theorem 12.75 The canonical commutation relation admits no bounded solution

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theorem 12.75: The canonical commutation relation admits no bounded solution12.75definition 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 matrices25.30definition 12.109: Weyl system12.109proof : ch:10-hilbert-spaces@proof-37proofdefinition 5.37: Linear transformation5.37definition 5.19: Norm5.19definition 12.45: Continuous linear functional; the dual12.45definition 12.88: Reducing subspace12.88definition 12.49: Resolvent set; spectrum12.49proposition 12.36: Boundedness is continuity12.36proposition 12.8: Absolutely convergent series test12.8lemma A.240: Spectral mapping for polynomialsA.240proposition 12.65: Exponential of a bounded self-adjoint operator12.65proposition 12.61: Uniqueness of the continuous functional calculus12.61proposition 12.39: Algebra of the adjoint; the C^\ast identity12.39proposition 12.52: Neumann series; the spectrum is bounded12.52theorem 12.38: Existence and uniqueness of the adjoint12.38proof : ch:10-hilbert-spaces@proof-19prooftheorem 12.74: Hellinger–Toeplitz12.74proof : ch:10-hilbert-spaces@proof-38proofequation 25.33: eq:pq-ccr25.33proof : ch:08-poisson-quantum-bridge@proof-12proofdefinition 12.64: Strongly continuous one-parameter unitary group12.64theorem 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 Neumann12.114

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typedirectionnode provenancewhere
depends_on Bounded operator; operator norm declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2055
depends_on $\mathcal{B}(\mathcal{H})$ is a Banach algebra declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2055
depends_on Position and momentum are unbounded, and cannot be everywhere defined declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2091
depends_on The relation cannot be realized by matrices declared parts/03-classical-mechanics/08-poisson-quantum-bridge.tex:1117
depends_on Weyl system declared parts/02-mathematical-methods/10-hilbert-spaces.tex:3009
proves ch:10-hilbert-spaces@proof-37 declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2058