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de André, João Pedro Athayde Marcondes; Barresi, Andrea; Bellato, Marco; Breton, Dominique; Brigatti, Augusto; Cabrera, Anatael; Caccianiga, Barbara; Cai, Hao; Cai, Zhiyan; Chen, Xin; Cheng, Yaping; Chiesa, Davide; Chin, Yen-Ting; Chukanov, Artem; Corso, Flavio Dal; De La Taille, Christophe; Doroshkevich, Evgeny; Fahrendholz, Ulrike; Feng, Li-Cheng; Gao, Feng; Gong, Hui; Gornushkin, Yuri; Guan, Yuduo; Guizzetti, Rosa Maria; Hagner, Caren; Han, Yang; Herrera, Rafael; Huang, Yongbo; Huo, Lei; Huss, Cédric; Ioannisian, Ara; Jia, Huihui; Jiang, Di; Jiang, Wei; Jollet, Cécile; Karaparabil, Rebin; Khatun, Amina; Khosonthongkee, Khanchai; Li, Min; Li, Xiaonan; Liang, Hao; Liao, Yuzhong; Limphirat, Ayut; Liu, Caimei; Liu, Haotian; Liu, Jiaxi; Liu, Runxuan; Liu, Shubin; Loo, Kai; Luo, Jianyi; Luo, Wuming; Ma, Bing; Ma, Qiumei; Ma, Si; Ma, Xubo; Mayer, Matthias; Naumov, Dmitry V; Peng, Haiping; Peng, Yu; Petitjean, Pierre-Alexandre; Petrucci, Fabrizio; Ricci, Barbara; Sava, Giuseppe; Sawangwit, Utane; Shao, Junyu; Singhal, Apeksha; Soonthornthum, Boonrucksar; Sterr, Tobias; Strati, Virginia; Sun, Guangbao; Sun, Zhengyang; Tuve, Cristina; von Sturm, Katharina; Voronin, Dmitriy; Votano, Lucia; Walker, Pablo; Wang, En; Wang, Guoli; Wang, Yangfu; Wang, Yifang; Wang, Zheng; Wei, Yadong; Weng, Jun; Wu, Yinhui; Xu, Jing; Xu, Yu; Yang, Jie; Ye, Jiaxuan; Ye, Mei; Yu, Boxiang; Yu, Hongzhao; Yu, Xianghui; Yuan, Cenxi; Zeng, Fanrui; Zhang, Hangchang; Zhang, Jie; Zhang, Shiqi; Zhang, Shuihan; Zhang, Yongpeng; Zhu, Kangfu
05/2024Journal Article
We explore the bound neutrons decay into invisible particles (e.g., $n\rightarrow 3 \nu$ or $nn \rightarrow 2 \nu$) in the JUNO liquid scintillator detector. The invisible decay includes two decay modes: $ n \rightarrow { inv} $ and $ nn \rightarrow { inv} $. The invisible decays of $s$-shell neutrons in $^{12}{\rm C}$ will leave a highly excited residual nucleus. Subsequently, some de-excitation modes of the excited residual nuclei can produce a time- and space-correlated triple coincidence signal in the JUNO detector. Based on a full Monte Carlo simulation informed with the latest available data, we estimate all backgrounds, including inverse beta decay events of the reactor antineutrino $\bar{\nu}_e$, natural radioactivity, cosmogenic isotopes and neutral current interactions of atmospheric neutrinos. Pulse shape discrimination and multivariate analysis techniques are employed to further suppress backgrounds. With two years of exposure, JUNO is expected to give an order of magnitude improvement compared to the current best limits. After 10 years of data taking, the JUNO expected sensitivities at a 90% confidence level are $\tau/B( n \rightarrow { inv} ) > 5.0 \times 10^{31} \, {\rm yr}$ and $\tau/B( nn \rightarrow { inv} ) > 1.4 \times 10^{32} \, {\rm yr}$.
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