proposition 12.111 The Weyl relation is a covariance statement

open in the book · parts/02-mathematical-methods/10-hilbert-spaces.tex:3041 · p. 446

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proposition 12.111: The Weyl relation is a covariance statement12.111definition 12.109: Weyl system12.109proposition 12.67: The generator is symmetric, and generates the motion12.67theorem 12.66: Stone12.66corollary 12.112: Commutator of the momentum with a function of the position12.112proof : ch:10-hilbert-spaces@proof-50proofdefinition 12.64: Strongly continuous one-parameter unitary group12.64theorem 12.75: The canonical commutation relation admits no bounded solution12.75definition A.580: Weyl operatorA.580example 12.110: The Schrödinger system12.110theorem A.579: Stone–von NeumannA.579theorem 12.114: Stone–von Neumann12.114lemma A.257: Integrated form of the equation of motionA.257proposition A.263: The two constructions are inverseA.263proposition A.259: The generator is self-adjointA.259theorem A.253: StoneA.253proof : ch:10-hilbert-spaces@proof-34proofproposition 12.65: Exponential of a bounded self-adjoint operator12.65theorem 12.59: Spectral theorem for a bounded self-adjoint operator12.59theorem 25.34: Stone–von Neumann25.34proof : ch:10-hilbert-spaces@prooflink-3proofproof : ch:10-hilbert-spaces@proof-51proof

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typedirectionnode provenancewhere
depends_on Weyl system declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3051
depends_on The generator is symmetric, and generates the motion declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3051
depends_on Stone declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3051
depends_on Commutator of the momentum with a function of the position declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3111
proves ch:10-hilbert-spaces@proof-50 declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3055