proposition 109.20 Properties of the Wightman functions

open in the book · parts/11-qft-standard-model/11-axiomatic-qft.tex:550 · p. 2299

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proposition 109.20: Properties of the Wightman functions109.20axiom 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; imported109.28theorem 109.21: Wightman reconstruction109.21proof : ch:11-axiomatic-qft@proof-4prooftheorem 109.54: Källén–Lehmann109.54theorem 109.46: Existence of the PCT operator109.46corollary 109.45: Locality implies PCT109.45theorem 109.34: Reeh–Schlieder109.34proposition 109.23: Uniqueness of the vacuum equals clustering109.23equation 106.30: eq:pathint-reflection-positivity106.30theorem 109.78: Osterwalder–Schrader109.78proposition 109.83: Mass gap and correlation length109.83proof : ch:11-axiomatic-qft@proof-28proofdefinition 109.27: The complex Lorentz group109.27theorem 109.26: Analyticity in the forward tube109.26corollary 109.43: Total inversion is automatic109.43theorem 109.49: Spin and statistics109.49proof : ch:11-axiomatic-qft@proof-9proofdefinition 109.19: Wightman functions109.19theorem 109.4: Haag109.4proof : ch:11-axiomatic-qft@proof-5proof

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typedirectionnode provenancewhere
depends_on Covariance declared parts/11-qft-standard-model/11-axiomatic-qft.tex:581
depends_on Fields declared parts/11-qft-standard-model/11-axiomatic-qft.tex:581
depends_on Local commutativity declared parts/11-qft-standard-model/11-axiomatic-qft.tex:581
depends_on Spectrum condition declared parts/11-qft-standard-model/11-axiomatic-qft.tex:581
depends_on Relativistic states declared parts/11-qft-standard-model/11-axiomatic-qft.tex:581
depends_on Unique vacuum declared parts/11-qft-standard-model/11-axiomatic-qft.tex:581
depends_on Reflection positivity is Hilbert positivity declared parts/11-qft-standard-model/11-axiomatic-qft.tex:2475
depends_on Bargmann–Hall–Wightman; imported declared parts/11-qft-standard-model/11-axiomatic-qft.tex:937
depends_on Wightman reconstruction declared parts/11-qft-standard-model/11-axiomatic-qft.tex:645
proves ch:11-axiomatic-qft@proof-4 declared parts/11-qft-standard-model/11-axiomatic-qft.tex:585