proposition 101.63 Parameter counting, and why three generations permit $CP$ violation

open in the book · parts/11-qft-standard-model/03-weak-interactions.tex:3028 · p. 1975

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proposition 101.63: Parameter counting, and why three generations permit CP violation101.63equation 101.67: eq:weak-ckm-current101.67theorem 101.62: The mixing matrix is unitary101.62theorem 101.59: Glashow–Iliopoulos–Maiani101.59proof : ch:03-weak-interactions@proof-44proofproposition 103.15: Why the counting forbids CP violation at N=2103.15proposition 5.155: Averaging trick5.155proposition 5.153: prop:rep-unitary-completely-reducible5.153theorem 103.11: GIM suppression at one loop103.11proof : ch:03-weak-interactions@proof-43proofequation 101.62: eq:weak-cabibbo-rotation101.62proposition 101.58: A single rotated doublet produces a flavour-changing neutral current101.58phenomenon 103.10: There are no flavour-changing neutral currents103.10theorem 104.38: Masses, mixing, and where the CKM matrix comes from104.38proof : ch:03-weak-interactions@proof-42proof

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typedirectionnode provenancewhere
depends_on eq:weak-ckm-current declared parts/11-qft-standard-model/03-weak-interactions.tex:3040
depends_on The mixing matrix is unitary declared parts/11-qft-standard-model/03-weak-interactions.tex:3040
depends_on Glashow–Iliopoulos–Maiani declared parts/11-qft-standard-model/03-weak-interactions.tex:3040
proves ch:03-weak-interactions@proof-44 declared parts/11-qft-standard-model/03-weak-interactions.tex:3043