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Eigenspaces of the diagonal operator

Statement

Assume the Axiom of Countable Choice (The Axiom of Countable Choice (ACω)). Let H be a complex Hilbert space (Hilbert space), let (en)n∈N be a complete orthonormal family of H (Orthonormal families, complete orthonormal systems and Hilbert bases), let (λn)n∈N⊆R, and let A be the self-adjoint diagonal operator of Diagonal adjoint and graph-core lemma: D(A)={x∈H:∑nλn2∣⟨x,en⟩∣2<∞},Ax=∑nλn⟨x,en⟩en. Then:

(a) for every λ∈R the eigenspace of A at λ is the closed linear span of the basis vectors carrying the eigenvalue λ: ker⁡(A−λI)=span⁡‾{en:λn=λ}; in particular λ is an eigenvalue of A exactly when λ=λn for some n;

(b) if λm≠λn whenever m≠n, then ker⁡(A−λnI)=Cen for every n: every eigenspace is one-dimensional with eigenvector en, the eigenspaces are pairwise orthogonal, and every nonzero eigenvector of A is a nonzero multiple of some en;

(c) in the situation of (b) the linear span of all eigenspaces of A is span⁡{en:n∈N}, which is dense in H.

Facts & Assumptions

Given: a complex Hilbert space H; a complete orthonormal family (en)n∈N of H; real numbers λn; the diagonal operator A displayed in the Statement; a real number λ.

[F1]

D(A) and A are as displayed, A is self-adjoint, Aen=λnen for every n, and the algebraic span D0=span⁡{en:n∈N} is a core for A (Diagonal adjoint and graph-core lemma clauses (b), (d), (e)).

[F2]

⟨ei,ej⟩=δij; a series ∑nanen converges in H exactly when ∑n∣an∣2<∞, and then ∥∑nanen∥2=∑n∣an∣2; every x∈H satisfies x=∑n⟨x,en⟩en and ∑n∣⟨x,en⟩∣2=∥x∥2; and the coefficients of a convergent expansion in the family are unique (Orthonormal families, complete orthonormal systems and Hilbert bases, Parseval equivalences for an orthonormal family).

Proof

Given: the Hilbert space H, the complete orthonormal family (en), the real numbers λn, the diagonal operator A of [F1], and a real number λ.

1.1givenF1F2

[One inclusion] Let x∈D(A) with coefficients cn=⟨x,en⟩ satisfy Ax=λx. By [F1] both series ∑nλncnen and ∑nλcnen converge, so their difference ∑n(λn−λ)cnen=0 converges; its coefficients in the orthonormal family are (λn−λ)cn, and by the uniqueness of coefficients in [F2] all of them vanish. Hence cn=0 whenever λn≠λ, so x=∑n:λn=λcnen lies in the closed linear span of {en:λn=λ}.

1.2givenF1F2algebra

[The converse inclusion] Conversely let I:={n:λn=λ} and let x=∑n∈Icnen be an element of the closed linear span of {en:n∈I}, so that ∑n∈I∣cn∣2<∞ and the series converges by [F2]. Then ∑nλn2∣⟨x,en⟩∣2=∑n∈Iλ2∣cn∣2<∞, so x∈D(A) by [F1], and Ax=∑n∈Iλcnen=λx.

2.1step 1.1step 1.2given

[Clause (a)] Steps 1.1 and 1.2 give ker⁡(A−λI)=span⁡‾{en:λn=λ} for every real λ, and this span is nonzero exactly when λ∈{λn:n∈N} because en≠0.

3.1step 2.1F1F2

[Clause (b)] Assume the λn are pairwise distinct and let λ=λk. Then {n:λn=λ}={k}, so step 2.1 gives ker⁡(A−λkI)=Cek; every such eigenspace is one-dimensional with eigenvector ek≠0, and distinct eigenspaces are orthogonal because ⟨em,ek⟩=0 for m≠k by [F2]. If x≠0 satisfies Ax=λx, then λ=λk for some k by step 2.1 and x∈Cek; conversely every nonzero multiple of ek is an eigenvector by [F1].

4.1step 3.1F1∎

[Clause (c)] The span of the union of the eigenspaces contains every en, hence contains D0=span⁡{en}, which is dense in H by [F1]; therefore the span of the eigenspaces is dense.

Depends on

Dependency tree · 2 levels

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