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arXiv 1108.0004hep-phhep-ex
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无中微子双β衰变和重无中微子

Neutrinoless Double Beta Decay and Heavy Sterile Neutrinos

Manimala Mitra, Goran Senjanovic, Francesco Vissani

摘要:

无中微子双β衰变的实验速率可以通过交换与普通中微子混合且重于200 MeV的虚拟无菌中微子而达到饱和。有趣的是,由于新的核基质元素,这一假设只受到边缘实验的限制。这种可能性进行了分析的上下文中的I型跷跷板模型,重中微子质谱,介子的稀有衰变以及中微子衰变搜索,大型强子对撞机,轻子味违反的影响也进行了探索性的调查。只有当它们的质量低于大约10 TeV时,重无菌中微子才能使速率饱和,但在这种情况下,轻中微子质量的抑制必须大于电弱标度和重中微子标度的比值;即,比天真的跷跷板期望更压抑。我们对最小版本的跷跷板模型中这一条件成立的情况进行了分类,表明它与(1)重中微子占主导地位的无中微子双β速率和(2)任何轻中微子质谱都是相容的。没有过多的微调和轻中微子质量矩阵的辐射稳定性,加上饱和的无菌中微子贡献,意味着重中微子质量的上限约为10 GeV。我们将我们的分析扩展到扩展的跷跷板方案,其中轻和重的无菌中微子的贡献是完全解耦的,允许无菌中微子饱和的无中微子双β衰变目前的实验约束。在分析的模型中,这个过程的速率与轻中微子质量的值没有严格的联系,并且快速的跃迁速率与轻于100 meV的中微子是相容的。

英文摘要:

The experimental rate of neutrinoless double beta decay can be saturated by the exchange of virtual sterile neutrinos, that mix with the ordinary neutrinos and are heavier than 200 MeV. Interestingly, this hypothesis is subject only to marginal experimental constraints, because of the new nuclear matrix elements. This possibility is analyzed in the context of the Type I seesaw model, performing also exploratory investigations of the implications for heavy neutrino mass spectra, rare decays of mesons as well as neutrino-decay search, LHC, and lepton flavor violation. The heavy sterile neutrinos can saturate the rate only when their masses are below some 10 TeV, but in this case, the suppression of the light-neutrino masses has to be more than the ratio of the electroweak scale and the heavy-neutrino scale; i.e., more suppressed than the naive seesaw expectation. We classify the cases when this condition holds true in the minimal version of the seesaw model, showing its compatibility (1) with neutrinoless double beta rate being dominated by heavy neutrinos and (2) with any light neutrino mass spectra. The absence of excessive fine-tunings and the radiative stability of light neutrino mass matrices, together with a saturating sterile neutrino contribution, imply an upper bound on the heavy neutrino masses of about 10 GeV. We extend our analysis to the Extended seesaw scenario, where the light and the heavy sterile neutrino contributions are completely decoupled, allowing the sterile neutrinos to saturate the present experimental bound on neutrinoless double beta decay. In the models analyzed, the rate of this process is not strictly connected with the values of the light neutrino masses, and a fast transition rate is compatible with neutrinos lighter than 100 meV.

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