Neutral D-meson mixing is the time evolution between the flavor states and . The states with definite propagation masses and decay widths are generally superpositions of these flavor states, so an initially tagged flavor need not remain unchanged before decay.
A measurement tags the production flavor and compares time-dependent rates into selected final states. Some final states can be reached both directly and after mixing, producing interference; a wrong-flavor candidate is therefore not automatically a pure mixing event. The effective two-state Hamiltonian includes both dispersive and absorptive parts. Separating mixing, direct suppressed decays and detector charge asymmetries is part of the inference.[ref]
Review of Particle Physics by Particle Data Group (2022). Review 70, D0–D0 Mixing, §§70.1–70.2 and Eqs. 70.1–70.6
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