{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,2,21]],"date-time":"2025-02-21T12:31:24Z","timestamp":1740141084294,"version":"3.37.3"},"reference-count":17,"publisher":"IOP Publishing","issue":"1","license":[{"start":{"date-parts":[[2021,12,1]],"date-time":"2021-12-01T00:00:00Z","timestamp":1638316800000},"content-version":"vor","delay-in-days":0,"URL":"http:\/\/creativecommons.org\/licenses\/by\/3.0\/"},{"start":{"date-parts":[[2021,12,1]],"date-time":"2021-12-01T00:00:00Z","timestamp":1638316800000},"content-version":"tdm","delay-in-days":0,"URL":"https:\/\/iopscience.iop.org\/info\/page\/text-and-data-mining"}],"content-domain":{"domain":["iopscience.iop.org"],"crossmark-restriction":false},"short-container-title":["J. Phys.: Conf. Ser."],"published-print":{"date-parts":[[2021,12,1]]},"abstract":"Abstract<\/jats:title>\n Coherent elastic neutrino-nucleus scattering (CE\u03bd<\/jats:italic>NS) offers a unique way to study neutrino properties and to search for new physics beyond the Standard Model. The NUCLEUS experiment aims to measure CE\u03bdNS of reactor anti-neutrinos down to unprecedented low nuclear recoil energies. The novel gram-scale cryogenic detectors feature an ultra-low energy threshold of \u226420eVnr<\/jats:sub> and a rise time of a few 100 \u03bc<\/jats:italic>s which allows the operation above ground. The fiducialization of the detectors provides an effective discrimination of ambient \u03b3<\/jats:italic>- and surface backgrounds. Furthermore, the use of multiple targets promises a high physics potential. The NUCLEUS experiment will be located at a new experimental site at the Chooz nuclear power plant in France, providing a high anti-neutrino flux of \n \n\n<\/jats:tex-math>\n \n \n 1.7<\/mml:mn>\n \u22c5<\/mml:mo>\n \n \n 10<\/mml:mn>\n <\/mml:mrow>\n \n 12<\/mml:mn>\n <\/mml:mrow>\n <\/mml:msup>\n \n \n \u03bd<\/mml:mi>\n \u00af<\/mml:mo>\n <\/mml:mover>\n e<\/mml:mi>\n <\/mml:msub>\n \/<\/mml:mo>\n (<\/mml:mo>\n s<\/mml:mi>\n \u22c5<\/mml:mo>\n \n \n cm<\/mml:mi>\n <\/mml:mrow>\n 2<\/mml:mn>\n <\/mml:msup>\n )<\/mml:mo>\n <\/mml:mrow>\n <\/mml:math>\n \n <\/jats:inline-formula>. The commissioning of the experimental setup with a comprehensive background measurement is planned for 2022.<\/jats:p>","DOI":"10.1088\/1742-6596\/2156\/1\/012118","type":"journal-article","created":{"date-parts":[[2022,2,21]],"date-time":"2022-02-21T04:48:06Z","timestamp":1645418886000},"page":"012118","update-policy":"https:\/\/doi.org\/10.1088\/crossmark-policy","source":"Crossref","is-referenced-by-count":1,"title":["Exploring CE\u03bdNS of reactor neutrinos with the NUCLEUS experiment"],"prefix":"10.1088","volume":"2156","author":[{"given":"V","family":"Wagner","sequence":"first","affiliation":[]},{"given":"G","family":"Angloher","sequence":"additional","affiliation":[]},{"given":"A","family":"Bento","sequence":"additional","affiliation":[]},{"given":"L","family":"Canonica","sequence":"additional","affiliation":[]},{"given":"F","family":"Cappella","sequence":"additional","affiliation":[]},{"given":"L","family":"Cardani","sequence":"additional","affiliation":[]},{"given":"N","family":"Casali","sequence":"additional","affiliation":[]},{"given":"R","family":"Cerulli","sequence":"additional","affiliation":[]},{"given":"I","family":"Colantoni","sequence":"additional","affiliation":[]},{"given":"A","family":"Cruciani","sequence":"additional","affiliation":[]},{"given":"G","family":"del Castello","sequence":"additional","affiliation":[]},{"given":"A","family":"Erhart","sequence":"additional","affiliation":[]},{"given":"M","family":"Friedl","sequence":"additional","affiliation":[]},{"given":"A","family":"Garai","sequence":"additional","affiliation":[]},{"given":"V M","family":"Ghete","sequence":"additional","affiliation":[]},{"given":"C","family":"Goupy","sequence":"additional","affiliation":[]},{"given":"V","family":"Guidi","sequence":"additional","affiliation":[]},{"given":"D","family":"Hauff","sequence":"additional","affiliation":[]},{"given":"M","family":"Kaznacheeva","sequence":"additional","affiliation":[]},{"given":"A","family":"Kinast","sequence":"additional","affiliation":[]},{"given":"L","family":"Klinkenberg","sequence":"additional","affiliation":[]},{"given":"H","family":"Kluck","sequence":"additional","affiliation":[]},{"given":"A","family":"Langenkamper","sequence":"additional","affiliation":[]},{"given":"T","family":"Lasserre","sequence":"additional","affiliation":[]},{"given":"D","family":"Lhuillier","sequence":"additional","affiliation":[]},{"given":"M","family":"Mancuso","sequence":"additional","affiliation":[]},{"given":"B","family":"Mauri","sequence":"additional","affiliation":[]},{"given":"A","family":"Mazzolari","sequence":"additional","affiliation":[]},{"given":"E","family":"Mazzucato","sequence":"additional","affiliation":[]},{"given":"H","family":"Neyrial","sequence":"additional","affiliation":[]},{"given":"C","family":"Nones","sequence":"additional","affiliation":[]},{"given":"L","family":"Oberauer","sequence":"additional","affiliation":[]},{"given":"A","family":"Onillon","sequence":"additional","affiliation":[]},{"given":"T","family":"Ortmann","sequence":"additional","affiliation":[]},{"given":"L","family":"Pattavina","sequence":"additional","affiliation":[]},{"given":"F","family":"Petricca","sequence":"additional","affiliation":[]},{"given":"W","family":"Potzel","sequence":"additional","affiliation":[]},{"given":"F","family":"Pr\u00f6bst","sequence":"additional","affiliation":[]},{"given":"F","family":"Pucci","sequence":"additional","affiliation":[]},{"given":"F","family":"Reindl","sequence":"additional","affiliation":[]},{"given":"R","family":"Rogly","sequence":"additional","affiliation":[]},{"given":"J","family":"Rothe","sequence":"additional","affiliation":[]},{"given":"V","family":"Savu","sequence":"additional","affiliation":[]},{"given":"N","family":"Schermer","sequence":"additional","affiliation":[]},{"given":"J","family":"Schieck","sequence":"additional","affiliation":[]},{"given":"S","family":"Sch\u00f6nert","sequence":"additional","affiliation":[]},{"given":"C","family":"Schwertner","sequence":"additional","affiliation":[]},{"given":"L","family":"Scola","sequence":"additional","affiliation":[]},{"given":"L","family":"Stodolsky","sequence":"additional","affiliation":[]},{"given":"R","family":"Strauss","sequence":"additional","affiliation":[]},{"given":"C","family":"Tomei","sequence":"additional","affiliation":[]},{"given":"K v","family":"Mirbach","sequence":"additional","affiliation":[]},{"given":"M","family":"Vignati","sequence":"additional","affiliation":[]},{"given":"M","family":"Vivier","sequence":"additional","affiliation":[]},{"given":"A","family":"Wex","sequence":"additional","affiliation":[]}],"member":"266","reference":[{"key":"JPCS_2156_1_012118bib1","doi-asserted-by":"crossref","first-page":"1389","DOI":"10.1103\/PhysRevD.9.1389","volume":"9","author":"Freedman","year":"1974","journal-title":"Phys. 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