论文标题

Majorana演示者的建模背景

Modeling Backgrounds for the MAJORANA DEMONSTRATOR

论文作者

Haufe, C. R., Arnquist, I. J., Avignone III, F. T., Barabash, A. S., Barton, C. J., Bhimani, K. H., Blalock, E., Bos, B., Busch, M., Buuck, M., Caldwell, T. S., Chan, Y-D., Christofferson, C. D., Chu, P. -H., Clark, M. L., Cuesta, C., Detwiler, J. A., Efremenko, Yu., Ejiri, H., Elliott, S. R., Giovanetti, G. K., Green, M. P., Gruszko, J., Guinn, I. S., Guiseppe, V. E., Henning, R., Aguilar, D. Hervas, Hoppe, E. W., Hostiuc, A., Kidd, M. F., Kim, I., Kouzes, R. T., Lannen V, T. E., Li, A., Lopez, A. M., López-Castaño, J. M., Martin, E. L., Martin, R. D., Massarczyk, R., Meijer, S. J., Oli, T. K., Othman, G., Paudel, L. S., Pettus, W., Poon, A. W. P., Radford, D. C., Reine, A. L., Rielage, K., Ruof, N. W., Schaper, D. C., Tedeschi, D., Varner, R. L., Vasilyev, S., Wilkerson, J. F., Wiseman, C., Xu, W., Yu, C. -H., Zhu, B. X.

论文摘要

Majorana示威者是一个中微子双β衰减($0νβ$)实验,其中包含$ \ sim $ 30千克的p型p型点接触族探测器,在76GE中富集至88%,$ \ sim $ \ sim $ 14 kg $ 14千克的天然也植物检测器。将探测器放入两个电型铜低温器中,并被带有活跃的muon否决的分级被动防护罩包围。在安装之前,进行了广泛的射线测定活动,以确保使用超清洁材料。示威者在$0νβ$ q值的区域中实现了最低的背景速率之一,15.7 $ \ pm $ 1.4 cts/cts/(fwhm t y),涉及64.5 kg-yr活性暴露的大部分。然而,这种背景速率比预计的背景速率高出五倍。这种差异源于第232个衰减链中的多次事件。背景模型拟合旨在了解与基于测定的投影的偏差,有可能确定观察到的背景的来源,并允许对两中性双β衰变半衰期进行精确测量。这些符合早期的仿真研究一致,这表明第232多次的起源不是来自近乎探索的组件,并且为下一代传说实验提供了理动的设计决策。最近的发现缩小了多余活动的可疑位置,激发了最终的模拟和测定活动以完成背景模型。

The MAJORANA DEMONSTRATOR is a neutrinoless double-beta decay ($0νββ$) experiment containing $\sim$30 kg of p-type point contact germanium detectors enriched to 88% in 76Ge and $\sim$14 kg of natural germanium detectors. The detectors are housed in two electroformed copper cryostats and surrounded by a graded passive shield with active muon veto. An extensive radioassay campaign was performed prior to installation to insure the use of ultra-clean materials. The DEMONSTRATOR achieved one of the lowest background rates in the region of the $0νββ$ Q-value, 15.7 $\pm$ 1.4 cts/(FWHM t y) from the low-background configuration spanning most of the 64.5 kg-yr active exposure. Nevertheless this background rate is a factor of five higher than the projected background rate. This discrepancy arises from an excess of events from the 232Th decay chain. Background model fits aim to understand this deviation from assay-based projections, potentially determine the source(s) of observed backgrounds, and allow a precision measurement of the two-neutrino double-beta decay half-life. The fits agree with earlier simulation studies, which indicate the origin of the 232Th excess is not from a near-detector component and have informed design decisions for the next-generation LEGEND experiment. Recent findings have narrowed the suspected locations for the excess activity, motivating a final simulation and assay campaign to complete the background model.

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