example 12.56 Multiplication by the coordinate: spectrum without eigenvectors

open in the book · parts/02-mathematical-methods/10-hilbert-spaces.tex:1492 · p. 429

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example 12.56: Multiplication by the coordinate: spectrum without eigenvectors12.56definition 12.50: Point, continuous and residual spectrum12.50example 12.11: The function space L^212.11theorem 12.55: The spectrum of a self-adjoint operator is real12.55proof : ch:10-hilbert-spaces@proof-31proofcorollary 12.19: Double complement; the density criterion12.19definition 12.49: Resolvent set; spectrum12.49definition 12.105: Generalized eigenvector12.105proposition 12.51: The three cases are exclusive and exhaustive12.51definition 12.2: Hilbert space12.2definition 5.18: Inner product5.18example 12.81: Momentum on a finite interval: a circle of self-adjoint momenta12.81example 12.25: Orthogonal polynomials12.25example 12.110: The Schrödinger system12.110example 12.104: The Schwartz triple12.104example 12.98: Two particles in three-dimensional space12.98proposition 12.102: Neither plane waves nor deltas are in L^212.102theorem 12.12: Riesz–Fischer12.12definition 12.41: The operator classes12.41theorem 12.54: The spectrum is compact and non-empty12.54theorem A.238: Spectral theorem, both formsA.238theorem 12.59: Spectral theorem for a bounded self-adjoint operator12.59proof : ch:10-hilbert-spaces@proof-30proof

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depends_on Point, continuous and residual spectrum declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1504
depends_on The function space $L^{2}$ declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1504
depends_on The spectrum of a self-adjoint operator is real declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1504
proves ch:10-hilbert-spaces@proof-31 declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1508