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Agostini M, Alexander A, Araujo GR, Bakalyarov AM, Balata M, Barabanov I, Baudis L, Bauer C, Belogurov S, Bettini A, Bezrukov L, Biancacci V, Bossio E, Bothe V, Brugnera R, Caldwell A, Calgaro S, Cattadori C, Chernogorov A, Chiu PJ, Comellato T, D'Andrea V, Demidova EV, Di Giacinto A, Di Marco N, Doroshkevich E, Fischer F, Fomina M, Gangapshev A, Garfagnini A, Gooch C, Grabmayr P, Gurentsov V, Gusev K, Hackenmüller S, Hemmer S, Hofmann W, Huang J, Hult M, Inzhechik LV, Janicskó Csáthy J, Jochum J, Junker M, Kazalov V, Kermaïdic Y, Khushbakht H, Kihm T, Kilgus K, Kirpichnikov IV, Klimenko A, Knöpfle KT, Kochetov O, Kornoukhov VN, Krause P, Kuzminov VV, Laubenstein M, Lehnert B, Lindner M, Lippi I, Lubashevskiy A, Lubsandorzhiev B, Lutter G, Macolino C, Majorovits B, Maneschg W, Manzanillas L, Marshall G, Miloradovic M, Mingazheva R, Misiaszek M, Morella M, Müller Y, Nemchenok I, Neuberger M, Pandola L, Pelczar K, Pertoldi L, Piseri P, Pullia A, Ransom C, Rauscher L, Redchuk M, Riboldi S, Rumyantseva N, Sada C, Sailer S, Salamida F, Schönert S, Schreiner J, Schütt M, Schütz AK, Schulz O, Schwarz M, Schwingenheuer B, Selivanenko O, Shevchik E, Shirchenko M, Shtembari L, Simgen H, Smolnikov A, Stukov D, Sullivan S, Vasenko AA, Veresnikova A, Vignoli C, von Sturm K, Wester T, Wiesinger C, Wojcik M, Yanovich E, Zatschler B, Zhitnikov I, Zhukov SV, Zinatulina D, Zschocke A, Zsigmond AJ, Zuber K, Zuzel G. Final Results of GERDA on the Two-Neutrino Double-β Decay Half-Life of ^{76}Ge. PHYSICAL REVIEW LETTERS 2023; 131:142501. [PMID: 37862664 DOI: 10.1103/physrevlett.131.142501] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/13/2023] [Accepted: 08/15/2023] [Indexed: 10/22/2023]
Abstract
We present the measurement of the two-neutrino double-β decay rate of ^{76}Ge performed with the GERDA Phase II experiment. With a subset of the entire GERDA exposure, 11.8 kg yr, the half-life of the process has been determined: T_{1/2}^{2ν}=(2.022±0.018_{stat}±0.038_{syst})×10^{21} yr. This is the most precise determination of the ^{76}Ge two-neutrino double-β decay half-life and one of the most precise measurements of a double-β decay process. The relevant nuclear matrix element can be extracted: M_{eff}^{2ν}=(0.101±0.001).
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Affiliation(s)
- M Agostini
- Department of Physics and Astronomy, University College London, London, United Kingdom
| | - A Alexander
- Department of Physics and Astronomy, University College London, London, United Kingdom
| | - G R Araujo
- Physik-Institut, Universität Zürich, Zurich, Switzerland
| | - A M Bakalyarov
- National Research Centre "Kurchatov Institute," Moscow, Russia
| | - M Balata
- INFN Laboratori Nazionali del Gran Sasso, Assergi, Italy
| | - I Barabanov
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - L Baudis
- Physik-Institut, Universität Zürich, Zurich, Switzerland
| | - C Bauer
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - S Belogurov
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
- Institute for Theoretical and Experimental Physics, NRC "Kurchatov Institute," Moscow, Russia
| | - A Bettini
- Dipartimento di Fisica e Astronomia, Università degli Studi di Padova, Padua, Italy
- INFN Padova, Padua, Italy
| | - L Bezrukov
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - V Biancacci
- Dipartimento di Fisica e Astronomia, Università degli Studi di Padova, Padua, Italy
- INFN Padova, Padua, Italy
| | - E Bossio
- Physik Department, Technische Universität München, Germany
| | - V Bothe
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - R Brugnera
- Dipartimento di Fisica e Astronomia, Università degli Studi di Padova, Padua, Italy
- INFN Padova, Padua, Italy
| | - A Caldwell
- Max-Planck-Institut für Physik, Munich, Germany
| | - S Calgaro
- Dipartimento di Fisica e Astronomia, Università degli Studi di Padova, Padua, Italy
- INFN Padova, Padua, Italy
| | | | - A Chernogorov
- Institute for Theoretical and Experimental Physics, NRC "Kurchatov Institute," Moscow, Russia
- National Research Centre "Kurchatov Institute," Moscow, Russia
| | - P-J Chiu
- Physik-Institut, Universität Zürich, Zurich, Switzerland
| | - T Comellato
- Physik Department, Technische Universität München, Germany
| | - V D'Andrea
- INFN Laboratori Nazionali del Gran Sasso and Università degli Studi dell'Aquila, L'Aquila, Italy
| | - E V Demidova
- Institute for Theoretical and Experimental Physics, NRC "Kurchatov Institute," Moscow, Russia
| | - A Di Giacinto
- INFN Laboratori Nazionali del Gran Sasso, Assergi, Italy
| | - N Di Marco
- INFN Laboratori Nazionali del Gran Sasso and Gran Sasso Science Institute, Assergi, Italy
| | - E Doroshkevich
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - F Fischer
- Max-Planck-Institut für Physik, Munich, Germany
| | - M Fomina
- Joint Institute for Nuclear Research, Dubna, Russia
| | - A Gangapshev
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - A Garfagnini
- Dipartimento di Fisica e Astronomia, Università degli Studi di Padova, Padua, Italy
- INFN Padova, Padua, Italy
| | - C Gooch
- Max-Planck-Institut für Physik, Munich, Germany
| | - P Grabmayr
- Physikalisches Institut, Eberhard Karls Universität Tübingen, Tübingen, Germany
| | - V Gurentsov
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - K Gusev
- Joint Institute for Nuclear Research, Dubna, Russia
- National Research Centre "Kurchatov Institute," Moscow, Russia
- Physik Department, Technische Universität München, Germany
| | | | | | - W Hofmann
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - J Huang
- Physik-Institut, Universität Zürich, Zurich, Switzerland
| | - M Hult
- European Commission, JRC-Geel, Geel, Belgium
| | - L V Inzhechik
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | | | - J Jochum
- Physikalisches Institut, Eberhard Karls Universität Tübingen, Tübingen, Germany
| | - M Junker
- INFN Laboratori Nazionali del Gran Sasso, Assergi, Italy
| | - V Kazalov
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - Y Kermaïdic
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - H Khushbakht
- Physikalisches Institut, Eberhard Karls Universität Tübingen, Tübingen, Germany
| | - T Kihm
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - K Kilgus
- Physikalisches Institut, Eberhard Karls Universität Tübingen, Tübingen, Germany
| | - I V Kirpichnikov
- Institute for Theoretical and Experimental Physics, NRC "Kurchatov Institute," Moscow, Russia
| | - A Klimenko
- Joint Institute for Nuclear Research, Dubna, Russia
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - K T Knöpfle
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - O Kochetov
- Joint Institute for Nuclear Research, Dubna, Russia
| | - V N Kornoukhov
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - P Krause
- Physik Department, Technische Universität München, Germany
| | - V V Kuzminov
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - M Laubenstein
- INFN Laboratori Nazionali del Gran Sasso, Assergi, Italy
| | - B Lehnert
- Institut für Kern- und Teilchenphysik, Technische Universität Dresden, Dresden, Germany
| | - M Lindner
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | | | | | - B Lubsandorzhiev
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - G Lutter
- European Commission, JRC-Geel, Geel, Belgium
| | - C Macolino
- INFN Laboratori Nazionali del Gran Sasso and Università degli Studi dell'Aquila, L'Aquila, Italy
| | | | - W Maneschg
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | | | - G Marshall
- Department of Physics and Astronomy, University College London, London, United Kingdom
| | - M Miloradovic
- Physik-Institut, Universität Zürich, Zurich, Switzerland
| | - R Mingazheva
- Physik-Institut, Universität Zürich, Zurich, Switzerland
| | - M Misiaszek
- Institute of Physics, Jagiellonian University, Cracow, Poland
| | - M Morella
- INFN Laboratori Nazionali del Gran Sasso and Gran Sasso Science Institute, Assergi, Italy
| | - Y Müller
- Physik-Institut, Universität Zürich, Zurich, Switzerland
| | - I Nemchenok
- Joint Institute for Nuclear Research, Dubna, Russia
| | - M Neuberger
- Physik Department, Technische Universität München, Germany
| | - L Pandola
- INFN Laboratori Nazionali del Sud, Catania, Italy
| | - K Pelczar
- European Commission, JRC-Geel, Geel, Belgium
| | - L Pertoldi
- Physik Department, Technische Universität München, Germany
- INFN Padova, Padua, Italy
| | - P Piseri
- Dipartimento di Fisica, Università degli Studi di Milano and INFN Milano, Milan, Italy
| | - A Pullia
- Dipartimento di Fisica, Università degli Studi di Milano and INFN Milano, Milan, Italy
| | - C Ransom
- Physik-Institut, Universität Zürich, Zurich, Switzerland
| | - L Rauscher
- Physikalisches Institut, Eberhard Karls Universität Tübingen, Tübingen, Germany
| | | | - S Riboldi
- Dipartimento di Fisica, Università degli Studi di Milano and INFN Milano, Milan, Italy
| | - N Rumyantseva
- Joint Institute for Nuclear Research, Dubna, Russia
- National Research Centre "Kurchatov Institute," Moscow, Russia
| | - C Sada
- Dipartimento di Fisica e Astronomia, Università degli Studi di Padova, Padua, Italy
- INFN Padova, Padua, Italy
| | - S Sailer
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - F Salamida
- INFN Laboratori Nazionali del Gran Sasso and Università degli Studi dell'Aquila, L'Aquila, Italy
| | - S Schönert
- Physik Department, Technische Universität München, Germany
| | - J Schreiner
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - M Schütt
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - A-K Schütz
- Physikalisches Institut, Eberhard Karls Universität Tübingen, Tübingen, Germany
| | - O Schulz
- Max-Planck-Institut für Physik, Munich, Germany
| | - M Schwarz
- Physik Department, Technische Universität München, Germany
| | | | - O Selivanenko
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - E Shevchik
- Joint Institute for Nuclear Research, Dubna, Russia
| | - M Shirchenko
- Joint Institute for Nuclear Research, Dubna, Russia
| | - L Shtembari
- Max-Planck-Institut für Physik, Munich, Germany
| | - H Simgen
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - A Smolnikov
- Joint Institute for Nuclear Research, Dubna, Russia
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - D Stukov
- National Research Centre "Kurchatov Institute," Moscow, Russia
| | - S Sullivan
- Max-Planck-Institut für Kernphysik, Heidelberg, Germany
| | - A A Vasenko
- Institute for Theoretical and Experimental Physics, NRC "Kurchatov Institute," Moscow, Russia
| | - A Veresnikova
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - C Vignoli
- INFN Laboratori Nazionali del Gran Sasso, Assergi, Italy
| | - K von Sturm
- Dipartimento di Fisica e Astronomia, Università degli Studi di Padova, Padua, Italy
- INFN Padova, Padua, Italy
| | - T Wester
- Institut für Kern- und Teilchenphysik, Technische Universität Dresden, Dresden, Germany
| | - C Wiesinger
- Physik Department, Technische Universität München, Germany
| | - M Wojcik
- Institute of Physics, Jagiellonian University, Cracow, Poland
| | - E Yanovich
- Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia
| | - B Zatschler
- Institut für Kern- und Teilchenphysik, Technische Universität Dresden, Dresden, Germany
| | - I Zhitnikov
- Joint Institute for Nuclear Research, Dubna, Russia
| | - S V Zhukov
- National Research Centre "Kurchatov Institute," Moscow, Russia
| | - D Zinatulina
- Joint Institute for Nuclear Research, Dubna, Russia
| | - A Zschocke
- Physikalisches Institut, Eberhard Karls Universität Tübingen, Tübingen, Germany
| | | | - K Zuber
- Institut für Kern- und Teilchenphysik, Technische Universität Dresden, Dresden, Germany
| | - G Zuzel
- Institute of Physics, Jagiellonian University, Cracow, Poland
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Azzolini O, Beeman JW, Bellini F, Beretta M, Biassoni M, Brofferio C, Bucci C, Capelli S, Caracciolo V, Cardani L, Carniti P, Casali N, Chiesa D, Clemenza M, Colantoni I, Cremonesi O, Cruciani A, D'Addabbo A, Dafinei I, De Dominicis F, Di Domizio S, Ferroni F, Gironi L, Giuliani A, Gorla P, Gotti C, Keppel G, Martinez M, Nagorny S, Nastasi M, Nisi S, Nones C, Orlandi D, Pagnanini L, Pallavicini M, Pattavina L, Pavan M, Pessina G, Pettinacci V, Pirro S, Pozzi S, Previtali E, Puiu A, Rusconi C, Schäffner K, Tomei C, Vignati M, Zolotarova AS. Final Result on the Neutrinoless Double Beta Decay of ^{82}Se with CUPID-0. PHYSICAL REVIEW LETTERS 2022; 129:111801. [PMID: 36154394 DOI: 10.1103/physrevlett.129.111801] [Citation(s) in RCA: 2] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/03/2022] [Accepted: 07/22/2022] [Indexed: 06/16/2023]
Abstract
CUPID-0, an array of Zn^{82}Se cryogenic calorimeters, was the first medium-scale demonstrator of the scintillating bolometers' technology. The first project phase (March 2017-December 2018) allowed the most stringent limit on the neutrinoless double beta decay half-life of the isotope of interest, ^{82}Se, to be set. After a six month long detector upgrade, CUPID-0 began its second and last phase (June 2019-February 2020). In this Letter, we describe the search for neutrinoless double beta decay of ^{82}Se with a total exposure (phase I+II) of 8.82 kg yr^{-1} of isotope. We set a limit on the half-life of ^{82}Se to the ground state of ^{82}Kr of T_{1/2}^{0ν}(^{82}Se)>4.6×10^{24} yr (90% credible interval), corresponding to an effective Majorana neutrino mass m_{ββ}<(263-545) meV. We also set the most stringent lower limits on the neutrinoless decays of ^{82}Se to the 0_{1}^{+}, 2_{1}^{+}, and 2_{2}^{+} excited states of ^{82}Kr, finding 1.8×10^{23} yr, 3.0×10^{23} yr, and 3.2×10^{23} yr (90% credible interval) respectively.
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Affiliation(s)
- O Azzolini
- INFN Laboratori Nazionali di Legnaro, I-35020 Legnaro (Pd), Italy
| | - J W Beeman
- Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - F Bellini
- Dipartimento di Fisica, Sapienza Università di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
| | - M Beretta
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - M Biassoni
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - C Brofferio
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - C Bucci
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - S Capelli
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - V Caracciolo
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - L Cardani
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
| | - P Carniti
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - N Casali
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
| | - D Chiesa
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - M Clemenza
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - I Colantoni
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
- Consiglio Nazionale delle Ricerche, Istituto di Nanotecnologia, c/o Dipartimento di Fisica, Sapienza Università di Roma, 00185 Rome, Italy
| | - O Cremonesi
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - A Cruciani
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
| | - A D'Addabbo
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - I Dafinei
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
| | - F De Dominicis
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
- Gran Sasso Science Institute, 67100 L'Aquila, Italy
| | - S Di Domizio
- Dipartimento di Fisica, Università di Genova, I-16146 Genova, Italy
- INFN Sezione di Genova, I-16146 Genova, Italy
| | - F Ferroni
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
- Gran Sasso Science Institute, 67100 L'Aquila, Italy
| | - L Gironi
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - A Giuliani
- CNRS/CSNSM, Centre de Sciences Nucléaires et de Sciences de la Matière, 91405 Orsay, France
| | - P Gorla
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - C Gotti
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - G Keppel
- INFN Laboratori Nazionali di Legnaro, I-35020 Legnaro (Pd), Italy
| | - M Martinez
- Dipartimento di Fisica, Sapienza Università di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
| | - S Nagorny
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - M Nastasi
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - S Nisi
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - C Nones
- IRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, France
| | - D Orlandi
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - L Pagnanini
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
- Gran Sasso Science Institute, 67100 L'Aquila, Italy
| | - M Pallavicini
- Dipartimento di Fisica, Università di Genova, I-16146 Genova, Italy
- INFN Sezione di Genova, I-16146 Genova, Italy
| | - L Pattavina
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - M Pavan
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - G Pessina
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - V Pettinacci
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
| | - S Pirro
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - S Pozzi
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Sezione di Milano - Bicocca, I-20126 Milano, Italy
| | - E Previtali
- Dipartimento di Fisica, Università di Milano-Bicocca, I-20126 Milano, Italy
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - A Puiu
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
- Gran Sasso Science Institute, 67100 L'Aquila, Italy
| | - C Rusconi
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
- Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208, USA
| | - K Schäffner
- INFN Laboratori Nazionali del Gran Sasso, I-67100 Assergi (AQ), Italy
| | - C Tomei
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
| | - M Vignati
- Dipartimento di Fisica, Sapienza Università di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
- INFN, Sezione di Roma, P.le Aldo Moro 2, 00185 Roma, Italy
| | - A S Zolotarova
- IRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, France
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Investigation on Rare Nuclear Processes in Hf Nuclides. RADIATION 2022. [DOI: 10.3390/radiation2020017] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/16/2022] Open
Abstract
In this work, a review of recent studies concerning rare nuclear processes in Hf isotopes is presented. In particular, the investigations using HP-Ge spectrometry and Hf-based crystal scintillators are focused; the potentiality and the results of the “source = detector” approach are underlined. In addition, a short introduction concerning the impact of such kind of research in the context of astroparticle and nuclear physics is pointed out. In particular, the study of α decay and double beta decay of 174Hf, 176Hf, 177Hf, 178Hf, 179Hf, 180Hf isotopes either to the ground state or to the lower bounded levels have been discussed. The observation of α decay of 174Hf isotope to the ground state with a T1/2=7.0(1.2)×1016 y is reported and discussed. No decay was detected for α decay of 174Hf isotope at the first excited level of daughter and of 176Hf, 177Hf, 178Hf, 179Hf, 180Hf isotopes either to the ground state or to the lower bounded levels. The T1/2 lower limits for these decays are at the level of 1016–1020 y. Nevertheless, the T1/2 lower limits for the transitions of 176Hf→172Yb (0+→0+) and 177Hf→173Yb (7/2−→5/2−) are near to the theoretical predictions, giving hope to their observation in the near future. All the other experimental limits (∼1016–1020 y) are absolutely far from the theoretical expectations. The experiments investigating the 2ϵ and ϵβ+ processes in 174Hf are also reported; the obtained half-life limits are set at the level of 1016–1018 y. Moreover, we estimate the T1/2 of 2ν2ϵ of 174Hf decay at the level of (0.3–6) × 1021 y (at now the related measured lower limit is 7.1×1016 y).
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Abstract
An overview of searches related to neutrinos of astronomical and astrophysical origin performed within the framework of the Standard-Model Extension is provided. For this effective field theory, key definitions, intriguing physical consequences, and the mathematical formalism are summarized within the neutrino sector to search for effects from a background that could lead to small deviations from Lorentz symmetry. After an introduction to the fundamental theory, examples of various experiments within the astronomical and astrophysical context are provided. Order-of-magnitude bounds of SME coefficients are shown illustratively for the tight constraints that this sector allows us to place on such violations.
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Abstract
Inorganic crystal scintillators play a crucial role in particle detection for various applications in fundamental physics and applied science. The use of such materials as scintillating bolometers, which operate at temperatures as low as 10 mK and detect both heat (phonon) and scintillation signals, significantly extends detectors performance compared to the conventional scintillation counters. In particular, such low-temperature devices offer a high energy resolution in a wide energy interval thanks to a phonon signal detection, while a simultaneous registration of scintillation emitted provides an efficient particle identification tool. This feature is of great importance for a background identification and rejection. Combined with a large variety of elements of interest, which can be embedded in crystal scintillators, scintillating bolometers represent powerful particle detectors for rare-event searches (e.g., rare alpha and beta decays, double-beta decay, dark matter particles, neutrino detection). Here, we review the features and results of low-temperature scintillation detection achieved over a 30-year history of developments of scintillating bolometers and their use in rare-event search experiments.
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6
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Adams DQ, Alduino C, Alfonso K, Avignone FT, Azzolini O, Bari G, Bellini F, Benato G, Biassoni M, Branca A, Brofferio C, Bucci C, Camilleri J, Caminata A, Campani A, Canonica L, Cao XG, Capelli S, Cappelli L, Cardani L, Carniti P, Casali N, Chiesa D, Clemenza M, Copello S, Cosmelli C, Cremonesi O, Creswick RJ, D'Addabbo A, Dafinei I, Davis CJ, Dell'Oro S, Di Domizio S, Dompè V, Fang DQ, Fantini G, Faverzani M, Ferri E, Ferroni F, Fiorini E, Franceschi MA, Freedman SJ, Fu SH, Fujikawa BK, Giachero A, Gironi L, Giuliani A, Gorla P, Gotti C, Gutierrez TD, Han K, Heeger KM, Huang RG, Huang HZ, Johnston J, Keppel G, Kolomensky YG, Ligi C, Ma L, Ma YG, Marini L, Maruyama RH, Mayer D, Mei Y, Moggi N, Morganti S, Napolitano T, Nastasi M, Nikkel J, Nones C, Norman EB, Nucciotti A, Nutini I, O'Donnell T, Ouellet JL, Pagan S, Pagliarone CE, Pagnanini L, Pallavicini M, Pattavina L, Pavan M, Pessina G, Pettinacci V, Pira C, Pirro S, Pozzi S, Previtali E, Puiu A, Rosenfeld C, Rusconi C, Sakai M, Sangiorgio S, Schmidt B, Scielzo ND, Sharma V, Singh V, Sisti M, Speller D, Surukuchi PT, Taffarello L, Terranova F, Tomei C, Vetter KJ, Vignati M, Wagaarachchi SL, Wang BS, Welliver B, Wilson J, Wilson K, Winslow LA, Zimmermann S, Zucchelli S. Measurement of the 2νββ Decay Half-Life of ^{130}Te with CUORE. PHYSICAL REVIEW LETTERS 2021; 126:171801. [PMID: 33988435 DOI: 10.1103/physrevlett.126.171801] [Citation(s) in RCA: 11] [Impact Index Per Article: 3.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/23/2020] [Revised: 03/10/2021] [Accepted: 03/11/2021] [Indexed: 06/12/2023]
Abstract
We measured two-neutrino double beta decay of ^{130}Te using an exposure of 300.7 kg yr accumulated with the CUORE detector. Using a Bayesian analysis to fit simulated spectra to experimental data, it was possible to disentangle all the major background sources and precisely measure the two-neutrino contribution. The half-life is in agreement with past measurements with a strongly reduced uncertainty: T_{1/2}^{2ν}=7.71_{-0.06}^{+0.08}(stat)_{-0.15}^{+0.12}(syst)×10^{20} yr. This measurement is the most precise determination of the ^{130}Te 2νββ decay half-life to date.
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Affiliation(s)
- D Q Adams
- Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208, USA
| | - C Alduino
- Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208, USA
| | - K Alfonso
- Department of Physics and Astronomy, University of California, Los Angeles, California 90095, USA
| | - F T Avignone
- Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208, USA
| | - O Azzolini
- INFN-Laboratori Nazionali di Legnaro, Legnaro (Padova) I-35020, Italy
| | - G Bari
- INFN-Sezione di Bologna, Bologna I-40127, Italy
| | - F Bellini
- Dipartimento di Fisica, Sapienza Università di Roma, Roma I-00185, Italy
- INFN-Sezione di Roma, Roma I-00185, Italy
| | - G Benato
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
| | - M Biassoni
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
| | - A Branca
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - C Brofferio
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - C Bucci
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
| | - J Camilleri
- Center for Neutrino Physics, Virginia Polytechnic Institute and State University, Blacksburg, Virginia 24061, USA
| | - A Caminata
- INFN-Sezione di Genova, Genova I-16146, Italy
| | - A Campani
- INFN-Sezione di Genova, Genova I-16146, Italy
- Dipartimento di Fisica, Università di Genova, Genova I-16146, Italy
| | - L Canonica
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - X G Cao
- Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Institute of Modern Physics, Fudan University, Shanghai 200433, China
| | - S Capelli
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - L Cappelli
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
- Department of Physics, University of California, Berkeley, California 94720, USA
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - L Cardani
- INFN-Sezione di Roma, Roma I-00185, Italy
| | - P Carniti
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - N Casali
- INFN-Sezione di Roma, Roma I-00185, Italy
| | - D Chiesa
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - M Clemenza
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - S Copello
- INFN-Sezione di Genova, Genova I-16146, Italy
- Dipartimento di Fisica, Università di Genova, Genova I-16146, Italy
| | - C Cosmelli
- Dipartimento di Fisica, Sapienza Università di Roma, Roma I-00185, Italy
- INFN-Sezione di Roma, Roma I-00185, Italy
| | - O Cremonesi
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
| | - R J Creswick
- Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208, USA
| | - A D'Addabbo
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
- Gran Sasso Science Institute, L'Aquila I-67100, Italy
| | - I Dafinei
- INFN-Sezione di Roma, Roma I-00185, Italy
| | - C J Davis
- Wright Laboratory, Department of Physics, Yale University, New Haven, Connecticut 06520, USA
| | - S Dell'Oro
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - S Di Domizio
- INFN-Sezione di Genova, Genova I-16146, Italy
- Dipartimento di Fisica, Università di Genova, Genova I-16146, Italy
| | - V Dompè
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
- Gran Sasso Science Institute, L'Aquila I-67100, Italy
| | - D Q Fang
- Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Institute of Modern Physics, Fudan University, Shanghai 200433, China
| | - G Fantini
- Dipartimento di Fisica, Sapienza Università di Roma, Roma I-00185, Italy
- INFN-Sezione di Roma, Roma I-00185, Italy
| | - M Faverzani
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - E Ferri
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - F Ferroni
- INFN-Sezione di Roma, Roma I-00185, Italy
- Gran Sasso Science Institute, L'Aquila I-67100, Italy
| | - E Fiorini
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - M A Franceschi
- INFN-Laboratori Nazionali di Frascati, Frascati (Roma) I-00044, Italy
| | - S J Freedman
- Department of Physics, University of California, Berkeley, California 94720, USA
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - S H Fu
- Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Institute of Modern Physics, Fudan University, Shanghai 200433, China
| | - B K Fujikawa
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - A Giachero
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - L Gironi
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - A Giuliani
- Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France
| | - P Gorla
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
| | - C Gotti
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
| | - T D Gutierrez
- Physics Department, California Polytechnic State University, San Luis Obispo, California 93407, USA
| | - K Han
- INPAC and School of Physics and Astronomy, Shanghai Jiao Tong University; Shanghai Laboratory for Particle Physics and Cosmology, Shanghai 200240, China
| | - K M Heeger
- Wright Laboratory, Department of Physics, Yale University, New Haven, Connecticut 06520, USA
| | - R G Huang
- Department of Physics, University of California, Berkeley, California 94720, USA
| | - H Z Huang
- Department of Physics and Astronomy, University of California, Los Angeles, California 90095, USA
| | - J Johnston
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - G Keppel
- INFN-Laboratori Nazionali di Legnaro, Legnaro (Padova) I-35020, Italy
| | - Yu G Kolomensky
- Department of Physics, University of California, Berkeley, California 94720, USA
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - C Ligi
- INFN-Laboratori Nazionali di Frascati, Frascati (Roma) I-00044, Italy
| | - L Ma
- Department of Physics and Astronomy, University of California, Los Angeles, California 90095, USA
| | - Y G Ma
- Key Laboratory of Nuclear Physics and Ion-beam Application (MOE), Institute of Modern Physics, Fudan University, Shanghai 200433, China
| | - L Marini
- Department of Physics, University of California, Berkeley, California 94720, USA
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - R H Maruyama
- Wright Laboratory, Department of Physics, Yale University, New Haven, Connecticut 06520, USA
| | - D Mayer
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - Y Mei
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - N Moggi
- INFN-Sezione di Bologna, Bologna I-40127, Italy
- Dipartimento di Fisica e Astronomia, Alma Mater Studiorum-Università di Bologna, Bologna I-40127, Italy
| | - S Morganti
- INFN-Sezione di Roma, Roma I-00185, Italy
| | - T Napolitano
- INFN-Laboratori Nazionali di Frascati, Frascati (Roma) I-00044, Italy
| | - M Nastasi
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - J Nikkel
- Wright Laboratory, Department of Physics, Yale University, New Haven, Connecticut 06520, USA
| | - C Nones
- IRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, France
| | - E B Norman
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
- Department of Nuclear Engineering, University of California, Berkeley, California 94720, USA
| | - A Nucciotti
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - I Nutini
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - T O'Donnell
- Center for Neutrino Physics, Virginia Polytechnic Institute and State University, Blacksburg, Virginia 24061, USA
| | - J L Ouellet
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - S Pagan
- Wright Laboratory, Department of Physics, Yale University, New Haven, Connecticut 06520, USA
| | - C E Pagliarone
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
- Dipartimento di Ingegneria Civile e Meccanica, Università degli Studi di Cassino e del Lazio Meridionale, Cassino I-03043, Italy
| | - L Pagnanini
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
- Gran Sasso Science Institute, L'Aquila I-67100, Italy
| | - M Pallavicini
- INFN-Sezione di Genova, Genova I-16146, Italy
- Dipartimento di Fisica, Università di Genova, Genova I-16146, Italy
| | - L Pattavina
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
| | - M Pavan
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - G Pessina
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
| | | | - C Pira
- INFN-Laboratori Nazionali di Legnaro, Legnaro (Padova) I-35020, Italy
| | - S Pirro
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
| | - S Pozzi
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - E Previtali
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - A Puiu
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
- Gran Sasso Science Institute, L'Aquila I-67100, Italy
| | - C Rosenfeld
- Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208, USA
| | - C Rusconi
- Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208, USA
- INFN-Laboratori Nazionali del Gran Sasso, Assergi (L'Aquila) I-67100, Italy
| | - M Sakai
- Department of Physics, University of California, Berkeley, California 94720, USA
| | - S Sangiorgio
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - B Schmidt
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - N D Scielzo
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - V Sharma
- Center for Neutrino Physics, Virginia Polytechnic Institute and State University, Blacksburg, Virginia 24061, USA
| | - V Singh
- Department of Physics, University of California, Berkeley, California 94720, USA
| | - M Sisti
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
| | - D Speller
- Department of Physics and Astronomy, The Johns Hopkins University, 3400 North Charles Street Baltimore, Maryland 21211, USA
| | - P T Surukuchi
- Wright Laboratory, Department of Physics, Yale University, New Haven, Connecticut 06520, USA
| | | | - F Terranova
- INFN-Sezione di Milano Bicocca, Milano I-20126, Italy
- Dipartimento di Fisica, Università di Milano-Bicocca, Milano I-20126, Italy
| | - C Tomei
- INFN-Sezione di Roma, Roma I-00185, Italy
| | - K J Vetter
- Department of Physics, University of California, Berkeley, California 94720, USA
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - M Vignati
- INFN-Sezione di Roma, Roma I-00185, Italy
| | - S L Wagaarachchi
- Department of Physics, University of California, Berkeley, California 94720, USA
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - B S Wang
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
- Department of Nuclear Engineering, University of California, Berkeley, California 94720, USA
| | - B Welliver
- Nuclear Science Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - J Wilson
- Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208, USA
| | - K Wilson
- Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208, USA
| | - L A Winslow
- Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - S Zimmermann
- Engineering Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
| | - S Zucchelli
- INFN-Sezione di Bologna, Bologna I-40127, Italy
- Dipartimento di Fisica e Astronomia, Alma Mater Studiorum-Università di Bologna, Bologna I-40127, Italy
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Techniques for Background Identification in the Search for Rare Processes with Crystal Scintillators. PHYSICS 2021. [DOI: 10.3390/physics3020015] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/16/2022]
Abstract
In astroparticle, nuclear and subnuclear physics, low-counting experiments play an increasingly important role in the investigation of rare processes such as dark matter, double beta decay, some neutrino processes and low-background spectrometry. Extremely low-background features are more and more required to produce detectors and apparata of suitable sensitivity. Over time, a great deal of interest and attention in developing experimental techniques suitable to improve, verify and maintain the radiopurity of these detectors has arisen. In this paper, the characterization of inorganic crystal scintillators (such as, e.g., NaI(Tl), ZnWO4 and CdWO4) using α, β and γ radioactive sources and the main experimental techniques applied in the field to quantitatively identify the radioactive contaminants are highlighted; in particular, we focus on inorganic crystal scintillators, widely used in rare processes investigation, considering their applications at noncryogenic temperatures in the framework of the DAMA experiment activities at the Gran Sasso National Laboratory of the INFN (National Institute for Nuclear Physics, INFN).
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Abstract
The investigation of 2β decay is an important issue in modern physics, allowing the test of the Standard Model of elementary particles and the study of the nature and properties of neutrinos. The crystal scintillators, especially made of isotopically-enriched materials, are powerful detectors for 2β decay experiments thanks to the high radiopurity level and the possibility to realize the calorimetric “source = detector” approach with a high detection efficiency. For the moment, the 2ν2β processes have been observed at the level of 1019–1024 years with enriched crystals; the sensitivity to the 0ν mode have reached the level of 1024–1026 years in some decay channels for different nuclides allowing one to calculate the upper limits on the effective mass of the Majorana neutrino at the level of 0.1–0.6 eV. The paper is intended to be a review on the latest results to investigate 2β processes with crystal scintillators enriched in 48Ca, 106Cd, and 116Cd.
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Initial State Interaction for the 20Ne + 130Te and 18O + 116Sn Systems at 15.3 AMeV from Elastic and Inelastic Scattering Measurements. UNIVERSE 2021. [DOI: 10.3390/universe7030058] [Citation(s) in RCA: 13] [Impact Index Per Article: 4.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/16/2022]
Abstract
Double charge exchange (DCE) reactions could provide experimentally driven information about nuclear matrix elements of interest in the context of neutrinoless double-β decay. To achieve this goal, a detailed description of the reaction mechanism is mandatory. This requires the full characterization of the initial and final-state interactions, which are poorly known for many of the projectile-target systems involved in future DCE studies. Among these, we intend to study the 20Ne + 130Te and 18O + 116Sn systems at 15.3 AMeV, which are particularly relevant due to their connection with the 130Te→130Xe and 116Cd→116Sn double-β decays. We measure the elastic and inelastic scattering cross-section angular distributions and compare them with theoretical calculations performed in the optical model, one-step distorted wave Born approximation, and coupled-channel approaches using the São Paulo double-folding optical potential. A good description of the experimental data in the whole explored range of transferred momenta is obtained provided that couplings with the 21+ states of the projectile and target are explicitly included within the coupled-channel approach. These results are relevant also in the analysis of other quasi-elastic reaction channels in these systems, in which the same couplings should be included.
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10
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Abstract
In this paper we review results obtained in the searches of double beta decays to excited states of the daughter nuclei and illustrate the related experimental techniques. In particular, we describe in some detail the only two cases in which the transition has been observed; that is the 2β−(0+→01+) decay of 100Mo and 150Nd nuclides. Moreover, the most significant results in terms of lower limits on the half-life are also summarized.
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11
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Search for Double Beta Decay of 106Cd with an Enriched 106CdWO4 Crystal Scintillator in Coincidence with CdWO4 Scintillation Counters. UNIVERSE 2020. [DOI: 10.3390/universe6100182] [Citation(s) in RCA: 12] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/16/2022]
Abstract
Studies on double beta decay processes in 106Cd were performed by using a cadmium tungstate scintillator enriched in 106Cd at 66% (106CdWO4) with two CdWO4 scintillation counters (with natural Cd composition). No effect was observed in the data that accumulated over 26,033 h. New improved half-life limits were set on the different channels and modes of the 106Cd double beta decay at level of limT1/2∼1020−1022 yr. The limit for the two neutrino electron capture with positron emission in 106Cd to the ground state of 106Pd, T1/22νECβ+≥2.1×1021 yr, was set by the analysis of the 106CdWO4 data in coincidence with the energy release 511 keV in both CdWO4 counters. The sensitivity approaches the theoretical predictions for the decay half-life that are in the range T1/2∼1021−1022 yr. The resonant neutrinoless double-electron capture to the 2718 keV excited state of 106Pd is restricted at the level of T1/20ν2K≥2.9×1021 yr.
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12
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Abstract
All existing positive results on two-neutrino double beta decay and two-neutrino double electron capture in different nuclei have been analyzed. Weighted average and recommended half-life values for 48Ca, 76Ge, 82Se, 96Zr, 100Mo, 100Mo - 100Ru (01+), 116Cd, 128Te, 130Te, 136Xe, 150Nd, 150Nd - 150Sm (01+), 238U, 78Kr, 124Xe and 130Ba have been obtained. Given the measured half-life values, effective nuclear matrix elements for all these transitions were calculated.
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13
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Recent Developments and Results on Double Beta Decays with Crystal Scintillators and HPGe Spectrometry. UNIVERSE 2018. [DOI: 10.3390/universe4120147] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 11/17/2022]
Abstract
Recent developments, results, and perspectives arising from double beta decay experiments at the Gran Sasso National Laboratory (LNGS) of the INFN by using HPGe detectors and crystal scintillators and by exploiting various approaches and different isotopes are summarized. The measurements here presented have been performed in the experimental set-ups of the DAMA collaboration. These setups are optimized for low-background studies and operate deep underground at LNGS. The presented results are of significant value to the field, and the sensitivity achieved for some of the considered isotopes is one of the best available to date.
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