论文标题

搜索具有Cupid-0的细粒子

Search for Majoron-like particles with CUPID-0

论文作者

0 Collaboration, Azzolini, O., Beeman, J. W., Bellini, F., Beretta, M., Biassoni, M., Brofferio, C., Bucci, C., Capelli, S., Caracciolo, V., Cardani, L., Carniti, P., Casali, N., Celi, E., Chiesa, D., Clemenza, M., Colantoni, I., Cremonesi, O., Cruciani, A., D'Addabbo, A., Dafinei, I., Di Domizio, S., Dompè, V., Fantini, G., Ferroni, F., Gironi, L., Giuliani, A., Gorla, P., Gotti, C., Keppel, G., Kotila, J., Martinez, M., Nagorny, S., Nastasi, M., Nisi, S., Nones, C., Orlandi, D., Pagnanini, L., Pallavicini, M., Pattavina, L., Pavan, M., Pessina, G., Pettinacci, V., Pirro, S., Pozzi, S., Previtali, E., Puiu, A., Ressa, A., Rusconi, C., Schäffner, K., Tomei, C., Vignati, M., Zolotarova, A. S.

论文摘要

我们首次介绍了使用闪烁的低温热量表的中微子双$β$衰减($0νββ的$β$衰减($0νββ的$))的首次搜索。我们使用贝叶斯方法来重建背景源活动,并评估$^{82} $ SE $0νββχ_0$的潜在贡献。我们考虑了几种可能的理论模型,这些模型预测了类似主要的玻色子偶联与中微子的存在。中性玻色子在中微子双$β$衰减中的排放引起的能量光谱具有光谱指标,$ n = $ 1、2、3或7。我们没有发现这些衰减模式中的任何一个证据,将下限设置为1.2 $^$^$^$^$^$^$^$^$ n = $^$ n = $^$ n = $ n = $ n = $ n = $ n = $ n = $ n = $ n = 1.2 $^$ n = 10 $^{22} $ yr for $ n = $ n = $ 2,1.4 $ \ times $ 10 $^{22} $ yr for $ n = $ n = $ 3和2.2 $ \ times $ 10 $^{21} $ yr for $ n = $ 7。这些是$ 0M $^$^$^$^upperiative $^apection的最佳限制。

We present the first search for the Majoron-emitting modes of the neutrinoless double $β$ decay ($0νββχ_0$) using scintillating cryogenic calorimeters. We analysed the CUPID-0 Phase I data using a Bayesian approach to reconstruct the background sources activities, and evaluate the potential contribution of the $^{82}$Se $0νββχ_0$. We considered several possible theoretical models which predict the existence of a Majoron-like boson coupling to the neutrino. The energy spectra arising from the emission of such bosons in the neutrinoless double $β$ decay have spectral indices $n=$ 1, 2, 3 or 7. We found no evidence of any of these decay modes, setting a lower limit (90% of credibility interval) on the half-life of 1.2 $\times$ 10$^{23}$ yr in the case of $n=$ 1, 3.8 $\times$ 10$^{22}$ yr for $n=$ 2, 1.4 $\times$ 10$^{22}$ yr for $n=$ 3 and 2.2 $\times$ 10$^{21}$ yr for $n=$ 7. These are the best limits on the $0νββχ_0$ half-life of the $^{82}$Se, and demonstrate the potentiality of the CUPID-0 technology in this field.

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