In this paper, we investigate the CP asymmetries A₂^pm and A₂^mp in B₂^ B^ K^0+B^ K⁰ B^ ^ e^ ₄ and B₂^ B^ K^0+B^ K⁰ B^ ^ e^ ₄ decays, both of them consist of three parts: the indirect CP violations in K⁰ -K⁰ mixing A₂, ₌₈ₗ^pm and A₂, ₌₈ₗ^mp, the direct CP violations in B₂ decay A₂, ₃₈ₑ^pm and A₂, ₃₈ₑ^mp, the new CP violation effects A₂, ₈₍ₓ^pm and A₂, ₈₍ₓ^mp, which originate from the interference between the amplitude of the B₂^- B^- K^0 (K⁰) B^- ^- e^+ ₄ (^+ e^- ₄) decay with the difference between the oscillating effect of K⁰ K⁰ and that of K⁰ K⁰. The strong phase differences of the direct CP asymmetries A₂, ₃₈ₑ^pm and A₂, ₃₈ₑ^mp arising from K⁰-K⁰ mixing parameters. A₂^pm and A₂^mp are of the order O (10^-4) and O (10^-3), respectively. The new CP violation effect A₂, ₈₍ₓ^pm plays a dominant role in A₂^pm, the CP asymmetry A₂^mp is dominated by the indirect CP violation A₂, ₌₈ₗ^mp, so the CP asymmetry A₂^pm provides an ideal place to study the new CP violation effect. We derive another two asymmetry observables A₂^pp and A₂^mm, which are dominated by K⁰-K⁰ mixing. The observables A₂^pm, A₂^mp, A₂^pp and A₂^mm are hopefully to be marginally observed at the LHC experiment and the HL-LHC experiment.
Cheng et al. (Sun,) studied this question.
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