theorem 12.66 Stone

open in the book · parts/02-mathematical-methods/10-hilbert-spaces.tex:1814 · p. 433

Rests on

Supports

Neighborhood

Every logical edge within two steps of this node.

theorem 12.66: Stone12.66definition 12.64: Strongly continuous one-parameter unitary group12.64proposition 12.65: Exponential of a bounded self-adjoint operator12.65theorem 12.59: Spectral theorem for a bounded self-adjoint operator12.59corollary 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 Neumann25.34proof : ch:10-hilbert-spaces@prooflink-3proofdefinition 12.41: The operator classes12.41definition 6.6: Continuous map6.6definition A.580: Weyl operatorA.580lemma A.255: Smoothed vectors lie in the domainA.255lemma A.581: Composition lawA.581lemma A.582: Joint strong continuityA.582proposition A.256: DensityA.256theorem A.253: StoneA.253proposition 12.37: B(H) is a Banach algebra12.37proposition 12.39: Algebra of the adjoint; the C^\ast identity12.39proof : ch:10-hilbert-spaces@proof-33proofdefinition 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 form12.91proof : ch:10-hilbert-spaces@prooflink-2proofproof : ch:10-hilbert-spaces@proof-51prooftheorem 12.75: The canonical commutation relation admits no bounded solution12.75example 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.259proof : ch:10-hilbert-spaces@proof-34proofproof : ch:10-hilbert-spaces@proof-50proofequation 25.33: eq:pq-ccr25.33lemma 25.39: The low-degree images are forced25.39neighborhood truncated

Edges

typedirectionnode provenancewhere
depends_on Strongly continuous one-parameter unitary group declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1825
depends_on Exponential of a bounded self-adjoint operator declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1825
depends_on Spectral theorem for a bounded self-adjoint operator declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1825
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 system declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3009
depends_on The generator is symmetric, and generates the motion declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1849
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 parts/03-classical-mechanics/08-poisson-quantum-bridge.tex:1272
proves ch:10-hilbert-spaces@prooflink-3 declared parts/02-mathematical-methods/10-hilbert-spaces.tex:1897