{"paper":{"title":"Calorimeter development for the SuperNEMO double beta decay experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"A. Basharina-Freshville, A. Chopra, A. Huber, A.J. Caffrey, A. Jeremie, A. Klimenko, A. Rebii, A. Remoto, A.S. Barabash, A. Smetana, A. Smolnikov, A. \\v{Z}ukauskas, B. Guillon, B. Morgan, B. Richards, B. Soul\\'e, C. Cerna, Ch. Bourgeois, C. Hugon, C.L. Riddle, C. Marquet, C. Vilela, D. Breton, D. Duchesneau, D. Filosofov, D. Waters, E. Chauveau, E. Rukhadze, F. Delalee, F. Mamedov, F. Mauger, F. Nova, F. Perrot, F. Piquemal, F. \\v{S}imkovic, G. Claverie, G. Eurin, G. Lutter, H. Bure\\v{s}ov\\`a, H. G\\'omez, H. Ohsumi, I. Moreau, I. Nemchenok, I. \\v{S}tekl, J. Busto, J.J. Evans, J. Maalmi, J. Mott, J.P. Cesar, J.R. Pater, J. Sedgbeer, J.S. Ricol, J. Thomas, K. Hol\\'y, K. Lang, K. Smolek, L. Fajt, L. Simard, M. Bongrand, M. Cascella, M. Kauer, M. Macko, M. Nomachi, M. \\v{S}pavorov\\'a, O. Kochetov, P. Guzowski, P. Loaiza, P. Povinec, P. P\\v{r}idal, R.B. Pahlka, R. Flack, R. Hod\\'ak, R. Saakyan, R. Salazar, S. Blot, S. Calvez, S. De Capua, S.I. Konovalov, S. Jullian, S. Snow, S. S\\\"oldner-Rembold, S. Torre, T. Le Noblet, V. Brudanin, V. Egorov, V.I. Tretyak, V.I. Umatov, V. Kovalenko, Vl.I. Tretyak, V. Timkin, V. Vorobel, X. Garrido, X.R. Liu, X. Sarazin, Y.A. Ramachers, Y. Lemi\\`ere, Yu. Shitov, Z. Liptak","submitted_at":"2017-07-21T10:09:05Z","abstract_excerpt":"SuperNEMO is a double-$\\beta$ decay experiment, which will employ the successful tracker-calorimeter technique used in the recently completed NEMO-3 experiment. SuperNEMO will implement 100 kg of double-$\\beta$ decay isotope, reaching a sensitivity to the neutrinoless double-$\\beta$ decay ($0\\nu\\beta\\beta$) half-life of the order of $10^{26}$ yr, corresponding to a Majorana neutrino mass of 50-100 meV. One of the main goals and challenges of the SuperNEMO detector development programme has been to reach a calorimeter energy resolution, $\\Delta$E/E, around 3%/$sqrt(E)$(MeV) $\\sigma$, or 7%/$sqr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1707.06823","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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"}