theorem 105.25 Number of physical phases

open in the book · parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2069 · p. 2134

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theorem 105.25: Number of physical phases105.25equation 104.46: eq:ewh-yukawa-lagrangian104.46proposition 105.27: When CP violation is possible105.27proof : ch:07-discrete-symmetries-cpt@proof-20proofproposition 104.61: The couplings are the masses divided by v104.61proposition 104.42: The sources of custodial violation104.42theorem 104.38: Masses, mixing, and where the CKM matrix comes from104.38definition 105.26: The Jarlskog invariant105.26proposition 103.30: Area and the Jarlskog invariant103.30proof : ch:07-discrete-symmetries-cpt@proof-21proof

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typedirectionnode provenancewhere
depends_on eq:ewh-yukawa-lagrangian declared parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2079
depends_on When $CP$ violation is possible declared parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2154
proves ch:07-discrete-symmetries-cpt@proof-20 declared parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2082