论文标题

双向衰减的$^{124} $ Xe和$^{136} $ XE在Xenon1t和Xenonnt实验中

Double-Weak Decays of $^{124}$Xe and $^{136}$Xe in the XENON1T and XENONnT Experiments

论文作者

Aprile, E., Abe, K., Agostini, F., Maouloud, S. Ahmed, Alfonsi, M., Althueser, L., Andrieu, B., Angelino, E., Angevaare, J. R., Antochi, V. C., Martin, D. Antón, Arneodo, F., Baudis, L., Baxter, A. L., Bellagamba, L., Biondi, R., Bismark, A., Brown, A., Bruenner, S., Bruno, G., Budnik, R., Cai, C., Capelli, C., Cardoso, J. M. R., Cichon, D., Clark, M., Colijn, A. P., Conrad, J., Cuenca-García, J. J., Cussonneau, J. P., D'Andrea, V., Decowski, M. P., Di Gangi, P., Di Pede, S., Di Giovanni, A., Di Stefano, R., Diglio, S., Eitel, K., Elykov, A., Farrell, S., Ferella, A. D., Fischer, H., Fulgione, W., Gaemers, P., Gaior, R., Rosso, A. Gallo, Galloway, M., Gao, F., Glade-Beucke, R., Grandi, L., Grigat, J., Guida, M., Higuera, A., Hils, C., Hoetzsch, L., Howlett, J., Iacovacci, M., Itow, Y., Jakob, J., Joerg, F., Joy, A., Kato, N., Kara, M., Kavrigin, P., Kazama, S., Kobayashi, M., Koltman, G., Kopec, A., Landsman, H., Lang, R. F., Levinson, L., Li, I., Li, S., Liang, S., Lindemann, S., Lindner, M., Liu, K., Loizeau, J., Lombardi, F., Long, J., Lopes, J. A. M., Ma, Y., Macolino, C., Mahlstedt, J., Mancuso, A., Manenti, L., Manfredini, A., Marignetti, F., Undagoitia, T. Marrodán, Martens, K., Masbou, J., Masson, D., Masson, E., Mastroianni, S., Messina, M., Miuchi, K., Mizukoshi, K., Molinario, A., Moriyama, S., Morå, K., Mosbacher, Y., Murra, M., Müller, J., Ni, K., Oberlack, U., Paetsch, B., Palacio, J., Peres, R., Pienaar, J., Pierre, M., Pizzella, V., Plante, G., Qi, J., Qin, J., García, D. Ramírez, Reichard, S., Rocchetti, A., Rupp, N., Sanchez, L., Santos, J. M. F. dos, Sarnoff, I., Sartorelli, G., Schreiner, J., Schulte, D., Schulte, P., Eißing, H. Schulze, Schumann, M., Lavina, L. Scotto, Selvi, M., Semeria, F., Shagin, P., Shi, S., Shockley, E., Silva, M., Simgen, H., Takeda, A., Tan, P. -L., Terliuk, A., Thers, D., Toschi, F., Trinchero, G., Tunnell, C., Tönnies, F., Valerius, K., Volta, G., Wei, Y., Weinheimer, C., Weiss, M., Wenz, D., Wittweg, C., Wolf, T., Xu, Z., Yamashita, M., Yang, L., Ye, J., Yuan, L., Zavattini, G., Zerbo, S., Zhong, M., Zhu, T.

论文摘要

我们在寻找$^{124} $ XE和NeutMinoLess Double-β$ decay($0νββ$)的$^{136} $ XE的$^{124} $ XE和NeutiMless $ Xe和NeutiMless $ Xe $^{124} $ XE和NeutiMnoless $ Xe的$^{124} $ XE $^{124} $ XE的搜索结果。我们考虑从$2ν\ text {ecec} $信号模型中捕获从k-到n-shell,并测量$ t_ {1/2}^{2ν\ text {ecec}} =(1.1 \ pm0.2_ \ pm0.2_ \ text}} 10^{22} \; \ text {yr} $,带有$ 0.87 \; \ text {kg} \ times \ text \ text {yr} $ isotope曝光。信号的统计意义为$ 7.0 \,σ$。我们使用$ 36.16 \; \ text {kg} \ times \ text {yr} $ $^{136} $ xe暴露于搜索$0νββ$的$^{136} $。我们没有发现信号的证据,也没有设置$ t_ {1/2}^{0νββ}> 1.2 \ times 10^{24} \; \ text {yr} \;; \ text {at} \; 90 \,\%\; \ text {cl} $。这是迄今为止没有丰富目标的暗物质检测器的最佳结果。我们还报告了对Xenonnt至0νβ$的灵敏度的预测。假设$ 275 \; \ text {kg} \ times \ text {yr} $ $^{136} $ xe暴露,预期的敏感性为$ t_ {1/2}^{0νββ}> 2.1> 2.1 \ 2.1 \ times 10^{25} {25} {25} {25} {25} {\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ yr} {yr} {yr}} \ text {at} \; 90 \,\%\; \ text {cl} $,对应于有效的majorana质量范围为$ \ langle m_ {ββ} \ rangle <(0.19-0.59)\; \; \ text {ev/c}^2 $。

We present results on the search for double-electron capture ($2ν\text{ECEC}$) of $^{124}$Xe and neutrinoless double-$β$ decay ($0νββ$) of $^{136}$Xe in XENON1T. We consider captures from the K- up to the N-shell in the $2ν\text{ECEC}$ signal model and measure a total half-life of $T_{1/2}^{2ν\text{ECEC}}=(1.1\pm0.2_\text{stat}\pm0.1_\text{sys})\times 10^{22}\;\text{yr}$ with a $0.87\;\text{kg}\times\text{yr}$ isotope exposure. The statistical significance of the signal is $7.0\,σ$. We use XENON1T data with $36.16\;\text{kg}\times\text{yr}$ of $^{136}$Xe exposure to search for $0νββ$. We find no evidence of a signal and set a lower limit on the half-life of $T_{1/2}^{0νββ} > 1.2 \times 10^{24}\;\text{yr}\; \text{at}\; 90\,\%\;\text{CL}$. This is the best result from a dark matter detector without an enriched target to date. We also report projections on the sensitivity of XENONnT to $0νββ$. Assuming a $275\;\text{kg}\times\text{yr}$ $^{136}$Xe exposure, the expected sensitivity is $T_{1/2}^{0νββ} > 2.1 \times 10^{25}\;\text{yr}\; \text{at}\; 90\,\%\;\text{CL}$, corresponding to an effective Majorana mass range of $\langle m_{ββ} \rangle < (0.19 - 0.59)\;\text{eV/c}^2$.

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