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Ram\\'irez Garc\\'ia, D. Schulte, D. Thers, D. Wenz, E. Angelino, E. Aprile, E. Masson, E. Shockley, F. Agostini, F. Arneodo, F. Gao, F. Joerg, F. Lombardi, F. Marignetti, F. Semeria, F. T\\\"onnies, F. Toschi, G. Bruno, G. Koltman, G. Plante, G. Sartorelli, G. Trinchero, G. Volta, G. Zavattini, H. Fischer, H. Landsman, H. Schulze Ei{\\ss}ing, H. Simgen, I. Li, I. Sarnoff, J. A. M. Lopes, J. Conrad, J. Grigat, J. Howlett, J. Jakob, J. J. Cuenca-Garc\\'ia, J. Loizeau, J. Long, J. Mahlstedt, J. Masbou, J. M. F. dos Santos, J. M. R. Cardoso, J. M\\\"uller, J. Palacio, J. P. Cussonneau, J. Pienaar, J. Qi, J. Qin, J. R. Angevaare, J. Schreiner, J. Ye, K. Abe, K. Eitel, K. Liu, K. Martens, K. Miuchi, K. Mizukoshi, K. Mor{\\aa}, K. Ni, K. Valerius, L. Althueser, L. Baudis, L. Bellagamba, L. Grandi, L. Hoetzsch, L. Levinson, L. Manenti, L. Sanchez, L. Scotto Lavina, L. Yang, L. Yuan, M. Alfonsi, M. Clark, M. Galloway, M. Guida, M. Iacovacci, M. Kara, M. Kobayashi, M. Lindner, M. Messina, M. Murra, M. P. Decowski, M. Pierre, M. Schumann, M. Selvi, M. Silva, M. Weiss, M. Yamashita, M. Zhong, N. Kato, N. Rupp, P. Di Gangi, P. Gaemers, P. Kavrigin, P.-L. Tan, P. Schulte, P. Shagin, R. Biondi, R. Budnik, R. Di Stefano, R. F. Lang, R. Gaior, R. Glade-Beucke, R. Peres, S. Ahmed Maouloud, S. Bruenner, S. Diglio, S. Di Pede, S. Farrell, S. Kazama, S. Li, S. Liang, S. Lindemann, S. Mastroianni, S. Moriyama, S. Reichard, S. Shi, S. Zerbo, T. Marrod\\'an Undagoitia, T. Wolf, T. Zhu, U. Oberlack, V. C. Antochi, V. D'Andrea, V. Pizzella, W. Fulgione, Y. Itow, Y. Ma, Y. Mosbacher, Y. Wei, Z. Xu","submitted_at":"2022-05-09T10:14:01Z","abstract_excerpt":"We present results on the search for double-electron capture ($2\\nu\\text{ECEC}$) of $^{124}$Xe and neutrinoless double-$\\beta$ decay ($0\\nu\\beta\\beta$) of $^{136}$Xe in XENON1T. We consider captures from the K- up to the N-shell in the $2\\nu\\text{ECEC}$ signal model and measure a total half-life of $T_{1/2}^{2\\nu\\text{ECEC}}=(1.1\\pm0.2_\\text{stat}\\pm0.1_\\text{sys})\\times 10^{22}\\;\\text{yr}$ with a $0.87\\;\\text{kg}\\times\\text{yr}$ isotope exposure. The statistical significance of the signal is $7.0\\,\\sigma$. We use XENON1T data with $36.16\\;\\text{kg}\\times\\text{yr}$ of $^{136}$Xe exposure to se"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2205.04158","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2022-05-09T10:14:01Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"8e95e67569c2fac20af92ca6320e2cc39519e3be48c6b708c85e4b411629ebff","abstract_canon_sha256":"85e19ff97590dc8667a7f0af5d05554b95fc3fae0bde587db6dc52fb5d0feb5b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:54:58.266875Z","signature_b64":"fOQyfNytuwkybNS2/aliMBbuW2Xp4awHahgaSymmgBXSEzDGXCg77m5PPnjU+WZUyA7tQqbSs9nLKLf8fW84CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"15d313814c4ac3d47908f8423bd531fe5ec406edbfc611d683760a8005b0880f","last_reissued_at":"2026-07-05T04:54:58.266358Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:54:58.266358Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Double-Weak Decays of $^{124}$Xe and $^{136}$Xe in the XENON1T and XENONnT Experiments","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"hep-ex","authors_text":"A. Bismark, A. Brown, A. D. Ferella, A. Di Giovanni, A. Elykov, A. Gallo Rosso, A. Higuera, A. Joy, A. Kopec, A. L. Baxter, A. Mancuso, A. Manfredini, A. Molinario, A. P. Colijn, A. Rocchetti, A. Takeda, A. Terliuk, B. Andrieu, B. Paetsch, C. Cai, C. Capelli, C. Hils, C. Macolino, C. Tunnell, C. Weinheimer, C. Wittweg, D. Ant\\'on Martin, D. Cichon, D. Masson, D. Ram\\'irez Garc\\'ia, D. Schulte, D. Thers, D. Wenz, E. Angelino, E. Aprile, E. Masson, E. Shockley, F. Agostini, F. Arneodo, F. Gao, F. Joerg, F. Lombardi, F. Marignetti, F. Semeria, F. T\\\"onnies, F. Toschi, G. Bruno, G. Koltman, G. Plante, G. Sartorelli, G. Trinchero, G. Volta, G. Zavattini, H. Fischer, H. Landsman, H. Schulze Ei{\\ss}ing, H. Simgen, I. Li, I. Sarnoff, J. A. M. Lopes, J. Conrad, J. Grigat, J. Howlett, J. Jakob, J. J. Cuenca-Garc\\'ia, J. Loizeau, J. Long, J. Mahlstedt, J. Masbou, J. M. F. dos Santos, J. M. R. Cardoso, J. M\\\"uller, J. Palacio, J. P. Cussonneau, J. Pienaar, J. Qi, J. Qin, J. R. Angevaare, J. 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Xu","submitted_at":"2022-05-09T10:14:01Z","abstract_excerpt":"We present results on the search for double-electron capture ($2\\nu\\text{ECEC}$) of $^{124}$Xe and neutrinoless double-$\\beta$ decay ($0\\nu\\beta\\beta$) of $^{136}$Xe in XENON1T. We consider captures from the K- up to the N-shell in the $2\\nu\\text{ECEC}$ signal model and measure a total half-life of $T_{1/2}^{2\\nu\\text{ECEC}}=(1.1\\pm0.2_\\text{stat}\\pm0.1_\\text{sys})\\times 10^{22}\\;\\text{yr}$ with a $0.87\\;\\text{kg}\\times\\text{yr}$ isotope exposure. The statistical significance of the signal is $7.0\\,\\sigma$. 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