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dc.contributor.authorAlfonso, K.
dc.contributor.authorArmatol, A.
dc.contributor.authorAugier, C.
dc.contributor.authorAvignone, F. T.
dc.contributor.authorAzzolini, O.
dc.contributor.authorBalata, M.
dc.contributor.authorBarabash, A. S.
dc.contributor.authorBari, G.
dc.contributor.authorBarresi, A.
dc.contributor.authorBaudin, D.
dc.contributor.authorBellini, F.
dc.contributor.authorBenato, G.
dc.contributor.authorBeretta, M.
dc.contributor.authorBettelli, M.
dc.contributor.authorBiassoni, M.
dc.contributor.authorBillard, J.
dc.contributor.authorBoldrini, V.
dc.contributor.authorBranca, A.
dc.contributor.authorBrofferio, C.
dc.contributor.authorBucci, C.
dc.date.accessioned2022-09-19T13:56:50Z
dc.date.available2022-09-19T13:56:50Z
dc.date.issued2022-09-12
dc.identifier.urihttps://hdl.handle.net/1721.1/145482
dc.description.abstractAbstract CUPID will be a next generation experiment searching for the neutrinoless double $$\beta $$ β decay, whose discovery would establish the Majorana nature of the neutrino. Based on the experience achieved with the CUORE experiment, presently taking data at LNGS, CUPID aims to reach a background free environment by means of scintillating Li $$_{2}$$ 2 $$^{100}$$ 100 MoO $$_4$$ 4 crystals coupled to light detectors. Indeed, the simultaneous heat and light detection allows us to reject the dominant background of $$\alpha $$ α particles, as proven by the CUPID-0 and CUPID-Mo demonstrators. In this work we present the results of the first test of the CUPID baseline module. In particular, we propose a new optimized detector structure and light sensors design to enhance the engineering and the light collection, respectively. We characterized the heat detectors, achieving an energy resolution of (5.9 ± 0.2) keV FWHM at the Q-value of $$^{100}$$ 100 Mo (about 3034 keV). We studied the light collection of the baseline CUPID design with respect to an alternative configuration which features gravity-assisted light detectors’ mounting. In both cases we obtained an improvement in the light collection with respect to past measures and we validated the particle identification capability of the detector, which ensures an $$\alpha $$ α particle rejection higher than 99.9%, fully satisfying the requirements for CUPID.en_US
dc.publisherSpringer Berlin Heidelbergen_US
dc.relation.isversionofhttps://doi.org/10.1140/epjc/s10052-022-10720-3en_US
dc.rightsCreative Commons Attributionen_US
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.titleOptimization of the first CUPID detector moduleen_US
dc.typeArticleen_US
dc.identifier.citationThe European Physical Journal C. 2022 Sep 12;82(9):810en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
dc.identifier.mitlicensePUBLISHER_CC
dc.eprint.versionFinal published versionen_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2022-09-18T03:13:06Z
dc.language.rfc3066en
dc.rights.holderThe Author(s)
dspace.embargo.termsN
dspace.date.submission2022-09-18T03:13:06Z
mit.licensePUBLISHER_CC
mit.metadata.statusAuthority Work and Publication Information Neededen_US


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