小中微子质量的无中微子双b衰变

F. Águila, J. Wudka, A. Aparici, Arcadi Santamaria, S. Bhattacharya
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引用次数: 8

摘要

如果对无中微子双β衰变(0nbb)的唯一贡献是中微子质量,它的发现可能会非常困难,特别是如果中微子呈现正常的层次谱。然而,这不是唯一的可能性;一般来说,0nbb可以产生手性电子,而中微子诱导的0nbb只能产生两个左手电子。利用有效的拉格朗日方法,我们对轻子数违反(LNV)有效算子进行了分类,这些有效算子具有两个手性轻子,但没有夸克,并根据它们对0nbb的贡献大小排序。我们指出,对于三个手性赋值中的每一个,eLeL;eLeR和eReR,最低阶对应类型的LNV算子只有一个,它们的维数分别为5、7、9。中微子质量总是由这些额外的算子引起的,但可以延迟到一个(7维)或两个(9维)环路。在假设0nbb由7维或9维的算子主导的情况下,我们发现新物理的尺度应该相对较低。30 TeV)。我们还列出了在重模态积分时产生这些算子的SM加法,并讨论了每种情况下可重整理论的简单现实例子。对产生9维算子的模型的现象学进行了一些详细的分析:如果在下一轮实验中可以看到0nbb,则可以在大型强子对撞机中看到模型的双带电标量,并且轻子味违反(LFV)率可以达到预期的实验。此外,在两个环路中产生的中微子质量显示出非常特殊的结构,并且受到强烈约束,事实上,当m!电子电气设备要求低于目前的实验限值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Neutrinoless double b decay with small neutrino masses
If the only contribution to neutrinoless double beta decay (0nbb ) are neutrino masses its discovery may be very difficult, especially if neutrinos present a normal hierarchy spectrum. However, this is not the only possibility; 0nbb can in general produce electrons of either chirality, in contrast with the neutrino induced 0nbb which predicts two left-handed electrons. Using an effective Lagrangian approach we classify the lepton number violating (LNV) effective operators with two leptons of either chirality but no quarks, ordered according to the magnitude of their contribution to 0nbb . We point out that, for each of the three chirality assignments, eLeL; eLeR and eReR , there is only one LNV operator of the corresponding type to lowest order, and these have dimensions 5, 7 and 9, respectively. Neutrino masses are always induced by these extra operators but can be delayed to one (dimension 7) or two loops (dimension 9). Under the assumption that 0nbb is dominated by the operators of dimension 7 or 9 we find that the scale of new physics should be relatively low (. 30 TeV). We also list the SM additions generating these operators upon integration of the heavy modes, and discuss simple realistic examples of renormalizable theories for each case. The phenomenology of a model giving rise to the dimension 9 operator has been analyzed with some detail: if 0nbb is going to be seen in the next round of experiments, the doubly charged scalars of the model could be seen at the LHC and lepton flavour violating (LFV) rates could be at the reach of foreseen experiments. Moreover neutrino masses, which arise at two loops, display a very particular structure and are strongly constrained, in fact, sin 2 q13 & 0:008, when m! eee is required to lie below its present experimental limit.
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