- Main
Modeling backgrounds for the Majorana Demonstrator
- Haufe, CR;
- Arnquist, IJ;
- Avignone, FT;
- Barabash, AS;
- Barton, CJ;
- Bhimani, KH;
- Blalock, E;
- Bos, B;
- Busch, M;
- Buuck, M;
- Caldwell, TS;
- Chan, Y-D;
- Christofferson, CD;
- Chu, P-H;
- Clark, ML;
- Cuesta, C;
- Detwiler, JA;
- Efremenko, Yu;
- Ejiri, H;
- Elliott, SR;
- Giovanetti, GK;
- Green, MP;
- Gruszko, J;
- Guinn, IS;
- Guiseppe, VE;
- Henning, R;
- Aguilar, D Hervas;
- Hoppe, EW;
- Hostiuc, A;
- Kidd, MF;
- Kim, I;
- Kouzes, RT;
- V., TE Lannen;
- Li, A;
- Lopez, AM;
- López-Castaño, JM;
- Martin, EL;
- Martin, RD;
- Massarczyk, R;
- Meijer, SJ;
- Oli, TK;
- Othman, G;
- Paudel, LS;
- Pettus, W;
- Poon, AWP;
- Radford, DC;
- Reine, AL;
- Rielage, K;
- Ruof, NW;
- Schaper, DC;
- Tedeschi, D;
- Varner, RL;
- Vasilyev, S;
- Wilkerson, JF;
- Wiseman, C;
- Xu, W;
- Yu, C-H;
- Zhu, BX
- et al.
Published Web Location
https://doi.org/10.1063/5.0161379Abstract
The MAJORANA DEMONSTRATOR is a neutrinoless double-beta decay (0νββ) experiment containing ~30 kg of p-type point-contact germanium detectors enriched to 88% in 76Ge and ~14 kg of natural germanium detectors. The detectors are housed in two electroformed copper cryostats and surrounded by a graded passive shield with an 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±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 explain the deviation from assay-based projections, potentially determine the source(s) of observed backgrounds, and allow a precise 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.
Main Content
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