Sensitivity of the CUPID experiment to $$0\nu \beta \beta $$ decay of 100Mo

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Authors: K. Alfonso, A. Armatol, C. Augier, Frank T. Avignone III, O Azzolini, A. S. Barabash, G Bari, Andrea Barresi, David Baudin, Fabio Bellini, G. Benato, L. Benussi
+88 more V. Berest, M. Beretta, L. Bergé, Manuele Bettelli, M Biassoni, Julien Billard, F. Boffelli, Virginia Boldrini, E. D. Brandani, C Brofferio, C. Bucci, M Buchynska, J Camilleri, A Campani, Jun Cao, C Capelli, S. Capelli, Vincenzo Caracciolo, L. Cardani, P. Carniti, N. Casali, E. Celi, Chia Cheng Chang, Marion Chapellier, Hannah Chen, D. Chiesa, D. Cintas, M. Clemenza, I Colantoni, S. Copello, O. Cremonesi, R. J. Creswick, Antonio D’Addabbo, I. Dafinei, Fedor A. Danevich, F. De Dominicis, M. De Jésus, P de Marcillac, Stefano Dell'Oro, S. Di Domizio, S Di Lorenzo, Terry Dixon, Alexey Drobizhev, Laurence Dumoulin, Moha El Idrissi, M. Faverzani, E Ferri, F. Ferri, F. Ferroni, Enectali Figueroa-Feliciano, Joseph A. Formaggio, A. Franceschi, S. Fu, Brian K. Fujikawa, Jules Gascon, Stefano Ghislandi, A Giachero, Massimo Girola, L. Gironi, Andrea Giuliani, P. Gorla, C. Gotti, Christopher L. Grant, P Gras, P. V. Guillaumon, T. D. Gutierrez, Kecen Han, E.V Hansen, Karsten M. Heeger, D.L Helis, H. Z. Huang, M.T Hurst, L. Imbert, T. Johnson, A. Juillard, Goran Tripun Karapetrov, Giorgio Keppel, Hawraa Khalife, Vladislav Kobychev, Yu. G. Kolomensky, R Kowalski, H. Lattaud, Marc Lefevre, M Lisovenko, Y. Liu, Y. Liu, Pia Loaiza, Fulvio Mancarella
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References: 75

Abstract

Abstract CUPID is a next-generation bolometric experiment to search for neutrinoless double-beta decay ( $$0\nu \beta \beta $$ 0 ν β β ) of 100 Mo using Li $$_2$$ 2 MoO $$_4$$ 4 scintillating crystals. It will operate 1596 crystals at $$\sim $$ ∼ 10 mK in the CUORE cryostat at the Laboratori Nazionali del Gran Sasso in Italy. Each crystal will be facing two Ge-based bolometric light detectors for $$\alpha $$ α rejection. We compute the discovery and the exclusion sensitivity of CUPID to $$0\nu \beta \beta $$ 0 ν β β in a Frequentist and a Bayesian framework. This computation is done numerically based on pseudo-experiments. For the CUPID baseline scenario, with a background and an energy resolution of $$1.0 \times 10^{-4}$$ 1.0 × 10 - 4 counts/keV/kg/yr and 5 keV FWHM at the Q-value, respectively, this results in a Bayesian exclusion sensitivity (90% c.i.) of $$\hat{T}_{1/2} > 1.6 \times 10^{27} \ \textrm{yr}$$ T ^ 1 / 2 > 1.6 × 10 27 yr , corresponding to the effective Majorana neutrino mass of $$\hat{m}_{\beta \beta } < \ 9.6$$ m ^ β β < 9.6 – $$28 \ \textrm{meV}$$ 28 meV . The Frequentist discovery sensitivity (3 $$\sigma $$ σ ) is $$\hat{T}_{1/2}= 1.0 \times 10^{27} \ \textrm{yr}$$ T ^ 1 / 2 = 1.0 × 10 27 yr

Fields of Study & Subjects

Particle physics theoretical and experimental studies Neutrino Physics Research Nuclear physics research studies

Publication details

Journal / source
The European Physical Journal C
Publisher
Springer Science and Business Media LLC
Volume
86
Issue
6
Publication date
12 June 2026
Language
EN