TheoremBase

Differentiating the known first partial derivative of a member of the trigonometric system a second time returns a multiple of the member itself, because reflecting one frequency coordinate twice restores the frequency. The coefficient identity follows by moving both derivatives onto the trigonometric factor through the weak-derivative test identity, applied once with the member and once with its partial derivative as test function.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied here to the data named. For k∈Znk\in\mathbb{Z}^{n} and i∈[n]i\in[n] let k(i)k^{(i)} be the point of Rn\mathbb{R}^{n} whose ii-th component is −ki-k_{i} and whose jj-th component is kjk_{j} for j∈[n]j\in[n] with j≠ij\ne i, as introduced in The Trigonometric System is Continuously Differentiable and Orthogonal in the Sobolev Space of the Torus, which records that k(i)∈Znk^{(i)}\in\mathbb{Z}^{n} and that

ek∈Cper1,∂iek(x)=−2πki ek(i)(x)for every x∈Rn,e_{k}\in C^{1}_{\mathrm{per}},\qquad \partial_{i}e_{k}(x)=-2\pi k_{i}\,e_{k^{(i)}}(x)\quad\text{for every }x\in\mathbb{R}^{n},

by The Trigonometric System is Continuously Differentiable and Orthogonal in the Sobolev Space of the Torus (i). Pointwise sums, scalar multiples and products of maps on Rn\mathbb{R}^{n} are those of Constants, Affine Functions, Sums, Products and Quotients of Cᵏ Functions.

Claim 1 (Reflecting one component twice). Let k∈Znk\in\mathbb{Z}^{n} and i∈[n]i\in[n]. Then (k(i))i=−ki(k^{(i)})_{i}=-k_{i} and (k(i))(i)=k(k^{(i)})^{(i)}=k.

The first is the definition of k(i)k^{(i)}. For the second, the ii-th component of (k(i))(i)(k^{(i)})^{(i)} is −(k(i))i=−(−ki)-(k^{(i)})_{i}=-(-k_{i}), which is kik_{i} because in a field the additive inverse of −ki-k_{i} is unique and kik_{i} is one such; and for j≠ij\ne i the jj-th component of (k(i))(i)(k^{(i)})^{(i)} is (k(i))j=kj(k^{(i)})_{j}=k_{j}. The two points of Rn\mathbb{R}^{n} therefore have the same components, so they are equal by claim 1 of Euclidean Points as Tuples of Real Numbers.

Claim 2 (Clause 1). Let k∈Znk\in\mathbb{Z}^{n} and i∈[n]i\in[n]. Applying the displayed identity of the preamble to k(i)k^{(i)} in place of kk, and then claim 1,

∂iek(i)(x)=−2π (k(i))i e(k(i))(i)(x)=−2π(−ki) ek(x)=2πki ek(x)\partial_{i}e_{k^{(i)}}(x)=-2\pi\,(k^{(i)})_{i}\,e_{(k^{(i)})^{(i)}}(x)=-2\pi(-k_{i})\,e_{k}(x)=2\pi k_{i}\,e_{k}(x)

for every x∈Rnx\in\mathbb{R}^{n}, using claim 2 of Zero Products and Elementary Identities in a Field for −2π(−ki)=2πki-2\pi(-k_{i})=2\pi k_{i}.

Now ∂iek\partial_{i}e_{k} is the scalar multiple (−2πki)ek(i)(-2\pi k_{i})e_{k^{(i)}} of ek(i)e_{k^{(i)}}, by the preamble. Since the partial derivative of ek(i)e_{k^{(i)}} with respect to the ii-th variable exists at every point, claim 1 of Constants, Affine Functions, Sums, Products and Quotients of Cᵏ Functions gives, for every x∈Rnx\in\mathbb{R}^{n},

∂i∂iek(x)=(−2πki) ∂iek(i)(x)=(−2πki)(2πki) ek(x)=−4π2ki2 ek(x),\partial_{i}\partial_{i}e_{k}(x)=(-2\pi k_{i})\,\partial_{i}e_{k^{(i)}}(x)=(-2\pi k_{i})(2\pi k_{i})\,e_{k}(x)=-4\pi^{2}k_{i}^{2}\,e_{k}(x),

the last equality being field arithmetic together with claim 2 of Zero Products and Elementary Identities in a Field.

It remains to see that eke_{k} is of class C2C^{2} on Rn\mathbb{R}^{n} and lies in Cper2C^{2}_{\mathrm{per}}. It is of class C1C^{1} on Rn\mathbb{R}^{n}, being a member of Cper1C^{1}_{\mathrm{per}} by the preamble and Lattice-Periodic Functions and the Periodic Function Classes (iii); and for each i∈[n]i\in[n] the function ∂iek=(−2πki)ek(i)\partial_{i}e_{k}=(-2\pi k_{i})e_{k^{(i)}} is of class C1C^{1} on Rn\mathbb{R}^{n} by claim 3 of Constants, Affine Functions, Sums, Products and Quotients of Cᵏ Functions, since ek(i)e_{k^{(i)}} is. By clause 2 of Functions of Class Cᵏ on an Open Subset of ℝⁿ, read with the scalar convention of clause 3 there, eke_{k} is of class C2C^{2} on Rn\mathbb{R}^{n}; and it is Zn\mathbb{Z}^{n}-periodic, being in Cper1C^{1}_{\mathrm{per}}, so it lies in Cper2C^{2}_{\mathrm{per}} by Lattice-Periodic Functions and the Periodic Function Classes (iii).

Claim 3 (Clause 2). Let k∈Znk\in\mathbb{Z}^{n} and x∈Rnx\in\mathbb{R}^{n}. By The Laplacian of a Twice Continuously Differentiable Function (i), applicable since eke_{k} is of class C2C^{2} on Rn\mathbb{R}^{n} by claim 2, and then by claim 2 again,

Δek(x)=∑i=1n∂i∂iek(x)=∑i=1n(−4π2ek(x))ki2=(−4π2ek(x))∑i=1nki2,\Delta e_{k}(x)=\sum_{i=1}^{n}\partial_{i}\partial_{i}e_{k}(x)=\sum_{i=1}^{n}\bigl(-4\pi^{2}e_{k}(x)\bigr)k_{i}^{2}=\bigl(-4\pi^{2}e_{k}(x)\bigr)\sum_{i=1}^{n}k_{i}^{2},

the last step by the homogeneity of claim 3 of Properties of Finite Sums. By 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 the remaining sum is ∥k∥2\lVert k\rVert^{2}, which gives clause 2.

Claim 4 (Regularity in clause 3). Let u∈Cper2u\in C^{2}_{\mathrm{per}} and i∈[n]i\in[n]. Then uu is of class C1C^{1} on Rn\mathbb{R}^{n} by claim 2 of Euclidean Space Is Open in Itself, hence u∈Cper1u\in C^{1}_{\mathrm{per}}, and u∈Cperu\in C_{\mathrm{per}} by claim 3 of that lemma with Lattice-Periodic Functions and the Periodic Function Classes (iii). By Elementary Properties of Lattice-Periodic Functions (ii) one has ∂iu∈Cper1\partial_{i}u\in C^{1}_{\mathrm{per}}, and then ∂i∂iu∈Cper\partial_{i}\partial_{i}u\in C_{\mathrm{per}} by that clause again.

Next, Δu∈Cper\Delta u\in C_{\mathrm{per}}. For m∈[n]m\in[n] let Pm:Rn→RP_{m}:\mathbb{R}^{n}\to\mathbb{R} be the map with Pm(x)=∑i=1m∂i∂iu(x)P_{m}(x)=\sum_{i=1}^{m}\partial_{i}\partial_{i}u(x). Throughout this paragraph m+1m+1 denotes the successor S(m)S(m) of mm, the two being equal by claim 1 of Arithmetic of Addition on the Natural Numbers, so that the clauses cited below, which are phrased with the successor map, apply as written.

Let TT be the union of the set of m∈Nm\in\mathbb{N} with n<mn<m and the set of m∈[n]m\in[n] with Pm∈CperP_{m}\in C_{\mathrm{per}}. Then 1∈T1\in T: if n<1n<1 this is immediate, and otherwise P1=∂1∂1uP_{1}=\partial_{1}\partial_{1}u by claim 1 of Properties of Finite Sums, which lies in CperC_{\mathrm{per}} by the previous paragraph. Let m∈Tm\in T; we show m+1∈Tm+1\in T. If n<m+1n<m+1 this is immediate, so assume m+1∈[n]m+1\in[n]; then m∈[n]m\in[n], since m<m+1m<m+1 by claim 5 of Properties of the Order on the Natural Numbers, hence m≤m+1m\le m+1 by claim 1 of that lemma, and m+1≤nm+1\le n, so m≤nm\le n by the transitivity of ≤\le in claim 1. Therefore Pm∈CperP_{m}\in C_{\mathrm{per}}, and by the recursion in claim 1 of Properties of Finite Sums the map Pm+1P_{m+1} is the pointwise sum Pm+∂m+1∂m+1uP_{m}+\partial_{m+1}\partial_{m+1}u, which lies in CperC_{\mathrm{per}} by Elementary Properties of Lattice-Periodic Functions (i). By Principle of Induction for the Natural Numbers with the inductive set TT we get T=NT=\mathbb{N}, and since n∈[n]n\in[n] this gives Pn∈CperP_{n}\in C_{\mathrm{per}}. By The Laplacian of a Twice Continuously Differentiable Function (i) the map Δu\Delta u is PnP_{n}.

Consequently u∣Qu|_{Q} and (Δu)∣Q(\Delta u)|_{Q} are measurable with respect to BQ\mathcal{B}_{Q} and belong to L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}), by Continuous Periodic Functions are Power-Integrable and Dense on the Torus (i); the same applies to (∂iu)∣Q(\partial_{i}u)|_{Q}, (∂i∂iu)∣Q(\partial_{i}\partial_{i}u)|_{Q} and ek∣Qe_{k}|_{Q} for every k∈Znk\in\mathbb{Z}^{n}, the last by The Trigonometric System on the Torus is Orthonormal (i).

Claim 5 (Moving one derivative at a time). Let u∈Cper2u\in C^{2}_{\mathrm{per}}, k∈Znk\in\mathbb{Z}^{n} and i∈[n]i\in[n]. Then

∫Tn(∂i∂iu)∣Q (ek∣Q) dx=−4π2ki2∫Tnu∣Q (ek∣Q) dx.\int_{\mathbb{T}^{n}}(\partial_{i}\partial_{i}u)|_{Q}\,\bigl(e_{k}|_{Q}\bigr)\,dx=-4\pi^{2}k_{i}^{2}\int_{\mathbb{T}^{n}}u|_{Q}\,\bigl(e_{k}|_{Q}\bigr)\,dx .

By claim 1 of Elementary Properties of the Weak Partial Derivative on the Torus, applied to u∈Cper1u\in C^{1}_{\mathrm{per}} and to ∂iu∈Cper1\partial_{i}u\in C^{1}_{\mathrm{per}} from claim 4, the class [(∂iu)∣Q][(\partial_{i}u)|_{Q}] is the ii-th weak partial derivative of [u∣Q][u|_{Q}] in L2(Tn)L^{2}(\mathbb{T}^{n}), and [(∂i∂iu)∣Q][(\partial_{i}\partial_{i}u)|_{Q}] is the ii-th weak partial derivative of [(∂iu)∣Q][(\partial_{i}u)|_{Q}] in L2(Tn)L^{2}(\mathbb{T}^{n}).

The map ∂iek\partial_{i}e_{k} lies in Cper1C^{1}_{\mathrm{per}}: it is the scalar multiple (−2πki)ek(i)(-2\pi k_{i})e_{k^{(i)}} of ek(i)∈Cper1e_{k^{(i)}}\in C^{1}_{\mathrm{per}}, so Elementary Properties of Lattice-Periodic Functions (i) applies. Now apply claim 3 of Elementary Properties of the Weak Partial Derivative on the Torus twice: first with the class [(∂iu)∣Q][(\partial_{i}u)|_{Q}], its weak derivative [(∂i∂iu)∣Q][(\partial_{i}\partial_{i}u)|_{Q}], the representatives (∂iu)∣Q(\partial_{i}u)|_{Q} and (∂i∂iu)∣Q(\partial_{i}\partial_{i}u)|_{Q}, and the test function ek∈Cper1e_{k}\in C^{1}_{\mathrm{per}}; then with the class [u∣Q][u|_{Q}], its weak derivative [(∂iu)∣Q][(\partial_{i}u)|_{Q}], the representatives u∣Qu|_{Q} and (∂iu)∣Q(\partial_{i}u)|_{Q}, and the test function ∂iek\partial_{i}e_{k}. This gives

∫Tn(∂iu)∣Q ((∂iek)∣Q) dx=−∫Tn(∂i∂iu)∣Q (ek∣Q) dx\int_{\mathbb{T}^{n}}(\partial_{i}u)|_{Q}\,\bigl((\partial_{i}e_{k})|_{Q}\bigr)\,dx=-\int_{\mathbb{T}^{n}}(\partial_{i}\partial_{i}u)|_{Q}\,\bigl(e_{k}|_{Q}\bigr)\,dx

and

∫Tnu∣Q ((∂i∂iek)∣Q) dx=−∫Tn(∂iu)∣Q ((∂iek)∣Q) dx.\int_{\mathbb{T}^{n}}u|_{Q}\,\bigl((\partial_{i}\partial_{i}e_{k})|_{Q}\bigr)\,dx=-\int_{\mathbb{T}^{n}}(\partial_{i}u)|_{Q}\,\bigl((\partial_{i}e_{k})|_{Q}\bigr)\,dx .

Combining the two, the left-hand side of the first display equals the negative of the left-hand side of the second, so

∫Tn(∂i∂iu)∣Q (ek∣Q) dx=∫Tnu∣Q ((∂i∂iek)∣Q) dx.\int_{\mathbb{T}^{n}}(\partial_{i}\partial_{i}u)|_{Q}\,\bigl(e_{k}|_{Q}\bigr)\,dx=\int_{\mathbb{T}^{n}}u|_{Q}\,\bigl((\partial_{i}\partial_{i}e_{k})|_{Q}\bigr)\,dx .

By claim 2 the map ∂i∂iek\partial_{i}\partial_{i}e_{k} is the scalar multiple (−4π2ki2)ek(-4\pi^{2}k_{i}^{2})e_{k}, so the integrand on the right is (−4π2ki2) u∣Q (ek∣Q)(-4\pi^{2}k_{i}^{2})\,u|_{Q}\,(e_{k}|_{Q}) at every point of QQ. The product u∣Q (ek∣Q)u|_{Q}\,(e_{k}|_{Q}) is integrable, being a product of two members of L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}) by claim 4 and L²(μ) Is a Real Hilbert Space (i); so Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions (ii), used with the single summand u∣Q (ek∣Q)u|_{Q}\,(e_{k}|_{Q}) and the constant −4π2ki2-4\pi^{2}k_{i}^{2}, moves that constant out of the integral and yields the assertion.

Claim 6 (Clause 3). Let u∈Cper2u\in C^{2}_{\mathrm{per}} and k∈Znk\in\mathbb{Z}^{n}; the membership assertions of clause 3 are claim 4. By L²(μ) Is a Real Hilbert Space (i), applied to the measure space (Q,BQ,λQ)(Q,\mathcal{B}_{Q},\lambda_{Q}) of The Flat Torus: Standing Notation (iii), both inner products in clause 3 are the integrals over Tn\mathbb{T}^{n} of the corresponding pointwise products.

At every point of QQ one has (Δu)∣Q (ek∣Q)=∑i=1n(∂i∂iu)∣Q (ek∣Q)(\Delta u)|_{Q}\,(e_{k}|_{Q})=\sum_{i=1}^{n}(\partial_{i}\partial_{i}u)|_{Q}\,(e_{k}|_{Q}), by The Laplacian of a Twice Continuously Differentiable Function (i) and the homogeneity of claim 3 of Properties of Finite Sums. Each summand is integrable, being a product of two members of L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}) by claim 4 and L²(μ) Is a Real Hilbert Space (i); so Linearity of the Lebesgue Integral over a Finite Sum of Integrable Functions (ii) gives

∫Tn(Δu)∣Q (ek∣Q) dx=∑i=1n∫Tn(∂i∂iu)∣Q (ek∣Q) dx.\int_{\mathbb{T}^{n}}(\Delta u)|_{Q}\,\bigl(e_{k}|_{Q}\bigr)\,dx=\sum_{i=1}^{n}\int_{\mathbb{T}^{n}}(\partial_{i}\partial_{i}u)|_{Q}\,\bigl(e_{k}|_{Q}\bigr)\,dx .

By claim 5 each term equals −4π2ki2∫Tnu∣Q (ek∣Q) dx-4\pi^{2}k_{i}^{2}\int_{\mathbb{T}^{n}}u|_{Q}\,(e_{k}|_{Q})\,dx, so by the homogeneity of claim 3 of Properties of Finite Sums the right-hand side is

(−4π2∫Tnu∣Q (ek∣Q) dx)∑i=1nki2,\Bigl(-4\pi^{2}\int_{\mathbb{T}^{n}}u|_{Q}\,\bigl(e_{k}|_{Q}\bigr)\,dx\Bigr)\sum_{i=1}^{n}k_{i}^{2},

and ∑i=1nki2=∥k∥2\sum_{i=1}^{n}k_{i}^{2}=\lVert k\rVert^{2} by 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. This is clause 3.

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