European Physical Journal C: Particles and Fields (Sep 2024)
Searching for beyond the Standard Model physics using the improved description of 100Mo $$2\nu \beta \beta $$ 2 ν β β decay spectral shape with CUPID-Mo
- 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,
- 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,
- A. Juillard,
- H. Khalife,
- M. Kleifges,
- V. V. Kobychev,
- Yu. G. Kolomensky,
- S. I. Konovalov,
- J. Kotila,
- P. Loaiza,
- L. Ma,
- E. P. Makarov,
- P. de Marcillac,
- 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,
- F. Šimkovic,
- V. Singh,
- C. Tomei,
- V. I. Tretyak,
- V. I. Umatov,
- L. Vagneron,
- M. Velázquez,
- B. Ware,
- B. Welliver,
- L. Winslow,
- M. Xue,
- E. Yakushev,
- M. Zarytskyy,
- A. S. Zolotarova
Affiliations
- C. Augier
- Univ Lyon, 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
- Univ Lyon, Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- Yu. A. Borovlev
- Nikolaev Institute of Inorganic Chemistry
- L. Cardani
- INFN, Sezione di Roma
- N. Casali
- INFN, Sezione di Roma
- A. Cazes
- Univ Lyon, 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
- F. A. Danevich
- Institute for Nuclear Research National Academy of Sciences of Ukraine
- M. De Jesus
- Univ Lyon, Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- 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
- Univ Lyon, 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
- INFN, Laboratori Nazionali del Gran Sasso
- 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
- A. Juillard
- Univ Lyon, 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 National Academy of Sciences of Ukraine
- 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
- International Center for Advanced Training and Research in Physics (CIFRA)
- 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
- P. de Marcillac
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- R. Mariam
- Université Paris-Saclay, CNRS/IN2P3, IJCLab
- L. Marini
- INFN, Laboratori Nazionali del Gran Sasso
- 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 Physics, 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
- 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
- Université Grenoble Alpes, CNRS, Grenoble INP, LPSC/LSM-IN2P3
- S. Rozov
- Laboratory of Nuclear Problems, JINR
- V. Sanglard
- Univ Lyon, 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
- F. Šimkovic
- Faculty of Mathematics, Physics and Informatics, Comenius University in Bratislava
- V. Singh
- Department of Physics, University of California
- C. Tomei
- INFN, Sezione di Roma
- 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
- Univ Lyon, Université Lyon 1, CNRS/IN2P3, IP2I-Lyon
- M. Velázquez
- Université Grenoble Alpes, CNRS, Grenoble INP, SIMAP
- B. Ware
- John de Laeter Centre for Isotope Research, GPO Box U 1987, Curtin University
- 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 National Academy of Sciences of Ukraine
- A. S. Zolotarova
- IRFU,CEA, Université Paris-Saclay
- DOI
- https://doi.org/10.1140/epjc/s10052-024-13286-4
- Journal volume & issue
-
Vol. 84,
no. 9
pp. 1 – 12
Abstract
Abstract The current experiments searching for neutrinoless double- $$\beta $$ β ( $$0\nu \beta \beta $$ 0 ν β β ) decay also collect large statistics of Standard Model allowed two-neutrino double- $$\beta $$ β ( $$2\nu \beta \beta $$ 2 ν β β ) decay events. These can be used to search for Beyond Standard Model (BSM) physics via $$2\nu \beta \beta $$ 2 ν β β decay spectral distortions. 100Mo has a natural advantage due to its relatively short half-life, allowing higher $$2\nu \beta \beta $$ 2 ν β β decay statistics at equal exposures compared to the other isotopes. We demonstrate the potential of the dual read-out bolometric technique exploiting a 100Mo exposure of 1.47 kg $$\times $$ × years, acquired in the CUPID-Mo experiment at the Modane underground laboratory (France). We set limits on $$0\nu \beta \beta $$ 0 ν β β decays with the emission of one or more Majorons, on $$2\nu \beta \beta $$ 2 ν β β decay with Lorentz violation, and $$2\nu \beta \beta $$ 2 ν β β decay with a sterile neutrino emission. In this analysis, we investigate the systematic uncertainty induced by modeling the $$2\nu \beta \beta $$ 2 ν β β decay spectral shape parameterized through an improved model, an effect never considered before. This work motivates searches for BSM processes in the upcoming CUPID experiment, which will collect the largest amount of $$2\nu \beta \beta $$ 2 ν β β decay events among the next-generation experiments.