European Physical Journal C: Particles and Fields (Jul 2023)

The background model of the CUPID-Mo $$0\nu \beta \beta $$ 0 ν β β experiment

  • C. Augier,
  • A. S. Barabash,
  • F. Bellini,
  • G. Benato,
  • M. Beretta,
  • L. Bergé,
  • J. Billard,
  • Yu. A. Borovlev,
  • L. Cardani,
  • N. Casali,
  • A. Cazes,
  • E. Celi,
  • M. Chapellier,
  • D. Chiesa,
  • I. Dafinei,
  • F. A. Danevich,
  • M. De Jesus,
  • P. de Marcillac,
  • T. Dixon,
  • L. Dumoulin,
  • K. Eitel,
  • F. Ferri,
  • B. K. Fujikawa,
  • J. Gascon,
  • L. Gironi,
  • A. Giuliani,
  • V. D. Grigorieva,
  • M. Gros,
  • D. L. Helis,
  • H. Z. Huang,
  • R. Huang,
  • L. Imbert,
  • J. Johnston,
  • A. Juillard,
  • H. Khalife,
  • M. Kleifges,
  • V. V. Kobychev,
  • Yu. G. Kolomensky,
  • S. I. Konovalov,
  • J. Kotila,
  • P. Loaiza,
  • L. Ma,
  • E. P. Makarov,
  • R. Mariam,
  • L. Marini,
  • S. Marnieros,
  • X.-F. Navick,
  • C. Nones,
  • E. B. Norman,
  • E. Olivieri,
  • J. L. Ouellet,
  • L. Pagnanini,
  • L. Pattavina,
  • B. Paul,
  • M. Pavan,
  • H. Peng,
  • G. Pessina,
  • S. Pirro,
  • D. V. Poda,
  • O. G. Polischuk,
  • S. Pozzi,
  • E. Previtali,
  • Th. Redon,
  • A. Rojas,
  • S. Rozov,
  • V. Sanglard,
  • J. A. Scarpaci,
  • B. Schmidt,
  • Y. Shen,
  • V. N. Shlegel,
  • V. Singh,
  • C. Tomei,
  • V. I. Tretyak,
  • V. I. Umatov,
  • L. Vagneron,
  • M. Velázquez,
  • B. Welliver,
  • L. Winslow,
  • M. Xue,
  • E. Yakushev,
  • M. Zarytskyy,
  • A. S. Zolotarova

DOI
https://doi.org/10.1140/epjc/s10052-023-11830-2
Journal volume & issue
Vol. 83, no. 7
pp. 1 – 24

Abstract

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Abstract CUPID-Mo, located in the Laboratoire Souterrain de Modane (France), was a demonstrator for the next generation $$0\nu \beta \beta $$ 0 ν β β decay experiment, CUPID. It consisted of an array of 20 enriched Li $$_{2}$$ 2 $$^{100}$$ 100 MoO $$_4$$ 4 bolometers and 20 Ge light detectors and has demonstrated that the technology of scintillating bolometers with particle identification capabilities is mature. Furthermore, CUPID-Mo can inform and validate the background prediction for CUPID. In this paper, we present a detailed model of the CUPID-Mo backgrounds. This model is able to describe well the features of the experimental data and enables studies of the $$2\nu \beta \beta $$ 2 ν β β decay and other processes with high precision. We also measure the radio-purity of the Li $$_{2}$$ 2 $$^{100}$$ 100 MoO $$_4$$ 4 crystals which are found to be sufficient for the CUPID goals. Finally, we also obtain a background index in the region of interest of 3.7 $$^{+0.9}_{-0.8}$$ - 0.8 + 0.9 (stat) $$^{+1.5}_{-0.7}$$ - 0.7 + 1.5 (syst) $$\times ~10 ^{-3}$$ × 10 - 3 counts/ $$\Delta E_{\text {FWHM}}/\text {mol}_{\text {iso}}/\text {year},$$ Δ E FWHM / mol iso / year , the lowest in a bolometric $$0\nu \beta \beta $$ 0 ν β β decay experiment.