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Branching ratios,CPasymmetries and polarizations of [equation] decays

机译:[等式]衰变的分支比,CP不对称和极化

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摘要

We analyze the non-leptonic decays (B/B_sightarrow psi (2S) V ) with (V=(ho , omega , K^{*}, phi )) by employing the perturbative QCD (pQCD) factorization approach. Here the branching ratios, the CP asymmetries and the complete set of polarization observables are investigated systematically. Besides the traditional contributions from the factorizable and non-factorizable diagrams at the leading order, the next-to-leading order (NLO) vertex corrections could also provide considerable contributions. The pQCD predictions for the branching ratios of the (B_{(s)} ightarrow psi (2S)K^{*}, psi (2S)phi ) decays are consistent with the measured values within errors. As for (B ightarrow psi (2S) ho , psi (2S) omega ) decays, the branching ratios can reach the order of (10^{-5}) and could be measured in the LHCb and Belle-II experiments. The numerical results show that the direct CP asymmetries of the considered decays are very small. Thus the observation of any large direct CP asymmetry for these decays will be a signal for new physics. The mixing-induced CP asymmetries in the neutral modes are very close to (sin 2eta _{(s)}), which suggests that these channels can give a cross-check on the measurement of the Cabbibo–Kobayashi–Maskawa (CKM) angle (eta ) and (eta _s). We find that the longitudinal polarization fractions (f_0) are suppressed to (sim 50%) due to the large non-factorizable contributions. The magnitudes and phases of the two transverse amplitudes (mathcal {A}_{parallel }) and (mathcal {A}_{perp }) are roughly equal, which is an indication for the approximate light-quark helicity conservation in these decays. The overall polarization observables of (B ightarrow psi (2S) K^{*0}) and (B_s ightarrow psi (2S) phi ) channels are also in good agreement with the experimental measurements as reported by LHCb and BaBar. Other results can also be tested by the LHCb and Belle-II experiments.
机译:我们通过采用扰动QCD(pQCD)分解方法来分析非轻子衰变(B / B_sightarrow psi(2S)V),其中(V =(ho,omega,K ^ {*},phi))。在这里,系统地研究了分支比,CP不对称性和可观察到的极化的完整集合。除了可分解和不可分解图中按先导顺序进行的传统贡献外,次要先导(NLO)顶点校正也可以提供可观的贡献。 (B _ {(s)} ightight psi(2S)K ^ {*},psi(2S)phi)衰变的分支比的pQCD预测与误差内的测量值一致。至于(Bightarrow psi(2S)ho,psi(2S)ω)衰减,分支比率可以达到(10 ^ {-5})的数量级,并且可以在LHCb和Belle-II实验中进行测量。数值结果表明,所考虑的衰减的直接CP不对称性很小。因此,对于这些衰变的任何大的直接CP不对称现象的观察将是新物理学的信号。在中性模式下,混合引起的CP不对称非常接近(sin 2eta _ {{s}}),这表明这些通道可以对Cabbibo–Kobayashi–Maskawa(CKM)角的测量结果进行交叉检查。 (eta)和(eta _s)。我们发现,由于较大的不可分解贡献,纵向极化率(f_0)被抑制为(sim 50 %)。两个横向振幅(数学{A} _ {平行})和(数学{A} _ {perp})的大小和相位大致相等,这表明在这些衰变中近似的夸克螺旋度守恒。 (B ightight psi(2S)K ^ {* 0})和(B_s ightarrow psi(2S)phi)通道的整体极化可观测值也与LHCb和BaBar报道的实验测量结果非常吻合。其他结果也可以通过LHCb和Belle-II实验进行测试。

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