TheoremBase

The Laplacian of the Trigonometric System, and the Fourier Coefficients of a Laplacian on the Torus

Each member of the trigonometric system is twice continuously differentiable and is an eigenfunction of the Laplacian with eigenvalue minus four pi squared times the squared length of its frequency; consequently the Fourier coefficients of the Laplacian of a twice continuously differentiable periodic function are those of the function multiplied by that eigenvalue.

Statement

We work in the setting of The Flat Torus: Standing Notation, used here with a natural number nn satisfying 1≤n1\le n; the initial segments [n][n], Euclidean space Rn\mathbb{R}^{n} with its norm ∥ ⋅ ∥\lVert\,\cdot\,\rVert, the integer lattice Zn\mathbb{Z}^{n}, the cell QQ, the class L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}) and the space L2(Tn)L^{2}(\mathbb{T}^{n}) with the class map [ ⋅ ][\,\cdot\,], the periodic classes CperC_{\mathrm{per}}, Cper1C^{1}_{\mathrm{per}} and Cper2C^{2}_{\mathrm{per}}, the restriction u∣Qu|_{Q}, and the partial derivatives ∂i\partial_{i}, the iterated partial derivatives and the classes CkC^{k} on a Euclidean open set are the ones fixed there; Rn\mathbb{R}^{n} is open in itself by claim 1 of Euclidean Space Is Open in Itself, so those calculus notions apply to maps on all of Rn\mathbb{R}^{n}. Let π\pi be the real number of The Number Pi (i) (the wrapping map of The Flat Torus: Standing Notation (ii) is not used here), let 2=1+12=1+1 and 4=2+24=2+2, and for a real number tt write t2=ttt^{2}=tt. Let ⟨ ⋅ ,⋅ ⟩L2\langle\,\cdot\,,\cdot\,\rangle_{L^{2}} be the inner product of L2(Tn)L^{2}(\mathbb{T}^{n}). Let eke_{k} for k∈Znk\in\mathbb{Z}^{n} be the trigonometric system on Tn\mathbb{T}^{n} and Ek=[ ek∣Q ]E_{k}=[\,e_{k}|_{Q}\,] its classes, as introduced in The Trigonometric System on the Torus is Orthonormal (i). Let Δ\Delta denote the Laplacian of a map of class C2C^{2} on Rn\mathbb{R}^{n}. Then the following hold.

1. (The trigonometric system is twice continuously differentiable) Let k∈Znk\in\mathbb{Z}^{n} and i∈[n]i\in[n]. Then eke_{k} is of class C2C^{2} on Rn\mathbb{R}^{n} and belongs to Cper2C^{2}_{\mathrm{per}}, and

∂i∂iek(x)=−4π2ki2 ek(x)for every x∈Rn.\partial_{i}\partial_{i}e_{k}(x)=-4\pi^{2}k_{i}^{2}\,e_{k}(x)\qquad\text{for every }x\in\mathbb{R}^{n}.

2. (Eigenfunctions of the Laplacian) Let k∈Znk\in\mathbb{Z}^{n}. Then

Δek(x)=−4π2∥k∥2 ek(x)for every x∈Rn.\Delta e_{k}(x)=-4\pi^{2}\lVert k\rVert^{2}\,e_{k}(x)\qquad\text{for every }x\in\mathbb{R}^{n}.

3. (Fourier coefficients of a Laplacian) Let u∈Cper2u\in C^{2}_{\mathrm{per}}. Then uu and Δu\Delta u belong to CperC_{\mathrm{per}}, their restrictions u∣Qu|_{Q} and (Δu)∣Q(\Delta u)|_{Q} belong to L2(Tn)\mathcal{L}^{2}(\mathbb{T}^{n}), and for every k∈Znk\in\mathbb{Z}^{n}

⟨ [ (Δu)∣Q ], Ek ⟩L2=−4π2∥k∥2 ⟨ [ u∣Q ], Ek ⟩L2.\bigl\langle\,[\,(\Delta u)|_{Q}\,],\,E_{k}\,\bigr\rangle_{L^{2}} =-4\pi^{2}\lVert k\rVert^{2}\,\bigl\langle\,[\,u|_{Q}\,],\,E_{k}\,\bigr\rangle_{L^{2}} .

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