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Development of 100 Mo -containing scintillating bolometers for a high-sensitivity neutrinoless double-beta decay search.
Armengaud, E; Augier, C; Barabash, A S; Beeman, J W; Bekker, T B; Bellini, F; Benoît, A; Bergé, L; Bergmann, T; Billard, J; Boiko, R S; Broniatowski, A; Brudanin, V; Camus, P; Capelli, S; Cardani, L; Casali, N; Cazes, A; Chapellier, M; Charlieux, F; Chernyak, D M; de Combarieu, M; Coron, N; Danevich, F A; Dafinei, I; Jesus, M De; Devoyon, L; Domizio, S Di; Dumoulin, L; Eitel, K; Enss, C; Ferroni, F; Fleischmann, A; Foerster, N; Gascon, J; Gastaldo, L; Gironi, L; Giuliani, A; Grigorieva, V D; Gros, M; Hehn, L; Hervé, S; Humbert, V; Ivannikova, N V; Ivanov, I M; Jin, Y; Juillard, A; Kleifges, M; Kobychev, V V; Konovalov, S I.
Afiliação
  • Armengaud E; 1IRFU, CEA, Université Paris-Saclay, 91191 Gif-sur-Yvette, France.
  • Augier C; 2Univ Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, 69622 Villeurbanne, France.
  • Barabash AS; National Research Centre Kurchatov Institute, Institute of Theoretical and Experimental Physics, 117218 Moscow, Russia.
  • Beeman JW; 4Lawrence Berkeley National Laboratory, Berkeley, CA 94720 USA.
  • Bekker TB; 5V.S. Sobolev Institute of Geology and Mineralogy of the Siberian Branch of the RAS, 630090 Novosibirsk, Russia.
  • Bellini F; 6Dipartimento di Fisica, Sapienza Università di Roma, P.le Aldo Moro 2, 00185 Rome, Italy.
  • Benoît A; 7INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Rome, Italy.
  • Bergé L; CNRS-Néel, 38042 Grenoble Cedex 9, France.
  • Bergmann T; 9CSNSM, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, 91405 Orsay, France.
  • Billard J; 10Karlsruhe Institute of Technology, Institut für Prozessdatenverarbeitung und Elektronik, 76021 Karlsruhe, Germany.
  • Boiko RS; 2Univ Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, 69622 Villeurbanne, France.
  • Broniatowski A; 11Institute for Nuclear Research, 03028 Kyiv, Ukraine.
  • Brudanin V; 9CSNSM, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, 91405 Orsay, France.
  • Camus P; 12Karlsruhe Institute of Technology, Institut für Experimentelle Teilchenphysik, 76128 Karlsruhe, Germany.
  • Capelli S; 13Laboratory of Nuclear Problems, JINR, 141980 Dubna, Moscow Region Russia.
  • Cardani L; CNRS-Néel, 38042 Grenoble Cedex 9, France.
  • Casali N; 14Dipartimento di Fisica, Università di Milano Bicocca, 20126 Milan, Italy.
  • Cazes A; 15INFN, Sezione di Milano Bicocca, 20126 Milan, Italy.
  • Chapellier M; 7INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Rome, Italy.
  • Charlieux F; 7INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Rome, Italy.
  • Chernyak DM; 2Univ Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, 69622 Villeurbanne, France.
  • de Combarieu M; 9CSNSM, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, 91405 Orsay, France.
  • Coron N; 2Univ Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, 69622 Villeurbanne, France.
  • Danevich FA; 11Institute for Nuclear Research, 03028 Kyiv, Ukraine.
  • Dafinei I; 34Present Address: Kavli Institute for the Physics and Mathematics of the Universe (WPI), The University of Tokyo Institutes for Advanced Study, The University of Tokyo, Kashiwa, Chiba Japan.
  • Jesus M; 16IRAMIS, CEA, Université Paris-Saclay, 91191 Gif-sur-Yvette, France.
  • Devoyon L; 17IAS, CNRS, Université Paris-Sud, 91405 Orsay, France.
  • Domizio SD; 11Institute for Nuclear Research, 03028 Kyiv, Ukraine.
  • Dumoulin L; 7INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Rome, Italy.
  • Eitel K; 2Univ Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, 69622 Villeurbanne, France.
  • Enss C; 18Orphée, CEA, Université Paris-Saclay, 91191 Gif-sur-Yvette, France.
  • Ferroni F; 19Dipartimento di Fisica, Università di Genova, 16146 Genoa, Italy.
  • Fleischmann A; 20INFN Sezione di Genova, 16146 Genoa, Italy.
  • Foerster N; 9CSNSM, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, 91405 Orsay, France.
  • Gascon J; 21Karlsruhe Institute of Technology, Institut für Kernphysik, 76021 Karlsruhe, Germany.
  • Gastaldo L; 22Kirchhoff Institute for Physics, Heidelberg University, 69120 Heidelberg, Germany.
  • Gironi L; 6Dipartimento di Fisica, Sapienza Università di Roma, P.le Aldo Moro 2, 00185 Rome, Italy.
  • Giuliani A; 7INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Rome, Italy.
  • Grigorieva VD; 22Kirchhoff Institute for Physics, Heidelberg University, 69120 Heidelberg, Germany.
  • Gros M; 12Karlsruhe Institute of Technology, Institut für Experimentelle Teilchenphysik, 76128 Karlsruhe, Germany.
  • Hehn L; 2Univ Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, 69622 Villeurbanne, France.
  • Hervé S; 22Kirchhoff Institute for Physics, Heidelberg University, 69120 Heidelberg, Germany.
  • Humbert V; 14Dipartimento di Fisica, Università di Milano Bicocca, 20126 Milan, Italy.
  • Ivannikova NV; 15INFN, Sezione di Milano Bicocca, 20126 Milan, Italy.
  • Ivanov IM; 9CSNSM, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, 91405 Orsay, France.
  • Jin Y; 23DISAT, Università dell'Insubria, 22100 Como, Italy.
  • Juillard A; 24Nikolaev Institute of Inorganic Chemistry, 630090 Novosibirsk, Russia.
  • Kleifges M; 1IRFU, CEA, Université Paris-Saclay, 91191 Gif-sur-Yvette, France.
  • Kobychev VV; 4Lawrence Berkeley National Laboratory, Berkeley, CA 94720 USA.
  • Konovalov SI; 21Karlsruhe Institute of Technology, Institut für Kernphysik, 76021 Karlsruhe, Germany.
Eur Phys J C Part Fields ; 77(11): 785, 2017.
Article em En | MEDLINE | ID: mdl-31997932
This paper reports on the development of a technology involving 100 Mo -enriched scintillating bolometers, compatible with the goals of CUPID, a proposed next-generation bolometric experiment to search for neutrinoless double-beta decay. Large mass ( ∼ 1 kg ), high optical quality, radiopure 100 Mo -containing zinc and lithium molybdate crystals have been produced and used to develop high performance single detector modules based on 0.2-0.4 kg scintillating bolometers. In particular, the energy resolution of the lithium molybdate detectors near the Q-value of the double-beta transition of 100 Mo (3034 keV) is 4-6 keV FWHM. The rejection of the α -induced dominant background above 2.6 MeV is better than 8 σ . Less than 10 µ Bq/kg activity of 232 Th ( 228 Th ) and 226 Ra in the crystals is ensured by boule recrystallization. The potential of 100 Mo -enriched scintillating bolometers to perform high sensitivity double-beta decay searches has been demonstrated with only 10 kg × d exposure: the two neutrino double-beta decay half-life of 100 Mo has been measured with the up-to-date highest accuracy as T 1 / 2 = [6.90 ± 0.15(stat.) ± 0.37(syst.)] × 10 18 years . Both crystallization and detector technologies favor lithium molybdate, which has been selected for the ongoing construction of the CUPID-0/Mo demonstrator, containing several kg of 100 Mo .

Texto completo: 1 Base de dados: MEDLINE Tipo de estudo: Diagnostic_studies Idioma: En Ano de publicação: 2017 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Tipo de estudo: Diagnostic_studies Idioma: En Ano de publicação: 2017 Tipo de documento: Article