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

Publication date: 12 Giu 2026

JournalSource: OPENALEXOpenAlex type: articleOpen Access
Authors: K. Alfonso, A. Armatol, C. Augier, F. T. Avignone, O Azzolini, A. S. Barabash, G Bari, Andrea Barresi, D. Baudin, F. Bellini, G. Benato, L. Benussi, V. Berest, M. Beretta, L. Bergé, Manuele Bettelli, M Biassoni, J. Billard, F. Boffelli, Virginia Boldrini, E. D. Brandani, C Brofferio, C. Bucci, M Buchynska, J Camilleri, A Campani, Jun Cao, C Capelli, S. Capelli, V. Caracciolo, L. Cardani, P. Carniti, N. Casali, E. Celi, Chia Cheng Chang, Marion Chapellier, H. Chen, D. Chiesa, D. Cintas, M. Clemenza, I Colantoni, S. Copello, O. Cremonesi, R. J. Creswick, A. D’Addabbo, I. Dafinei, F.A. Danevich, F. De Dominicis, M de Jesus, P de Marcillac, S. Dell’Oro, S. Di Domizio, S Di Lorenzo, T. Dixon, A. Drobizhev, Laurence Dumoulin, M. El Idrissi, M. Faverzani, E Ferri, F. Ferri, F. Ferroni, E. Figueroa‐Feliciano, J. A. Formaggio, A. Franceschi, S. Fu, B. K. Fujikawa, J. Gascon, S. Ghislandi, A Giachero, M. Girola, L. Gironi, A. Giuliani, P. Gorla, C. Gotti, C. Grant, P Gras, P. V. Guillaumon, T. D. Gutierrez, K. Han, E.V Hansen, K. M. Heeger, D.L Helis, H. Z. Huang, M.T Hurst, L. Imbert, A. Juillard, G. Karapetrov, G. Keppel, H. Khalife, V. Kobychev, Yu. G. Kolomensky, R Kowalski, H. Lattaud, Marc Lefevre, M Lisovenko, R Liu, Y. Liu, P. Loaiza, L. Ma, Fulvio Mancarella

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 </mml:mro

Origin
The European Physical Journal C
Volume
86
Issue
6
Cited by
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