Search for double-beta decay of $$\mathrm {^{130}Te}$$ 130 Te to the $$0^+$$ 0 + states of $$\mathrm {^{130}Xe}$$ 130 Xe with CUORE
Abstract The CUORE experiment is a large bolometric array searching for the lepton number violating neutrino-less double beta decay ( $$0\nu \beta \beta $$ 0 ν β β ) in the isotope $$\mathrm {^{130}Te}$$ 130 Te . In this work we present the latest results on two searches for the double beta decay (D...
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| Format: | Article |
| Language: | English |
| Published: |
SpringerOpen
2021-07-01
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| Series: | European Physical Journal C: Particles and Fields |
| Online Access: | https://doi.org/10.1140/epjc/s10052-021-09317-z |
| _version_ | 1819034922060349440 |
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| author | D. Q. Adams C. Alduino K. Alfonso F. T. III Avignone O. Azzolini G. Bari F. Bellini G. Benato M. Biassoni A. Branca C. Brofferio C. Bucci J. Camilleri A. Caminata A. Campani L. Canonica X. G. Cao S. Capelli L. Cappelli L. Cardani P. Carniti N. Casali E. Celi D. Chiesa M. Clemenza S. Copello C. Cosmelli O. Cremonesi R. J. Creswick A. D’Addabbo I. Dafinei C. J. Davis S. Dell’Oro S. Di Domizio V. Dompè D. Q. Fang G. Fantini M. Faverzani E. Ferri F. Ferroni E. Fiorini M. A. Franceschi S. J. Freedman S. H. Fu B. K. Fujikawa A. Giachero L. Gironi A. Giuliani P. Gorla C. Gotti T. D. Gutierrez K. Han K. M. Heeger R. G. Huang H. Z. Huang J. Johnston G. Keppel Yu. G. Kolomensky C. Ligi L. Ma Y. G. Ma L. Marini R. H. Maruyama D. Mayer Y. Mei N. Moggi S. Morganti T. Napolitano M. Nastasi J. Nikkel C. Nones E. B. Norman A. Nucciotti I. Nutini T. O’Donnell J. L. Ouellet S. Pagan C. E. Pagliarone L. Pagnanini M. Pallavicini L. Pattavina M. Pavan G. Pessina V. Pettinacci C. Pira S. Pirro S. Pozzi E. Previtali A. Puiu C. Rosenfeld C. Rusconi M. Sakai S. Sangiorgio B. Schmidt N. D. Scielzo V. Sharma V. Singh M. Sisti D. Speller P. T. Surukuchi L. Taffarello F. Terranova C. Tomei K. J. Vetter M. Vignati S. L. Wagaarachchi B. S. Wang B. Welliver J. Wilson K. Wilson L. A. Winslow S. Zimmermann S. Zucchelli |
| author_facet | D. Q. Adams C. Alduino K. Alfonso F. T. III Avignone O. Azzolini G. Bari F. Bellini G. Benato M. Biassoni A. Branca C. Brofferio C. Bucci J. Camilleri A. Caminata A. Campani L. Canonica X. G. Cao S. Capelli L. Cappelli L. Cardani P. Carniti N. Casali E. Celi D. Chiesa M. Clemenza S. Copello C. Cosmelli O. Cremonesi R. J. Creswick A. D’Addabbo I. Dafinei C. J. Davis S. Dell’Oro S. Di Domizio V. Dompè D. Q. Fang G. Fantini M. Faverzani E. Ferri F. Ferroni E. Fiorini M. A. Franceschi S. J. Freedman S. H. Fu B. K. Fujikawa A. Giachero L. Gironi A. Giuliani P. Gorla C. Gotti T. D. Gutierrez K. Han K. M. Heeger R. G. Huang H. Z. Huang J. Johnston G. Keppel Yu. G. Kolomensky C. Ligi L. Ma Y. G. Ma L. Marini R. H. Maruyama D. Mayer Y. Mei N. Moggi S. Morganti T. Napolitano M. Nastasi J. Nikkel C. Nones E. B. Norman A. Nucciotti I. Nutini T. O’Donnell J. L. Ouellet S. Pagan C. E. Pagliarone L. Pagnanini M. Pallavicini L. Pattavina M. Pavan G. Pessina V. Pettinacci C. Pira S. Pirro S. Pozzi E. Previtali A. Puiu C. Rosenfeld C. Rusconi M. Sakai S. Sangiorgio B. Schmidt N. D. Scielzo V. Sharma V. Singh M. Sisti D. Speller P. T. Surukuchi L. Taffarello F. Terranova C. Tomei K. J. Vetter M. Vignati S. L. Wagaarachchi B. S. Wang B. Welliver J. Wilson K. Wilson L. A. Winslow S. Zimmermann S. Zucchelli |
| author_sort | D. Q. Adams |
| collection | DOAJ |
| description | Abstract The CUORE experiment is a large bolometric array searching for the lepton number violating neutrino-less double beta decay ( $$0\nu \beta \beta $$ 0 ν β β ) in the isotope $$\mathrm {^{130}Te}$$ 130 Te . In this work we present the latest results on two searches for the double beta decay (DBD) of $$\mathrm {^{130}Te}$$ 130 Te to the first $$0^{+}_2$$ 0 2 + excited state of $$\mathrm {^{130}Xe}$$ 130 Xe : the $$0\nu \beta \beta $$ 0 ν β β decay and the Standard Model-allowed two-neutrinos double beta decay ( $$2\nu \beta \beta $$ 2 ν β β ). Both searches are based on a 372.5 kg $$\times $$ × yr TeO $$_2$$ 2 exposure. The de-excitation gamma rays emitted by the excited Xe nucleus in the final state yield a unique signature, which can be searched for with low background by studying coincident events in two or more bolometers. The closely packed arrangement of the CUORE crystals constitutes a significant advantage in this regard. The median limit setting sensitivities at 90% Credible Interval (C.I.) of the given searches were estimated as $$\mathrm {S^{0\nu }_{1/2} = 5.6 \times 10^{24} \, \mathrm {yr}}$$ S 1 / 2 0 ν = 5.6 × 10 24 yr for the $${0\nu \beta \beta }$$ 0 ν β β decay and $$\mathrm {S^{2\nu }_{1/2} = 2.1 \times 10^{24} \, \mathrm {yr}}$$ S 1 / 2 2 ν = 2.1 × 10 24 yr for the $${2\nu \beta \beta }$$ 2 ν β β decay. No significant evidence for either of the decay modes was observed and a Bayesian lower bound at $$90\%$$ 90 % C.I. on the decay half lives is obtained as: $$\mathrm {(T_{1/2})^{0\nu }_{0^+_2} > 5.9 \times 10^{24} \, \mathrm {yr}}$$ ( T 1 / 2 ) 0 2 + 0 ν > 5.9 × 10 24 yr for the $$0\nu \beta \beta $$ 0 ν β β mode and $$\mathrm {(T_{1/2})^{2\nu }_{0^+_2} > 1.3 \times 10^{24} \, \mathrm {yr}}$$ ( T 1 / 2 ) 0 2 + 2 ν > 1.3 × 10 24 yr for the $$2\nu \beta \beta $$ 2 ν β β mode. These represent the most stringent limits on the DBD of $$^{130}$$ 130 Te to excited states and improve by a factor $$\sim 5$$ ∼ 5 the previous results on this process. |
| first_indexed | 2024-12-21T07:41:25Z |
| format | Article |
| id | doaj.art-1eced73e316e4b50a61402429509e45c |
| institution | Directory Open Access Journal |
| issn | 1434-6044 1434-6052 |
| language | English |
| last_indexed | 2024-12-21T07:41:25Z |
| publishDate | 2021-07-01 |
| publisher | SpringerOpen |
| record_format | Article |
| series | European Physical Journal C: Particles and Fields |
| spelling | doaj.art-1eced73e316e4b50a61402429509e45c2022-12-21T19:11:19ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-07-0181711410.1140/epjc/s10052-021-09317-zSearch for double-beta decay of $$\mathrm {^{130}Te}$$ 130 Te to the $$0^+$$ 0 + states of $$\mathrm {^{130}Xe}$$ 130 Xe with CUORED. Q. Adams0C. Alduino1K. Alfonso2F. T. III Avignone3O. Azzolini4G. Bari5F. Bellini6G. Benato7M. Biassoni8A. Branca9C. Brofferio10C. Bucci11J. Camilleri12A. Caminata13A. Campani14L. Canonica15X. G. Cao16S. Capelli17L. Cappelli18L. Cardani19P. Carniti20N. Casali21E. Celi22D. Chiesa23M. Clemenza24S. Copello25C. Cosmelli26O. Cremonesi27R. J. Creswick28A. D’Addabbo29I. Dafinei30C. J. Davis31S. Dell’Oro32S. Di Domizio33V. Dompè34D. Q. Fang35G. Fantini36M. Faverzani37E. Ferri38F. Ferroni39E. Fiorini40M. A. Franceschi41S. J. Freedman42S. H. Fu43B. K. Fujikawa44A. Giachero45L. Gironi46A. Giuliani47P. Gorla48C. Gotti49T. D. Gutierrez50K. Han51K. M. Heeger52R. G. Huang53H. Z. Huang54J. Johnston55G. Keppel56Yu. G. Kolomensky57C. Ligi58L. Ma59Y. G. Ma60L. Marini61R. H. Maruyama62D. Mayer63Y. Mei64N. Moggi65S. Morganti66T. Napolitano67M. Nastasi68J. Nikkel69C. Nones70E. B. Norman71A. Nucciotti72I. Nutini73T. O’Donnell74J. L. Ouellet75S. Pagan76C. E. Pagliarone77L. Pagnanini78M. Pallavicini79L. Pattavina80M. Pavan81G. Pessina82V. Pettinacci83C. Pira84S. Pirro85S. Pozzi86E. Previtali87A. Puiu88C. Rosenfeld89C. Rusconi90M. Sakai91S. Sangiorgio92B. Schmidt93N. D. Scielzo94V. Sharma95V. Singh96M. Sisti97D. Speller98P. T. Surukuchi99L. Taffarello100F. Terranova101C. Tomei102K. J. Vetter103M. Vignati104S. L. Wagaarachchi105B. S. Wang106B. Welliver107J. Wilson108K. Wilson109L. A. Winslow110S. Zimmermann111S. Zucchelli112Department of Physics and Astronomy, University of South CarolinaDepartment of Physics and Astronomy, University of South CarolinaDepartment of Physics and Astronomy, University of CaliforniaDepartment of Physics and Astronomy, University of South CarolinaINFN–Laboratori Nazionali di LegnaroINFN–Sezione di BolognaDipartimento di Fisica, Sapienza Università di RomaINFN–Laboratori Nazionali del Gran SassoINFN–Sezione di Milano-BicoccaINFN–Sezione di Milano-BicoccaINFN–Sezione di Milano-BicoccaINFN–Laboratori Nazionali del Gran SassoCenter for Neutrino Physics, Virginia Polytechnic Institute and State UniversityINFN–Sezione di GenovaINFN–Sezione di GenovaINFN–Laboratori Nazionali del Gran SassoKey Laboratory of Nuclear Physics and Ion-beam Application (MOE), Institute of Modern Physics, Fudan UniversityINFN–Sezione di Milano-BicoccaINFN–Laboratori Nazionali del Gran SassoINFN–Sezione di RomaINFN–Sezione di Milano-BicoccaINFN–Sezione di RomaINFN–Laboratori Nazionali del Gran SassoINFN–Sezione di Milano-BicoccaINFN–Sezione di Milano-BicoccaINFN–Sezione di GenovaDipartimento di Fisica, Sapienza Università di RomaINFN–Sezione di Milano-BicoccaDepartment of Physics and Astronomy, University of South CarolinaINFN–Laboratori Nazionali del Gran SassoINFN–Sezione di RomaWright Laboratory, Department of Physics, Yale UniversityINFN–Sezione di Milano-BicoccaINFN–Sezione di GenovaINFN–Laboratori Nazionali del Gran SassoKey Laboratory of Nuclear Physics and Ion-beam Application (MOE), Institute of Modern Physics, Fudan UniversityDipartimento di Fisica, Sapienza Università di RomaINFN–Sezione di Milano-BicoccaINFN–Sezione di Milano-BicoccaINFN–Sezione di RomaINFN–Sezione di Milano-BicoccaINFN–Laboratori Nazionali di FrascatiDepartment of Physics, University of CaliforniaKey Laboratory of Nuclear Physics and Ion-beam Application (MOE), Institute of Modern Physics, Fudan UniversityNuclear Science Division, Lawrence Berkeley National LaboratoryINFN–Sezione di Milano-BicoccaINFN–Sezione di Milano-BicoccaUniversité Paris-Saclay, CNRS/IN2P3, IJCLabINFN–Laboratori Nazionali del Gran SassoINFN–Sezione di Milano-BicoccaPhysics Department, California Polytechnic State UniversityINPAC and School of Physics and Astronomy, Shanghai Laboratory for Particle Physics and Cosmology, Shanghai Jiao Tong UniversityWright Laboratory, Department of Physics, Yale UniversityDepartment of Physics, University of CaliforniaDepartment of Physics and Astronomy, University of CaliforniaMassachusetts Institute of TechnologyINFN–Laboratori Nazionali di LegnaroDepartment of Physics, University of CaliforniaINFN–Laboratori Nazionali di FrascatiDepartment of Physics and Astronomy, University of CaliforniaKey Laboratory of Nuclear Physics and Ion-beam Application (MOE), Institute of Modern Physics, Fudan UniversityDepartment of Physics, University of CaliforniaWright Laboratory, Department of Physics, Yale UniversityMassachusetts Institute of TechnologyNuclear Science Division, Lawrence Berkeley National LaboratoryINFN–Sezione di BolognaINFN–Sezione di RomaINFN–Laboratori Nazionali di FrascatiINFN–Sezione di Milano-BicoccaWright Laboratory, Department of Physics, Yale UniversityService de Physique des Particules, CEA/SaclayLawrence Livermore National LaboratoryINFN–Sezione di Milano-BicoccaINFN–Sezione di Milano-BicoccaCenter for Neutrino Physics, Virginia Polytechnic Institute and State UniversityMassachusetts Institute of TechnologyWright Laboratory, Department of Physics, Yale UniversityINFN–Laboratori Nazionali del Gran SassoINFN–Laboratori Nazionali del Gran SassoINFN–Sezione di GenovaINFN–Laboratori Nazionali del Gran SassoINFN–Sezione di Milano-BicoccaINFN–Sezione di Milano-BicoccaINFN–Sezione di RomaINFN–Laboratori Nazionali di LegnaroINFN–Laboratori Nazionali del Gran SassoINFN–Sezione di Milano-BicoccaINFN–Sezione di Milano-BicoccaINFN–Laboratori Nazionali del Gran SassoDepartment of Physics and Astronomy, University of South CarolinaDepartment of Physics and Astronomy, University of South CarolinaDepartment of Physics, University of CaliforniaLawrence Livermore National LaboratoryNuclear Science Division, Lawrence Berkeley National LaboratoryLawrence Livermore National LaboratoryCenter for Neutrino Physics, Virginia Polytechnic Institute and State UniversityDepartment of Physics, University of CaliforniaINFN–Sezione di Milano-BicoccaDepartment of Physics and Astronomy, The Johns Hopkins UniversityWright Laboratory, Department of Physics, Yale UniversityINFN–Sezione di PadovaINFN–Sezione di Milano-BicoccaINFN–Sezione di RomaDepartment of Physics, University of CaliforniaINFN–Sezione di RomaDepartment of Physics, University of CaliforniaLawrence Livermore National LaboratoryNuclear Science Division, Lawrence Berkeley National LaboratoryDepartment of Physics and Astronomy, University of South CarolinaDepartment of Physics and Astronomy, University of South CarolinaMassachusetts Institute of TechnologyEngineering Division, Lawrence Berkeley National LaboratoryINFN–Sezione di BolognaAbstract The CUORE experiment is a large bolometric array searching for the lepton number violating neutrino-less double beta decay ( $$0\nu \beta \beta $$ 0 ν β β ) in the isotope $$\mathrm {^{130}Te}$$ 130 Te . In this work we present the latest results on two searches for the double beta decay (DBD) of $$\mathrm {^{130}Te}$$ 130 Te to the first $$0^{+}_2$$ 0 2 + excited state of $$\mathrm {^{130}Xe}$$ 130 Xe : the $$0\nu \beta \beta $$ 0 ν β β decay and the Standard Model-allowed two-neutrinos double beta decay ( $$2\nu \beta \beta $$ 2 ν β β ). Both searches are based on a 372.5 kg $$\times $$ × yr TeO $$_2$$ 2 exposure. The de-excitation gamma rays emitted by the excited Xe nucleus in the final state yield a unique signature, which can be searched for with low background by studying coincident events in two or more bolometers. The closely packed arrangement of the CUORE crystals constitutes a significant advantage in this regard. The median limit setting sensitivities at 90% Credible Interval (C.I.) of the given searches were estimated as $$\mathrm {S^{0\nu }_{1/2} = 5.6 \times 10^{24} \, \mathrm {yr}}$$ S 1 / 2 0 ν = 5.6 × 10 24 yr for the $${0\nu \beta \beta }$$ 0 ν β β decay and $$\mathrm {S^{2\nu }_{1/2} = 2.1 \times 10^{24} \, \mathrm {yr}}$$ S 1 / 2 2 ν = 2.1 × 10 24 yr for the $${2\nu \beta \beta }$$ 2 ν β β decay. No significant evidence for either of the decay modes was observed and a Bayesian lower bound at $$90\%$$ 90 % C.I. on the decay half lives is obtained as: $$\mathrm {(T_{1/2})^{0\nu }_{0^+_2} > 5.9 \times 10^{24} \, \mathrm {yr}}$$ ( T 1 / 2 ) 0 2 + 0 ν > 5.9 × 10 24 yr for the $$0\nu \beta \beta $$ 0 ν β β mode and $$\mathrm {(T_{1/2})^{2\nu }_{0^+_2} > 1.3 \times 10^{24} \, \mathrm {yr}}$$ ( T 1 / 2 ) 0 2 + 2 ν > 1.3 × 10 24 yr for the $$2\nu \beta \beta $$ 2 ν β β mode. These represent the most stringent limits on the DBD of $$^{130}$$ 130 Te to excited states and improve by a factor $$\sim 5$$ ∼ 5 the previous results on this process.https://doi.org/10.1140/epjc/s10052-021-09317-z |
| spellingShingle | D. Q. Adams C. Alduino K. Alfonso F. T. III Avignone O. Azzolini G. Bari F. Bellini G. Benato M. Biassoni A. Branca C. Brofferio C. Bucci J. Camilleri A. Caminata A. Campani L. Canonica X. G. Cao S. Capelli L. Cappelli L. Cardani P. Carniti N. Casali E. Celi D. Chiesa M. Clemenza S. Copello C. Cosmelli O. Cremonesi R. J. Creswick A. D’Addabbo I. Dafinei C. J. Davis S. Dell’Oro S. Di Domizio V. Dompè D. Q. Fang G. Fantini M. Faverzani E. Ferri F. Ferroni E. Fiorini M. A. Franceschi S. J. Freedman S. H. Fu B. K. Fujikawa A. Giachero L. Gironi A. Giuliani P. Gorla C. Gotti T. D. Gutierrez K. Han K. M. Heeger R. G. Huang H. Z. Huang J. Johnston G. Keppel Yu. G. Kolomensky C. Ligi L. Ma Y. G. Ma L. Marini R. H. Maruyama D. Mayer Y. Mei N. Moggi S. Morganti T. Napolitano M. Nastasi J. Nikkel C. Nones E. B. Norman A. Nucciotti I. Nutini T. O’Donnell J. L. Ouellet S. Pagan C. E. Pagliarone L. Pagnanini M. Pallavicini L. Pattavina M. Pavan G. Pessina V. Pettinacci C. Pira S. Pirro S. Pozzi E. Previtali A. Puiu C. Rosenfeld C. Rusconi M. Sakai S. Sangiorgio B. Schmidt N. D. Scielzo V. Sharma V. Singh M. Sisti D. Speller P. T. Surukuchi L. Taffarello F. Terranova C. Tomei K. J. Vetter M. Vignati S. L. Wagaarachchi B. S. Wang B. Welliver J. Wilson K. Wilson L. A. Winslow S. Zimmermann S. Zucchelli Search for double-beta decay of $$\mathrm {^{130}Te}$$ 130 Te to the $$0^+$$ 0 + states of $$\mathrm {^{130}Xe}$$ 130 Xe with CUORE European Physical Journal C: Particles and Fields |
| title | Search for double-beta decay of $$\mathrm {^{130}Te}$$ 130 Te to the $$0^+$$ 0 + states of $$\mathrm {^{130}Xe}$$ 130 Xe with CUORE |
| title_full | Search for double-beta decay of $$\mathrm {^{130}Te}$$ 130 Te to the $$0^+$$ 0 + states of $$\mathrm {^{130}Xe}$$ 130 Xe with CUORE |
| title_fullStr | Search for double-beta decay of $$\mathrm {^{130}Te}$$ 130 Te to the $$0^+$$ 0 + states of $$\mathrm {^{130}Xe}$$ 130 Xe with CUORE |
| title_full_unstemmed | Search for double-beta decay of $$\mathrm {^{130}Te}$$ 130 Te to the $$0^+$$ 0 + states of $$\mathrm {^{130}Xe}$$ 130 Xe with CUORE |
| title_short | Search for double-beta decay of $$\mathrm {^{130}Te}$$ 130 Te to the $$0^+$$ 0 + states of $$\mathrm {^{130}Xe}$$ 130 Xe with CUORE |
| title_sort | search for double beta decay of mathrm 130 te 130 te to the 0 0 states of mathrm 130 xe 130 xe with cuore |
| url | https://doi.org/10.1140/epjc/s10052-021-09317-z |
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