{"paper":{"title":"Observation of a low energy nuclear recoil peak in the neutron calibration data of the CRESST-III Experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"A. Bento, A. Bertolini, A. D'Addabbo, A. Erb, A. Fuss, A. Garai, A. Kinast, A. Langenk\\\"amper, A. Nilima, C. Bucci, C. Pagliarone, CRESST Collaboration: G. Angloher, C. Schwertner, C. Strandhagen, D. Fuchs, D. Hauff, D. Schmiedmayer, F. Petricca, F. Pr\\\"obst, F. Pucci, F. Reindl, F. v. Feilitzsch, F. Wagner, G. Benato, H. Kluck, H. Kraus, I. Usherov, J. Burkhart, J. Jochum, J. Rothe, J. Schieck, K. Sch\\\"affner, L. Canonica, L. Einfalt, L. Marini, L. Meyer, L. Pattavina, L. Stodolsky, M. Je\\v{s}kovsk\\'y, M. Kaznacheeva, M. Mancuso, M. Olmi, M. Stahlberg, M. Willers, P. Gorla, P. Povinec, P. V. Guillaumon, R. Breier, R. Strauss, S. Banik, S. Di Lorenzo, S. Fichtinger, S. Gerster, S. Gupta, S. Sch\\\"onert, T. Ortmann, V. M. Ghete, V. Mokina, V. Zema, W. Potzel","submitted_at":"2023-03-27T15:27:06Z","abstract_excerpt":"New-generation direct searches for low mass dark matter feature detection thresholds at energies well below 100 eV, much lower than the energies of commonly used X-ray calibration sources. This requires new calibration sources with sub-keV energies. When searching for nuclear recoil signals, the calibration source should ideally cause mono-energetic nuclear recoils in the relevant energy range. Recently, a new calibration method based on the radiative neutron capture on $^{182}$W with subsequent de-excitation via single $\\gamma$-emission leading to a nuclear recoil peak at 112 eV was proposed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.15315","kind":"arxiv","version":2},"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/2303.15315/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"}