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Eigenspaces of the diagonal operator
Statement
Assume the Axiom of Countable Choice (The Axiom of Countable Choice ()). Let be a complex Hilbert space (Hilbert space), let be a complete orthonormal family of (Orthonormal families, complete orthonormal systems and Hilbert bases), let , and let be the self-adjoint diagonal operator of Diagonal adjoint and graph-core lemma: Then:
(a) for every the eigenspace of at is the closed linear span of the basis vectors carrying the eigenvalue : in particular is an eigenvalue of exactly when for some ;
(b) if whenever , then for every : every eigenspace is one-dimensional with eigenvector , the eigenspaces are pairwise orthogonal, and every nonzero eigenvector of is a nonzero multiple of some ;
(c) in the situation of (b) the linear span of all eigenspaces of is , which is dense in .
Facts & Assumptions
Given: a complex Hilbert space ; a complete orthonormal family of ; real numbers ; the diagonal operator displayed in the Statement; a real number .
and are as displayed, is self-adjoint, for every , and the algebraic span is a core for (Diagonal adjoint and graph-core lemma clauses (b), (d), (e)).
; a series converges in exactly when , and then ; every satisfies and ; 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 , the complete orthonormal family , the real numbers , the diagonal operator of [F1], and a real number .
[One inclusion] Let with coefficients satisfy . By [F1] both series and converge, so their difference converges; its coefficients in the orthonormal family are , and by the uniqueness of coefficients in [F2] all of them vanish. Hence whenever , so lies in the closed linear span of .
[The converse inclusion] Conversely let and let be an element of the closed linear span of , so that and the series converges by [F2]. Then , so by [F1], and .
[Clause (a)] Steps 1.1 and 1.2 give for every real , and this span is nonzero exactly when because .
[Clause (b)] Assume the are pairwise distinct and let . Then , so step 2.1 gives ; every such eigenspace is one-dimensional with eigenvector , and distinct eigenspaces are orthogonal because for by [F2]. If satisfies , then for some by step 2.1 and ; conversely every nonzero multiple of is an eigenvector by [F1].
[Clause (c)] The span of the union of the eigenspaces contains every , hence contains , which is dense in by [F1]; therefore the span of the eigenspaces is dense.
Depends on
Dependency tree · 2 levels
Sources
- G. Teschl, Mathematical Methods in Quantum Mechanics, 1st edition 2009, §2.4 pp. 73-74 (eigenvalues, eigenspaces and the multiplication-operator example)
- MIT 8.05 Quantum Physics II (Fall 2013), Chapter 6 'Quantum Dynamics', §1 pp. 1-9 (non-degeneracy of the oscillator ground state and the ladder spectrum)