Dispersive and Absorptive CP Violation in Mixing
arXiv:2001.07207 · doi:10.1103/PhysRevD.103.053008
Abstract
CP violation (CPV) in mixing is described in terms of the dispersive and absorptive `weak phases' and . They parametrize CPV originating from the interference of decays with and without dispersive mixing, and with and without absorptive mixing, respectively, for CP conjugate hadronic final states , . These are distinct and separately measurable effects. For CP eigenstate final states, indirect CPV only depends on (dispersive CPV), whereas (absorptive CPV) can only be probed with non-CP eigenstate final states. Measurements of the final state dependent phases , determine the intrinsic dispersive and absorptive mixing phases and . The latter are the arguments of the dispersive and absorptive mixing amplitudes and , relative to their dominant () -spin components. The intrinsic phases are experimentally accessible due to approximate universality: in the SM, and in extensions with negligible new CPV phases in Cabibbo favored/doubly Cabibbo suppressed (CF/DCS) decays, the deviation of from is negligible in CF/DCS decays , and below in CF/DCS decays (up to precisely known corrections). In Singly Cabibbo Suppressed (SCS) decays, QCD pollution enters at in -spin breaking and can be significant, but is in the average over , . SM estimates yield . A fit to current data allows larger phases at , from new physics. A fit based on naively extrapolated experimental precision suggests that sensitivity to and in the SM may be achieved at the LHCb Phase II upgrade.
28 pages, 3 figures. v2: Modified the discussion of SM estimates for , in Section IVB, cf. Eqs 110-118, includes a new upper bound on ; typos corrected in Eqs. 73, 77, 151, 152; added Eqs 155, 156, modified Eq A6, writing clarified in a few places. v3: version to appear in Phys Rev D. Intro shortened, improved Sec. III.B.3, typos in the Appendix corrected
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