Enhanced light signal for the suppression of pile-up events in Mo-based bolometers for the 0 $$\nu \beta \beta $$ ν β β decay search.
bolometer; scintillating bolometer; light detection; pile-up; cryogenic calorimeter; Neganov-Trofimov-Luke effect
QB460-466
Physics - Instrumentation and Detectors
Nuclear and particle physics. Atomic energy. Radioactivity
0103 physical sciences
FOS: Physical sciences
QC770-798
Instrumentation and Detectors (physics.ins-det)
Astrophysics
01 natural sciences
DOI:
10.48550/arxiv.2302.13944
Publication Date:
2023-05-06
AUTHORS (27)
ABSTRACT
AbstractRandom coincidences of events could be one of the main sources of background in the search for neutrino-less double-beta decay of $$^{100}$$ 100 Mo with macro-bolometers, due to their modest time resolution. Scintillating bolometers as those based on Li$$_2$$ 2 MoO$$_4$$ 4 crystals and employed in the CROSS and CUPID experiments can eventually exploit the coincident fast signal detected in a light detector to reduce this background. However, the scintillation provides a modest signal-to-noise ratio, making difficult a pile-up pulse-shape recognition and rejection at timescales shorter than a few ms. Neganov–Trofimov–Luke assisted light detectors (NTL-LDs) offer the possibility to effectively increase the signal-to-noise ratio, preserving a fast time-response, and enhance the capability of pile-up rejection via pulse shape analysis. In this article we present: (a) an experimental work performed with a Li$$_2$$ 2 MoO$$_4$$ 4 scintillating bolometer, studied in the framework of the CROSS experiment, and utilizing a NTL-LD; (b) a simulation method to reproduce, synthetically, randomly coincident two-neutrino double-beta decay events; (c) a new analysis method based on a pulse-shape discrimination algorithm capable of providing high pile-up rejection efficiencies. We finally show how the NTL-LDs offer a balanced solution between performance and complexity to reach background index $$\sim $$ ∼ $$10^{-4}$$ 10 - 4 counts/keV/kg/year with 280 g Li$$_2$$ 2 MoO$$_4$$ 4 ($$^{100}$$ 100 Mo enriched) bolometers at 3034 keV, the Q$$_{\beta \beta }$$ β β of the double-beta decay, and target the goal of a next generation experiment like CUPID.
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