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
Affiliations
- C. Augier
- Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- A. S. Barabash
- National Research Centre Kurchatov Institute, Kurchatov Complex of Theoretical and Experimental Physics
- F. Bellini
- Dipartimento di Fisica, Sapienza Università di Roma
- G. Benato
- Gran Sasso Science Institute
- M. Beretta
- Department of Physics, University of California
- L. Bergé
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- J. Billard
- Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- Yu. A. Borovlev
- Nikolaev Institute of Inorganic Chemistry
- L. Cardani
- INFN, Sezione di Roma Tor Vergata
- N. Casali
- INFN, Sezione di Roma Tor Vergata
- A. Cazes
- Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- E. Celi
- Gran Sasso Science Institute
- M. Chapellier
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- D. Chiesa
- Dipartimento di Fisica, Università di Milano-Bicocca
- I. Dafinei
- INFN, Sezione di Roma Tor Vergata
- F. A. Danevich
- INFN, Sezione di Roma Tor Vergata
- M. De Jesus
- Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- P. de Marcillac
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- T. Dixon
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- L. Dumoulin
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- K. Eitel
- Institute for Astroparticle Physics, Karlsruhe Institute of Technology
- F. Ferri
- IRFU, CEA, Université Paris-Saclay
- B. K. Fujikawa
- Nuclear Science Division, Lawrence Berkeley National Laboratory
- J. Gascon
- Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- L. Gironi
- Dipartimento di Fisica, Università di Milano-Bicocca
- A. Giuliani
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- V. D. Grigorieva
- Nikolaev Institute of Inorganic Chemistry
- M. Gros
- IRFU, CEA, Université Paris-Saclay
- D. L. Helis
- Gran Sasso Science Institute
- H. Z. Huang
- Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Fudan University
- R. Huang
- Department of Physics, University of California
- L. Imbert
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- J. Johnston
- Massachusetts Institute of Technology
- A. Juillard
- Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- H. Khalife
- IRFU, CEA, Université Paris-Saclay
- M. Kleifges
- Institute for Data Processing and Electronics, Karlsruhe Institute of Technology
- V. V. Kobychev
- Institute for Nuclear Research of NASU
- Yu. G. Kolomensky
- Department of Physics, University of California
- S. I. Konovalov
- National Research Centre Kurchatov Institute, Kurchatov Complex of Theoretical and Experimental Physics
- J. Kotila
- Department of Physics, University of Jyväskylä
- P. Loaiza
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- L. Ma
- Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Fudan University
- E. P. Makarov
- Nikolaev Institute of Inorganic Chemistry
- R. Mariam
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- L. Marini
- Gran Sasso Science Institute
- S. Marnieros
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- X.-F. Navick
- IRFU, CEA, Université Paris-Saclay
- C. Nones
- IRFU, CEA, Université Paris-Saclay
- E. B. Norman
- Department of Nuclear Engineering, University of California
- E. Olivieri
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- J. L. Ouellet
- Massachusetts Institute of Technology
- L. Pagnanini
- Gran Sasso Science Institute
- L. Pattavina
- INFN, Laboratori Nazionali del Gran Sasso
- B. Paul
- IRFU, CEA, Université Paris-Saclay
- M. Pavan
- Dipartimento di Fisica, Università di Milano-Bicocca
- H. Peng
- Department of Modern Physics, University of Science and Technology of China
- G. Pessina
- INFN, Sezione di Milano-Bicocca
- S. Pirro
- INFN, Laboratori Nazionali del Gran Sasso
- D. V. Poda
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- O. G. Polischuk
- INFN, Sezione di Roma Tor Vergata
- S. Pozzi
- INFN, Sezione di Milano-Bicocca
- E. Previtali
- Dipartimento di Fisica, Università di Milano-Bicocca
- Th. Redon
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- A. Rojas
- LSM, Laboratoire Souterrain de Modane
- S. Rozov
- Laboratory of Nuclear Problems, JINR
- V. Sanglard
- Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- J. A. Scarpaci
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- B. Schmidt
- IRFU, CEA, Université Paris-Saclay
- Y. Shen
- Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Fudan University
- V. N. Shlegel
- Nikolaev Institute of Inorganic Chemistry
- V. Singh
- Department of Physics, University of California
- C. Tomei
- INFN, Sezione di Roma Tor Vergata
- V. I. Tretyak
- INFN, Laboratori Nazionali del Gran Sasso
- V. I. Umatov
- National Research Centre Kurchatov Institute, Kurchatov Complex of Theoretical and Experimental Physics
- L. Vagneron
- Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- M. Velázquez
- Université Grenoble Alpes, CNRS, Grenoble INP, SIMAP
- B. Welliver
- Department of Physics, University of California
- L. Winslow
- Massachusetts Institute of Technology
- M. Xue
- Department of Modern Physics, University of Science and Technology of China
- E. Yakushev
- Laboratory of Nuclear Problems, JINR
- M. Zarytskyy
- Institute for Nuclear Research of NASU
- A. S. Zolotarova
- IRFU, CEA, Université Paris-Saclay
- DOI
- https://doi.org/10.1140/epjc/s10052-023-11830-2
- Journal volume & issue
-
Vol. 83,
no. 7
pp. 1 – 24
Abstract
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.