Double-weak decays of Xe-124 and Xe-136 in the XENON1T and XENONnT experiments

E. Aprile,K. Abe,F. Agostini,S. Ahmed Maouloud,M. Alfonsi,L. Althueser,B. Andrieu,E. Angelino,J. R. Angevaare,V. C. Antochi,D. Anton Martin,F. Arneodo,L. Baudis,A. L. Baxter,L. Bellagamba,R. Biondi,A. Bismark,A. Brown,S. Bruenner,G. Bruno,R. Budnik,C. Cai,C. Capelli,J. M. R. Cardoso,D. Cichon,M. Clark,A. P. Colijn,J. Conrad,J. J. Cuenca-Garcia,J. P. Cussonneau,M. P. Decowski,P. Di Gangi,S. Di Pede,A. Di Giovanni,R. Di Stefano,S. Diglio,K. Eitel,A. Elykov,S. Farrell,A. D. Ferella,H. Fischer,W. Fulgione,P. Gaemers,R. Gaior,A. Gallo Rosso,M. Galloway,F. Gao,R. Glade-Beucke,L. Grandi,J. Grigat, M. Guida,A. Higuera,C. Hils,L. Hoetzsch,J. Howlett,M. Iacovacci,Y. Itow,J. Jakob,F. Joerg,A. Joy,N. Kato,M. Kara,P. Kavrigin,S. Kazama,M. Kobayashi,G. Koltman,A. Kopec,H. Landsman,R. F. Lang,L. Levinson,I Li,S. Li,S. Liang,S. Lindemann,M. Lindner,K. Liu,J. Loizeau,F. Lombardi,J. Long,J. A. M. Lopes,Y. Ma,C. Macolino,J. Mahlstedt,A. Mancuso,L. Manenti,A. Manfredini,F. Marignetti,T. Marrodan Undagoitia,K. Martens,J. Masbou,D. Masson,E. Masson,S. Mastroianni,M. Messina,K. Miuchi,K. Mizukoshi,A. Molinario,S. Moriyama,K. Mora,Y. Mosbacher,M. Murra,J. Mueller,K. Ni,U. Oberlack,B. Paetsch,J. Palacio,R. Peres,J. Pienaar,M. Pierre,V Pizzella,G. Plante,J. Qi,J. Qin, D. Ramirez Garcia,S. Reichard,A. Rocchetti,N. Rupp,L. Sanchez,J. M. F. dos Santos,I Sarnoff,G. Sartorelli,J. Schreiner,D. Schulte,P. Schulte,H. Schulze Eissing,M. Schumann,L. Scotto Lavina,M. Selvi,F. Semeria,P. Shagin,S. Shi,E. Shockley,M. Silva,H. Simgen,A. Takeda,P-L Tan,A. Terliuk, D. Thers,F. Toschi,G. Trinchero,C. Tunnell,F. Tonnies,K. Valerius,G. Volta,Y. Wei,C. Weinheimer,M. Weiss,D. Wenz,C. Wittweg,T. Wolf,Z. Xu,M. Yamashita,L. Yang,J. Ye,L. Yuan,G. Zavattini,S. Zerbo,M. Zhong,T. Zhu

PHYSICAL REVIEW C(2022)

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摘要
We present results on the search for two-neutrino double-electron capture (2 nu ECEC) of Xe-124 and neutrinoless double-beta decay (OW) of 136Xe in XENON1T. We consider captures from the K shell up to the N shell in the 2 nu ECEC signal model and measure a total half-life of T-1/2(2 nu EcEc) = (1.1 +/- 0.2(stat) +/- 0.1(sys)) x 10(22) yr with a 0.87 kg yr isotope exposure. The statistical significance of the signal is 7.00. We use XENON1T data with 36.16 kg yr of Xe-136 exposure to search for O nu beta beta. We find no evidence of a signal and set a lower limit on the half-life of T-1/2(beta beta) > 1.2 x 10(24) yr at 90% CL. This is the best result from a dark matter detector without an enriched target to date. We also report projections on the sensitivity of XENONnT to OW. Assuming a 275 kg yr Xe-136 exposure, the expected sensitivity is T-1/2(0 nu) > 2.1 x 10(25) yr at 90% CL, corresponding to an effective Majorana mass range of < m(beta beta)> < (0.19-0.59) eV/c(2).
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