theorem 12.114 Stone–von Neumann

open in the book · parts/02-mathematical-methods/10-hilbert-spaces.tex:3184 · p. 447

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theorem 12.114: Stone–von Neumann12.114definition 12.90: Self-adjoint family; commutant; irreducibility12.90definition 12.109: Weyl system12.109theorem 12.91: Schur's lemma, commutant form12.91definition 12.41: The operator classes12.41definition 12.88: Reducing subspace12.88proposition A.589: Cyclic subspaces and the rank of the averageA.589theorem A.579: Stone–von NeumannA.579definition 12.64: Strongly continuous one-parameter unitary group12.64theorem 12.75: The canonical commutation relation admits no bounded solution12.75theorem 12.66: Stone12.66corollary 12.112: Commutator of the momentum with a function of the position12.112definition A.580: Weyl operatorA.580example 12.110: The Schrödinger system12.110proposition 12.111: The Weyl relation is a covariance statement12.111proposition 12.89: Reduction is commutation12.89theorem 12.59: Spectral theorem for a bounded self-adjoint operator12.59proposition A.591: Any two irreducible Weyl systems are equivalentA.591proof : ch:10-hilbert-spaces@proof-44proof

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depends_on Self-adjoint family; commutant; irreducibility declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3196
depends_on Weyl system declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3196
depends_on Schur's lemma, commutant form declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3196