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Measurement of the 2νßß Decay Rate and Spectral Shape of
Augier, C; Barabash, A S; Bellini, F; Benato, G; Beretta, M; Bergé, L; Billard, J; Borovlev, Yu A; Cardani, L; Casali, N; Cazes, A; Celi, E; Chapellier, M; Chiesa, D; Dafinei, I; Danevich, F A; De Jesus, M; Dixon, T; Dumoulin, L; Eitel, K; Ferri, F; Fujikawa, B K; Gascon, J; Gironi, L; Giuliani, A; Grigorieva, V D; Gros, M; Helis, D L; Huang, H Z; Huang, R; Imbert, L; Johnston, J; Juillard, A; Khalife, H; Kleifges, M; Kobychev, V V; Kolomensky, Yu G; Konovalov, S I; Kotila, J; Loaiza, P; Ma, L; Makarov, E P; de Marcillac, P; Mariam, R; Marini, L; Marnieros, S; Navick, X-F; Nones, C; Norman, E B; Olivieri, E.
Afiliação
  • Augier C; Univ Lyon, Université Lyon 1, CNRS/IN2P3, IP2I-Lyon, F-69622 Villeurbanne, France.
  • Barabash AS; National Research Centre "Kurchatov Institute," Kurchatov Complex of Theoretical and Experimental Physics, 117218 Moscow, Russia.
  • Bellini F; Dipartimento di Fisica, Sapienza Università di Roma, Piazzale Aldo Moro 2, I-00185 Rome, Italy.
  • Benato G; INFN, Sezione di Roma, P.le Aldo Moro 2, I-00185 Rome, Italy.
  • Beretta M; INFN, Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy.
  • Bergé L; INFN, Gran Sasso Science Institute, I-67100 L'Aquila, Italy.
  • Billard J; University of California, Berkeley, California 94720, USA.
  • Borovlev YA; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Cardani L; Univ Lyon, Université Lyon 1, CNRS/IN2P3, IP2I-Lyon, F-69622 Villeurbanne, France.
  • Casali N; Nikolaev Institute of Inorganic Chemistry, 630090 Novosibirsk, Russia.
  • Cazes A; INFN, Sezione di Roma, P.le Aldo Moro 2, I-00185 Rome, Italy.
  • Celi E; INFN, Sezione di Roma, P.le Aldo Moro 2, I-00185 Rome, Italy.
  • Chapellier M; Univ Lyon, Université Lyon 1, CNRS/IN2P3, IP2I-Lyon, F-69622 Villeurbanne, France.
  • Chiesa D; INFN, Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy.
  • Dafinei I; INFN, Gran Sasso Science Institute, I-67100 L'Aquila, Italy.
  • Danevich FA; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • De Jesus M; Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy.
  • Dixon T; INFN, Sezione di Milano-Bicocca, I-20126 Milano, Italy.
  • Dumoulin L; INFN, Sezione di Roma, P.le Aldo Moro 2, I-00185 Rome, Italy.
  • Eitel K; Institute for Nuclear Research of NASU, 03028 Kyiv, Ukraine.
  • Ferri F; INFN, Sezione di Roma Tor Vergata, Via della Ricerca Scientifica 1, I-00133 Rome, Italy.
  • Fujikawa BK; Univ Lyon, Université Lyon 1, CNRS/IN2P3, IP2I-Lyon, F-69622 Villeurbanne, France.
  • Gascon J; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Gironi L; IRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, France.
  • Giuliani A; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Grigorieva VD; Karlsruhe Institute of Technology, Institute for Astroparticle Physics, 76021 Karlsruhe, Germany.
  • Gros M; IRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, France.
  • Helis DL; Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.
  • Huang HZ; Univ Lyon, Université Lyon 1, CNRS/IN2P3, IP2I-Lyon, F-69622 Villeurbanne, France.
  • Huang R; Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy.
  • Imbert L; INFN, Sezione di Milano-Bicocca, I-20126 Milano, Italy.
  • Johnston J; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Juillard A; Nikolaev Institute of Inorganic Chemistry, 630090 Novosibirsk, Russia.
  • Khalife H; IRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, France.
  • Kleifges M; INFN, Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy.
  • Kobychev VV; IRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, France.
  • Kolomensky YG; Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Fudan University, Shanghai 200433, People's Republic of China.
  • Konovalov SI; University of California, Berkeley, California 94720, USA.
  • Kotila J; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • Loaiza P; Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
  • Ma L; Univ Lyon, Université Lyon 1, CNRS/IN2P3, IP2I-Lyon, F-69622 Villeurbanne, France.
  • Makarov EP; Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France.
  • de Marcillac P; Karlsruhe Institute of Technology, Institute for Data Processing and Electronics, 76021 Karlsruhe, Germany.
  • Mariam R; Institute for Nuclear Research of NASU, 03028 Kyiv, Ukraine.
  • Marini L; University of California, Berkeley, California 94720, USA.
  • Marnieros S; Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA.
  • Navick XF; National Research Centre Kurchatov Institute, Institute of Theoretical and Experimental Physics, 117218 Moscow, Russia.
  • Nones C; Department of Physics, University of Jyväskylä, P.O. Box 35, FI-40014 Jyväskylä, Finland.
  • Norman EB; Finnish Institute for Educational Research, University of Jyväskylä, P.O. Box 35, FI-40014 Jyvaäskylä, Finland.
  • Olivieri E; Center for Theoretical Physics, Sloane Physics Laboratory, Yale University, New Haven, Connecticut 06520-8120, USA.
Phys Rev Lett ; 131(16): 162501, 2023 Oct 20.
Article em En | MEDLINE | ID: mdl-37925694
ABSTRACT
Neutrinoless double beta decay (0νßß) is a yet unobserved nuclear process that would demonstrate Lepton number violation, a clear evidence of beyond standard model physics. The process two neutrino double beta decay (2νßß) is allowed by the standard model and has been measured in numerous experiments. In this Letter, we report a measurement of 2νßß decay half-life of ^{100}Mo to the ground state of ^{100}Ru of [7.07±0.02(stat)±0.11(syst)]×10^{18} yr by the CUPID-Mo experiment. With a relative precision of ±1.6% this is the most precise measurement to date of a 2νßß decay rate in ^{100}Mo. In addition, we constrain higher-order corrections to the spectral shape, which provides complementary nuclear structure information. We report a novel measurement of the shape factor ξ_{3,1}=0.45±0.03(stat)±0.05(syst) based on a constraint on the ratio of higher-order terms from theory, which can be reliably calculated. This is compared to theoretical predictions for different nuclear models. We also extract the first value for the effective axial vector coupling constant obtained from a spectral shape study of 2νßß decay.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2023 Tipo de documento: Article