Bourbaki

Example

Tag 037B, permanent. Cite it as [Bourbaki, Tag 037B].

Théories spectrales, chapter IV, § 5. Opérateurs partiels normaux et théorème spectral

Let n∈Nn\in \mathbf{N}. Let U be an open set in Rn\mathbf{R}^n. Endow U with Lebesgue measure, denoted by μ\mu. Let Δ be the scalar differential operator −∑i=1n∂i2-\sum^n_{i=1}\partial_i^2 on U. The partial operator Δ−\Delta_- with domain D(U)\mathscr{D}(U) defined by φ↦Δ(φ)\varphi \mapsto \Delta (\varphi ) is closable (Proposition 13 of IV, p. 242) and symmetric (IV, p. 243). It is positive, since for every φ∈D\varphi \in \mathscr{D}(U), we have

⟨φ∣Δ−(φ)⟩=∫Uφ‾Δ(φ)dμ=−∑i=1n∫Uφ∂i2φdμ \langle \varphi |\Delta_-(\varphi )\rangle =\int_U\overline{\varphi}\Delta (\varphi )d\mu=-\sum_{i=1}^n\int_U\varphi \partial_i^2\varphi d\mu
=∑i=1n∫U∂iφ∂iφdμ=∫U∑i=1n∣∂iφ∣2dμ⩾0 =\sum_{i=1}^n\int_U\partial_i\varphi \partial_i\varphi d\mu=\int_U\sum_{i=1}^n|\partial_i\varphi |^2d\mu\geqslant 0

We denote by ΔD\Delta_D the Friedrichs extension of the positive symmetric partial operator Δ−(\Delta_-(IV, p. 295, Example); it is a Laplacian on U, called the Dirichlet Laplacian on U.

Let qq be the positive partial form associated with ΔD\Delta_D. The domain of qq is the Hilbert space completion of D(U)\mathscr{D}(U) for the positive Hermitian form defined by

(φ1,φ2)↦∫Uφ‾1φ2+∑i=1n∫U∂iφ1‾∂iφ2 (\varphi_1, \varphi_2)\mapsto \int_U\overline{\varphi}_1\varphi_2+\sum_{i=1}^n\int_U\overline{\partial_i\varphi_1}\partial_i\varphi_2

for every (φ1,φ2)∈D(U)×D(U)(\varphi_1, \varphi_2)\in \mathscr{D}(U)\times \mathscr{D}(U). In other words, the domain of qq is the Sobolev space H01(U)H^1_0(U) (No.o14^o14 of IV, p. 221).

*Suppose that U is bounded. The canonical injection of H01(U)H^1_0(U) into L2(U)L^2(U) is compact; the Dirichlet Laplacian on U is therefore an operator with compact resolvent (Corollary of Proposition 20). Since the Hilbert space H01(U)H^1_0(U) is of countable type (Proposition 20 of IV, p. 222), and since the image of ΔD\Delta_D is of infinite dimension, there exists an increasing sequence (λn)n⩾0(\lambda_n)_{n\geqslant 0} of real numbers tending to +∞+\infty and an orthonormal basis (fn)n∈N(f_n)_{n\in\mathbf{N}} of L2L^2(U), whose elements belong to the domain of ΔD\Delta_D, such that ΔD(fn)=λnfn\Delta_D(f_n) =\lambda_nf_n for every n∈Nn\in \mathbf{N}. One can prove ("Weyl's law") that as T tends to +∞+\infty, one has

∑n∈N1∼cn(2π)nmTn/2 \sum_{n\in\mathbf{N}}1\sim \frac{c_n}{(2\pi)^n}mT^{n/2}
λn⩽T\lambda_n\leqslant T

where cn=πn/2/Γ(1+n/2)c_n=\pi^{n/2}/\Gamma (1 +n/2) is the volume of the unit ball in Rn\mathbf{R}^n (INT, V, p. 101, § 8, no7^o7) and m>0m >0 is the Lebesgue measure of U.*

Bourbaki sets the proof directly after the statement, and the corpus does not separate them, so what is above is the statement and its proof together.

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Machine translation of the English, by gpt-5.4, gpt-5-6-mini, against glossary version 34. Not checked by a person. That model is a cut down version of the one the rest of this language was written by.