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Predicting the values of the leptonic CP violation phases in theories with discrete flavour symmetries

机译:预测具有离散风味对称性的理论中瘦蛋白CP破坏阶段的值

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Using the fact that the neutrino mixing matrix U = (UeU nu)-U-dagger, where U-e and U-nu result from the diagonalisation of the charged lepton and neutrino mass matrices, we consider a number of forms of U-nu associated with a variety of discrete symmetries: i) bimaximal (BM) and ii) tri-bimaximal (TBM) forms, the forms corresponding iii) to the conservation of the lepton charge L' = L-e - L-mu - L-tau (LC), iv) to golden ratio type A (GRA) mixing, v) to golden ratio type B (GRB) mixing, and vi) to hexagonal (HG) mixing. Employing the minimal form of U-e, in terms of angles and phases it contains, that can provide the requisite corrections to U-nu so that reactor, atmospheric and solar neutrino mixing angles theta(13), theta(23) and theta(12) have values compatible with the current data, including a possible sizable deviation of theta(23) from pi/4, we discuss the possibility to obtain predictions for the CP violation phases in the neutrino mixing matrix. Considering the "standard ordering" of the 12 and the 23 rotations in U-e and following the approach developed in [1] we derive predictions for the Dirac phase delta and the rephasing invariant J(CP) in the cases of GRA, ORB and HG forms of U-nu (results for the TBM and BM (LC) forms were obtained in [1]). We show also that under rather general conditions within the scheme considered the values of the Majorana phases in the PMNS matrix can be predicted for each of the forms of U-nu discussed. We give examples of these predictions and of their implications for neutrinoless double beta decay. In the GRA, ORB and HG cases, as in the TBM one, relatively large CP violation effects in neutrino oscillations are predicted (vertical bar J(CP)vertical bar similar to (0.031-0.034)). Distinguishing between the TBM, BM (LC), GRA, GRB and HG forms of U-nu requires a measurement of cos (3 or a relatively high precision measurement of J(CP).
机译:利用中微子混合矩阵U =(UeU nu)-U-匕首这一事实,其中Ue和U-nu是由带电的轻子和中微子质量矩阵的对角线产生的,我们考虑了多种形式的U-nu与多种离散对称性:i)双极大值(BM)和ii)三极大值(TBM)形式,这些形式对应于iii)保持轻子电荷L'= Le-L-mu-L-tau(LC) ; iv)与黄金比例类型A(GRA)混合,v)与黄金比例类型B(GRB)混合,以及vi)与六角形(HG)混合。利用Ue所包含的角度和相位的最小形式,可以对U-nu提供必要的校正,从而使反应堆,大气和太阳中微子的混合角theta(13),theta(23)和theta(12)具有与当前数据兼容的值,包括与pi / 4可能的theta(23)可能的较大偏差,我们讨论了获得中微子混合矩阵中CP违规相的预测的可能性。考虑到Ue的12和23圈的“标准排序”,并按照[1]中开发的方法,我们得出了GRA,ORB和HG形式的Dirac相差和相移不变J(CP)的预测U-nu(在[1]中获得了TBM和BM(LC)形式的结果)。我们还表明,在所考虑的方案中,在相当一般的条件下,可以针对所讨论的每种形式的U-nu预测PMNS矩阵中Majorana相的值。我们给出了这些预测的例子,以及它们对中微子双β衰变的影响。在GRA,ORB和HG情况下,与在TBM中一样,预测了中微子振荡中CP的影响较大(垂直线J(CP)垂直线类似于(0.031-0.034))。要区分U-nu的TBM,BM(LC),GRA,GRB和HG形式,需要测量cos(3或J(CP)的相对高精度测量。

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