The Cabibbo–Kobayashi–Maskawa (CKM) matrix is a fundamental concept in the field of particle physics, specifically in the study of the weak interaction and the quark sector of the Standard Model. It describes the mixing between the three generations of quarks and plays a crucial role in the phenomenon of flavor mixing as well as in the understanding of CP violation (charge-parity violation) in weak decays.
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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 isThis convention agrees with Makoto Kobayashi's account of three-generation quark mixing.[ref]
Nobel Lecture: CP violation and flavor mixing by Makoto Kobayashi. p. 1022, Section III, exact mixing matrix
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]
CP-Violation in the Renormalizable Theory of Weak Interaction by Makoto Kobayashi and Toshihide Maskawa. pp. 654 and 657, Eq. (6) and six-plet model, Eq. (13)
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]
Nobel Lecture: CP violation and flavor mixing by Makoto Kobayashi. p. 1024, Section IV, concluding limitations