The CKM matrix appears in the charged current of b. For a tree semileptonic transition, a schematic extraction is . Measure an absolute rate or differential spectrum, calculate or independently determine the hadronic factor, and solve for the modulus. The process is not a direct count of quark flavours in a detector: form factors, decay constants, nuclear structure and radiation can limit the result.
  • : superallowed nuclear beta decay, with neutron and pion beta decay cross-checks; correct for nuclear and radiative effects.
  • : spectra with the form factor; compare and using decay constants.
  • and : exclusive and , or inclusive charmless/charmed semileptonic spectra; separate the rare charmless component and control the hadronic calculation.
  • and : charm semileptonic or leptonic decays with form factors or decay constants, and charm production by neutrinos; charm-tagged W boson decays give a complementary constraint.
  • : single-top quark production and the ratio of to all decays, under stated assumptions about allowed interactions.
  • and : neutral B-meson mixing frequencies and rare loop-induced decays, with loop dynamics and hadronic inputs. Mixing-frequency ratios cancel some common uncertainties.
Rate moduli alone do not determine the complex phase. CP-asymmetric decay distributions and interference in neutral-meson systems, or tree-level interference, constrain the phase and the CKM unitarity triangle. Unitarity supplies consistency checks and indirect determinations, but a fit that imposes it must be distinguished from a direct measurement of an element.

Articles by others on the same topic (0)

There are currently no matching articles.