theorem 109.21 Wightman reconstruction

open in the book · parts/11-qft-standard-model/11-axiomatic-qft.tex:635 · p. 2300

Rests on

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theorem 109.21: Wightman reconstruction109.21definition 109.19: Wightman functions109.19proposition 109.20: Properties of the Wightman functions109.20theorem 109.4: Haag109.4proof : ch:11-axiomatic-qft@proof-5proofaxiom 109.13: Covariance109.13axiom 109.12: Fields109.12axiom 109.14: Local commutativity109.14axiom 109.10: Spectrum condition109.10axiom 109.9: Relativistic states109.9axiom 109.11: Unique vacuum109.11proposition 109.79: Reflection positivity is Hilbert positivity109.79theorem 109.28: Bargmann–Hall–Wightman; imported109.28proof : ch:11-axiomatic-qft@proof-4proofequation 109.1: eq:axqft-free-wightman109.1theorem 109.26: Analyticity in the forward tube109.26corollary 109.5: The interaction picture does not exist109.5proof : ch:11-axiomatic-qft@proof-2proof

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typedirectionnode provenancewhere
cites Quantum Field Theory in Terms of Vacuum Expectation Values derived parts/11-qft-standard-model/11-axiomatic-qft.tex:644
depends_on Wightman functions declared parts/11-qft-standard-model/11-axiomatic-qft.tex:645
depends_on Properties of the Wightman functions declared parts/11-qft-standard-model/11-axiomatic-qft.tex:645
depends_on Haag declared parts/11-qft-standard-model/11-axiomatic-qft.tex:202
proves ch:11-axiomatic-qft@proof-5 declared parts/11-qft-standard-model/11-axiomatic-qft.tex:648