theorem A.579 Stone–von Neumann

open in the book · appendices/A-long-proofs.tex:27692 · p. 3069

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theorem A.579: Stone–von NeumannA.579definition 12.90: Self-adjoint family; commutant; irreducibility12.90definition 12.109: Weyl system12.109example 12.110: The Schrödinger system12.110proof : app:A-long-proofs@proof-357proofdefinition 12.41: The operator classes12.41definition 12.88: Reducing subspace12.88proposition A.589: Cyclic subspaces and the rank of the averageA.589theorem 12.91: Schur's lemma, commutant form12.91theorem 12.114: Stone–von Neumann12.114definition 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.580proposition 12.111: The Weyl relation is a covariance statement12.111example 12.11: The function space L^212.11proposition A.592: The vacuum of the Schrödinger systemA.592

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typedirectionnode provenancewhere
depends_on Self-adjoint family; commutant; irreducibility declared appendices/A-long-proofs.tex:27706
depends_on Weyl system declared appendices/A-long-proofs.tex:27706
depends_on The Schrödinger system declared appendices/A-long-proofs.tex:27706
proves app:A-long-proofs@proof-357 declared appendices/A-long-proofs.tex:28488