Cabibbo-Kobayashi-Maskawa matrix Created 2026-09-24 Updated 2026-10-18
The Cabibbo-Kobayashi-Maskawa matrix compares the left-handed unitary matrices that diagonalize the up-type and down-type Yukawa matrices. Its rows label up quarks, charm quarks and top quarks; its columns label down quarks, strange quarks and bottom quarks. In the weak charged current, the coefficient of is . A single CKM matrix therefore connects quark masses, flavour-changing decay amplitudes, and CP violation.
Write and . An exactly unitary matrix with three mixing angles and one CP-violating phase is
This convention agrees with Makoto Kobayashi's account of three-generation quark mixing.[ref]
The Christenson-Cronin-Fitch-Turlay kaon CP violation experiment established the phenomenon that required an explanation. Makoto Kobayashi and Toshihide Maskawa showed that two-generation quark mixing cannot supply it, whereas adding a third quark generation permits an irreducible weak phase. Their 1973 paper also considered additional fields as alternative mechanisms; the three-generation conclusion concerns CP violation from the minimal unitary quark mixing mechanism.[ref]
A common weak phase makes CP violation across mesons testable through the BABAR time-dependent CP violation experiment. It does not explain the cosmic baryon asymmetry.[ref]
CP violation Created 2026-09-24 Updated 2026-10-18
CP violation is the failure of a theory to be invariant under the combination of charge conjugation and parity. Under CPT invariance it is equivalent to time-reversal violation.
CP violation matters experimentally because a symmetry predicts a forbidden transition, not merely a small correction to a permitted one. The Christenson-Cronin-Fitch-Turlay kaon CP violation experiment found evidence for precisely such a transition: a long-lived neutral kaon decaying into two pions. Understanding that inference requires both two-pion kaon event reconstruction and the distinction between kaon CP eigenstates and the physical states of neutral kaon mixing.