proposition 12.106 The plane wave is a generalized momentum eigenvector

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proposition 12.106: The plane wave is a generalized momentum eigenvector12.106definition 12.105: Generalized eigenvector12.105equation 12.54: eq:hilbert-momentum-operator12.54example 12.104: The Schwartz triple12.104example A.283: Momentum on the lineA.283proof : ch:10-hilbert-spaces@proof-49proofdefinition 12.103: Gelfand triple12.103definition 12.50: Point, continuous and residual spectrum12.50theorem A.279: Gelfand–MaurinA.279theorem 12.107: Nuclear spectral theorem12.107example 12.11: The function space L^212.11proposition 12.102: Neither plane waves nor deltas are in L^212.102

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depends_on Generalized eigenvector declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2867
depends_on eq:hilbert-momentum-operator declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2867
depends_on The Schwartz triple declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2867
depends_on Momentum on the line declared appendices/A-long-proofs.tex:14226
proves ch:10-hilbert-spaces@proof-49 declared parts/02-mathematical-methods/10-hilbert-spaces.tex:2871