodic Function Classes; by claim 1 of Euclidean Continuity Agrees with Metric Continuity for Real-Valued Functions it is therefore continuous in the Euclidean sense at every point of Rn\mathbb{R}^{n}. For i∈[n]i\in[n] the map ∂iek\partial_{i}e_{k} equals −2πki ek(i)-2\pi k_{i}\,e_{k^{(i)}} by the previous paragraph; the map ek(i)e_{k^{(i)}} lies in CperC_{\mathrm{per}} by The Trigonometric System on the Torus is Orthonormal (i) and Claim 1, so ∂iek\partial_{i}e_{k} is continuous on Rn\mathbb{R}^{n} relative to Rn\mathbb{R}^{n} by claim 5 of Continuity of Sums and Products of Real-Valued Functions on a Metric Space, in its scalar-multiple form, applied on Rn\mathbb{R}^{n} with the real constant −2πki-2\pi k_{i} and the companion ek(i)e_{k^{(i)}}, and hence is continuous in the Euclidean sense at every point of Rn\mathbb{R}^{n} by claim 1 of Euclidean Continuity Agrees with Metric Continuity for Real-Valued Functions. So eke_{k} is continuous at every point of Rn\mathbb{R}^{n}, all of its partial derivatives exist at every point of Rn\mathbb{R}^{n}, and each ∂iek\partial_{i}e_{k} is continuous at every point of Rn\mathbb{R}^{n}; by clauses 1 and 3 of Functions of Class Cᵏ on an Open Subset of ℝⁿ the map eke_{k} is of class C1C^{1} on Rn\mathbb{R}^{n}.

Finally eke_{k} is Zn\mathbb{Z}^{n}-periodic, being a member of CperC_{\mathrm{per}}, so ek∈Cper1e_{k}\in C^{1}_{\mathrm{per}} by Lattice-Periodic Functions and the Periodic Function Classes (iii).

Proof of claim 2 of the statement. Let k∈Znk\in\mathbb{Z}^{n}. By claim 1 of the statement ek∈Cper1e_{k}\in C^{1}_{\mathrm{per}}, so Ek=[ ek∣Q ]E_{k}=[\,e_{k}|_{Q}\,] lies in H1(Tn)H^{1}(\mathbb{T}^{n}) by The Sobolev Space of Once Weakly Differentiable Square-Integrable Classes on the Torus (i).

Let i∈[n]i\in[n]. By Elementary Properties of the Weak Partial Derivative on the Torus (i), applied to ek∈Cper1e_{k}\in C^{1}_{\mathrm{per}} with r=2r=2, the class [ (∂iek)∣Q ][\,(\partial_{i}e_{k})|_{Q}\,] is the ii-th weak partial derivative of EkE_{k} in L2(Tn)L^{2}(\mathbb{T}^{n}). By claim 1 of the statement ∂iek=−2πki ek(i)\partial_{i}e_{k}=-2\pi k_{i}\,e_{k^{(i)}} as maps on Rn\mathbb{R}^{n}, and ek(i)∈Cpere_{k^{(i)}}\in C_{\mathrm{per}} by The Trigonometric System on the Torus is Orthonormal (i), so Continuous Periodic Functions are Power-Integrable and Dense on the Torus (iii), used with p=2p=2 and the scalar −2πki-2\pi k_{i}, gives

[ (∂iek)∣Q ]=[ (−2πki ek(i))∣Q ]=−2πki [ ek(i)∣Q ]=−2πki Ek(i).\bigl[\,(\partial_{i}e_{k})|_{Q}\,\bigr]=\bigl[\,(-2\pi k_{i}\,e_{k^{(i)}})|_{Q}\,\bigr]=-2\pi k_{i}\,\bigl[\,e_{k^{(i)}}|_{Q}\,\bigr]=-2\pi k_{i}\,E_{k^{(i)}} .

Hence ∂iEk=−2πkiEk(i)\partial_{i}E_{k}=-2\pi k_{i}E_{k^{(i)}}.

Proof of claim 3 of the statement. Let k,m∈Znk,m\in\mathbb{Z}^{n}. By The Sobolev Space of Once Weakly Differentiable Square-Integrable Classes on the Torus (ii) and claim 2 of the statement,

⟨Ek,Em⟩H1=⟨Ek,Em⟩L2+∑j=1n⟨−2πkjEk(j), −2πmjEm(j)⟩L2.\langle E_{k},E_{m}\rangle_{H^{1}}=\langle E_{k},E_{m}\rangle_{L^{2}}+\sum_{j=1}^{n}\bigl\langle -2\pi k_{j}E_{k^{(j)}},\,-2\pi m_{j}E_{m^{(j)}}\bigr\rangle_{L^{2}} .

For each jj, the linearity of the inner product in its first argument and its symmetry, both recorded in Real Inner Product Spaces (i), give

⟨−2πkjEk(j), −2πmjEm(j)⟩L2=(−2πkj)(−2πmj) ⟨Ek(j),Em(j)⟩L2=4π2kjmj ⟨Ek(j),Em(j)⟩L2,\bigl\langle -2\pi k_{j}E_{k^{(j)}},\,-2\pi m_{j}E_{m^{(j)}}\bigr\rangle_{L^{2}}=(-2\pi k_{j})(-2\pi m_{j})\,\bigl\langle E_{k^{(j)}},E_{m^{(j)}}\bigr\rangle_{L^{2}}=4\pi^{2}k_{j}m_{j}\,\bigl\langle E_{k^{(j)}},E_{m^{(j)}}\bigr\rangle_{L^{2}},

the second equality by claim 2 of Zero Products and Elementary Identities in a Field and 4=2+2=2⋅24=2+2=2\cdot2.

Suppose first k=mk=m. Then k(j)=m(j)k^{(j)}=m^{(j)} for every jj, so ⟨Ek,Em⟩L2=1\langle E_{k},E_{m}\rangle_{L^{2}}=1 and ⟨Ek(j),Em(j)⟩L2=1\langle E_{k^{(j)}},E_{m^{(j)}}\rangle_{L^{2}}=1 for every jj, by The Trigonometric System on the Torus is Orthonormal (iii). Hence the jjth summand is 4π2kjkj=4π2kj24\pi^{2}k_{j}k_{j}=4\pi^{2}k_{j}^{2}, and by claim 3 of Properties of Finite Sums, applied with the constant 4π24\pi^{2}, together with claim 1 of Properties of the Euclidean Norm on Rn\mathbb{R}^n: Square, Distance, Vanishing, Coordinate Bounds, Homogeneity, Triangle Inequalities and Expansion of a Square,

∑j=1n4π2kj2=4π2∑j=1nkj2=4π2∥k∥2,\sum_{j=1}^{n}4\pi^{2}k_{j}^{2}=4\pi^{2}\sum_{j=1}^{n}k_{j}^{2}=4\pi^{2}\lVert k\rVert^{2},

so ⟨Ek,Em⟩H1=1+4π2∥k∥2\langle E_{k},E_{m}\rangle_{H^{1}}=1+4\pi^{2}\lVert k\rVert^{2}.

Suppose now k≠mk\ne m. Then ⟨Ek,Em⟩L2=0\langle E_{k},E_{m}\rangle_{L^{2}}=0 by The Trigonometric System on the Torus is Orthonormal (iii). Moreover k(j)≠m(j)k^{(j)}\ne m^{(j)} for every j∈[n]j\in[n]: points of Rn\mathbb{R}^{n} are nn-tuples of real numbers, and k(j)=m(j)k^{(j)}=m^{(j)} would give −kj=−mj-k_{j}=-m_{j}, hence kj=mjk_{j}=m_{j}, together with kl=mlk_{l}=m_{l} for every l≠jl\ne j, that is k=mk=m. So each ⟨Ek(j),Em(j)⟩L2\langle E_{k^{(j)}},E_{m^{(j)}}\rangle_{L^{2}} vanishes by the same clause, each summand is 00 by claim 1 of Zero Products and Elementary Identities in a Field, and the sum is 00 by claim 7 of Properties of Finite Sums, applied with the index 11, every other summand being 00. Hence ⟨Ek,Em⟩H1=0+0=0\langle E_{k},E_{m}\rangle_{H^{1}}=0+0=0.

Citations

Loading…

Dependencies

Uses0

Loading…

Comments

Log in to comment.

Loading…