{"paper":{"title":"Improved limit on neutrinoless double beta decay of $^{100}$Mo from AMoRE-I","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"nucl-ex","authors_text":"A. Agrawal, A. Fleischmann, A. Khan, A.M. Gangapshev, A.M. Gezhaev, B. Bhandari, B. Mailyan, B. Sharma, C. Enss, C. Ha, C.H. Lee, C.R. Byeon, C.S. Kang, D. Drung, D.H. Ha, D.H. Hwang, D.H. Kwon, DongYeup Lee, D.S. Leonard, D.Y. Kim, E.J. Ha, E.J. Jeon, E.K. Lee, E.P. Makarov, F.A. Danevich, G. Rooh, G.W. Kim, H.B. Kim, H.J. Kim, H.J. Lee, H.J. Yeon, H.K. Park, H.L. Kim, Ho-Jong Kim, H. Prihtiadi, H.S. Jo, H.S. Kim, H.S. Lee, H.S. Lim, H.S. Park, J.A. Jeon, J. Beyer, J. Kaewkhao, J.K. Son, J. Lee, J.S. Choe, J.S. Chung, J. Seo, J. So, J.W. Song, J.Y. Lee, K.A. Shin, K.B. Lee, K. Boonin, K. Kirdsiri, K.M. Seo, K.R. Woo, K. Siyeon, K.S. Park, L. Gastaldo, M.B. Kim, M.B. Sari, M. Djamal, M.H. Lee, M.K. Cheoun, M.K. Lee, N. Chanthima, N. Srisittipokakun, N.V. Sokur, O. Buzanov, O. Gileva, O.G. Polischuk, P. Aryal, P. Nyanda, Q. Yue, R.S. Boiko, R. Wirawan, S. Choudhury, S.C. Kim, Seonho Choi, S.I. Panasenko, S. Kempf, S. Khan, S.K. Kim, S.L. Olsen, S. Ra, S.R. Kim, S.S. Ratkevich, S.W. Lee, S.Y. Park, V.D. Grigorieva, V.I. Gurentsov, V.I. Tretyak, V. Kornoukhov, V.N. Shlegel, V.V. Alenkov, V. V. Kazalov, V.V. Kobychev, V.V. Kuzminov, W.G. Kang, W.T. Kim, Y.C. Lee, Y.D. Kim, Y.H. Kim, Y.J. Ko, Y.M. Gavrilyuk, Y. Oh, Y.S. Yoon","submitted_at":"2024-07-08T05:15:17Z","abstract_excerpt":"AMoRE searches for the signature of neutrinoless double beta decay of $^{100}$Mo with a 100 kg sample of enriched $^{100}$Mo. Scintillating molybdate crystals coupled with a metallic magnetic calorimeter operate at milli-Kelvin temperatures to measure the energy of electrons emitted in the decay. As a demonstration of the full-scale AMoRE, we conducted AMoRE-I, a pre-experiment with 18 molybdate crystals, at the Yangyang Underground Laboratory for over two years. The exposure was 8.02 kg$\\cdot$year (or 3.89 kg$_{\\mathrm{^{100}Mo}}\\cdot$year) and the total background rate near the Q-value was 0"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2407.05618","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2407.05618/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}