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Sterile neutrinos in Λb0 → (Λc+, p+)l1-l2-l3+ν decays

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PHYSICAL REVIEW D
卷 105, 期 1, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.105.013009

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In this study, we investigate lepton number violating and lepton number conserving semi-leptonic decays of heavy baryons Lambda(0)(b) to three charged leptons and a neutrino. These decays occur through intermediate quasi-degenerate GeV-scale sterile neutrinos of either Majorana or Dirac type. Interference between the intermediate heavy neutrinos leads to CP violation in the final states. The effects of neutrino oscillations between the heavy states are also considered in the observables of interest.
We study lepton number violating and lepton number conserving semileptonic decays of heavy baryons Lambda(0)(b) to three charged leptons and a neutrino. The decays occur through two intermediate quasidegenerate GeV-scale sterile neutrinos of either Majorana or Dirac type that can be on-shell. Interference between the intermediate heavy neutrinos leads to CP violation in the final states. Effect of neutrino oscillations between the heavy states are also considered in observables of interests, i.e., branching ratio, and the CP-asymmetry. Given the present constraints on the heavy-to-light mixing elements vertical bar V-eN vertical bar and vertical bar V-mu N&VERBAR, CP-averaged branching ratio of Lambda(0)(b) -> (Lambda(c), p)mu mu e nu with intermediate Majorana neutrinos is almost two orders of magnitude larger than for the same with Dirac neutrinos, whereas, CP-averaged branching ratio of Lambda(0)(b) -> (Lambda(c), p)ee mu nu is of the same order of magnitude for both Majorana and Dirac neutrino induced decays. CP-violation is found to be appreciable when the neutrino mass difference is comparable with the average decay widths.

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