theorem 12.59 Spectral theorem for a bounded self-adjoint operator

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theorem 12.59: Spectral theorem for a bounded self-adjoint operator12.59definition 12.58: Projection-valued measure12.58proposition 12.43: Norm of a self-adjoint operator12.43theorem 12.55: The spectrum of a self-adjoint operator is real12.55definition 12.60: Functional calculus12.60theorem 12.107: Nuclear spectral theorem12.107theorem 12.91: Schur's lemma, commutant form12.91theorem 12.66: Stone12.66proof : ch:10-hilbert-spaces@prooflink-2proofdefinition 12.41: The operator classes12.41proposition 12.21: Characterization of orthogonal projections12.21lemma A.247: Integration against a projection-valued measureA.247theorem A.238: Spectral theorem, both formsA.238proposition 12.42: Elementary consequences12.42proposition 12.39: Algebra of the adjoint; the C^\ast identity12.39lemma A.232: AttainmentA.232lemma A.239: The norm of a self-adjoint operator lies in its spectrumA.239theorem A.229: Hilbert–SchmidtA.229theorem 12.44: Hilbert–Schmidt: compact self-adjoint operators12.44proof : ch:10-hilbert-spaces@proof-23proofcorollary 12.19: Double complement; the density criterion12.19theorem 12.54: The spectrum is compact and non-empty12.54example 12.56: Multiplication by the coordinate: spectrum without eigenvectors12.56proof : ch:10-hilbert-spaces@proof-30proofproposition 12.61: Uniqueness of the continuous functional calculus12.61definition 12.103: Gelfand triple12.103definition 12.105: Generalized eigenvector12.105proof : ch:10-hilbert-spaces@prooflink-5proofdefinition 12.90: Self-adjoint family; commutant; irreducibility12.90proposition 12.89: Reduction is commutation12.89proposition A.591: Any two irreducible Weyl systems are equivalentA.591theorem 12.114: Stone–von Neumann12.114proof : ch:10-hilbert-spaces@proof-44proofdefinition 12.64: Strongly continuous one-parameter unitary group12.64proposition 12.65: Exponential of a bounded self-adjoint operator12.65corollary 12.112: Commutator of the momentum with a function of the position12.112definition 12.109: Weyl system12.109proposition 12.67: The generator is symmetric, and generates the motion12.67proposition 12.111: The Weyl relation is a covariance statement12.111theorem 25.34: Stone–von Neumann25.34neighborhood truncated

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typedirectionnode provenancewhere
depends_on Projection-valued measure declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1620
depends_on Norm of a self-adjoint operator declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1620
depends_on The spectrum of a self-adjoint operator is real declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1620
depends_on Functional calculus declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1658
depends_on Nuclear spectral theorem declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2901
depends_on Schur's lemma, commutant form declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2490
depends_on Stone declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1825
proves ch:10-hilbert-spaces@prooflink-2 declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1642