definition 12.109 Weyl system

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definition 12.109: Weyl system12.109definition 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 statement12.111theorem A.579: Stone–von NeumannA.579theorem 12.114: Stone–von Neumann12.114definition 12.41: The operator classes12.41definition 6.6: Continuous map6.6lemma A.255: Smoothed vectors lie in the domainA.255lemma A.581: Composition lawA.581lemma A.582: Joint strong continuityA.582proposition A.256: DensityA.256proposition 12.65: Exponential of a bounded self-adjoint operator12.65proposition 12.67: The generator is symmetric, and generates the motion12.67theorem A.253: StoneA.253theorem 25.34: Stone–von Neumann25.34definition 12.35: Bounded operator; operator norm12.35proposition 12.37: B(H) is a Banach algebra12.37corollary 12.76: Position and momentum are unbounded, and cannot be everywhere defined12.76corollary 25.30: The relation cannot be realized by matrices25.30proof : ch:10-hilbert-spaces@proof-37prooftheorem 12.59: Spectral theorem for a bounded self-adjoint operator12.59proof : ch:10-hilbert-spaces@prooflink-3proofproof : ch:10-hilbert-spaces@proof-51proofequation 12.71: eq:hilbert-weyl-relation12.71definition A.585: The Gaussian average of the Weyl operatorsA.585example 12.11: The function space L^212.11proposition A.592: The vacuum of the Schrödinger systemA.592proof : ch:10-hilbert-spaces@proof-50proofdefinition 12.90: Self-adjoint family; commutant; irreducibility12.90proof : app:A-long-proofs@proof-357prooftheorem 12.91: Schur's lemma, commutant form12.91

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typedirectionnode provenancewhere
depends_on Strongly continuous one-parameter unitary group declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3009
depends_on The canonical commutation relation admits no bounded solution declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3009
depends_on Stone declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3009
depends_on Commutator of the momentum with a function of the position declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3111
depends_on Weyl operator declared appendices/A-long-proofs.tex:27740
depends_on The Schrödinger system declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3038
depends_on The Weyl relation is a covariance statement declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3051
depends_on Stone–von Neumann declared appendices/A-long-proofs.tex:27706
depends_on Stone–von Neumann declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3196