BABAR used asymmetric Electron-Positron collisions near the Upsilon meson resonance to prepare neutral B meson pairs. It reconstructed one decay into charmonium plus a kaon, and used flavour tagging on the other B meson with charged leptons or kaons. Silicon tracking reconstructed decay vertices for the decay-time difference. Self-tagging decays calibrated mistags and time resolution; charged decays provided a control. The tagged time distributions established CP violation, limited by backgrounds, mistags and vertex alignment.[ref]
The Lorentz boost converts vertex separation to at leading order. Unequal beam energies thus make a time difference measurable as a distance.[ref]
Figure 1.
From flavour tag and decay vertices to a toy CP asymmetry
. Functional B meson readout above, an original illustrative time-dependent neutral-B CP asymmetry below. The curves are a teaching model, not measured events or a detector drawing. Details.
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]