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dc.contributor.authorAugier, C.
dc.contributor.authorBarabash, A. S.
dc.contributor.authorBellini, F.
dc.contributor.authorBenato, G.
dc.contributor.authorBeretta, M.
dc.contributor.authorBergé, L.
dc.contributor.authorBillard, J.
dc.contributor.authorBorovlev, Yu. A.
dc.contributor.authorCardani, L.
dc.contributor.authorCasali, N.
dc.contributor.authorCazes, A.
dc.contributor.authorCeli, E.
dc.contributor.authorChapellier, M.
dc.contributor.authorChiesa, D.
dc.contributor.authorDafinei, I.
dc.contributor.authorDanevich, F. A.
dc.contributor.authorDe Jesus, M.
dc.contributor.authorde Marcillac, P.
dc.contributor.authorDixon, T.
dc.contributor.authorDumoulin, L.
dc.date.accessioned2023-09-20T18:55:28Z
dc.date.available2023-09-20T18:55:28Z
dc.date.issued2023-07-28
dc.identifier.urihttps://hdl.handle.net/1721.1/152185
dc.description.abstractAbstract CUPID-Mo, located in the Laboratoire Souterrain de Modane (France), was a demonstrator for the next generation $$0\nu \beta \beta $$ 0 ν β β decay experiment, CUPID. It consisted of an array of 20 enriched Li $$_{2}$$ 2 $$^{100}$$ 100 MoO $$_4$$ 4 bolometers and 20 Ge light detectors and has demonstrated that the technology of scintillating bolometers with particle identification capabilities is mature. Furthermore, CUPID-Mo can inform and validate the background prediction for CUPID. In this paper, we present a detailed model of the CUPID-Mo backgrounds. This model is able to describe well the features of the experimental data and enables studies of the $$2\nu \beta \beta $$ 2 ν β β decay and other processes with high precision. We also measure the radio-purity of the Li $$_{2}$$ 2 $$^{100}$$ 100 MoO $$_4$$ 4 crystals which are found to be sufficient for the CUPID goals. Finally, we also obtain a background index in the region of interest of 3.7  $$^{+0.9}_{-0.8}$$ - 0.8 + 0.9  (stat) $$^{+1.5}_{-0.7}$$ - 0.7 + 1.5  (syst)  $$\times ~10 ^{-3}$$ × 10 - 3  counts/ $$\Delta E_{\text {FWHM}}/\text {mol}_{\text {iso}}/\text {year},$$ Δ E FWHM / mol iso / year , the lowest in a bolometric $$0\nu \beta \beta $$ 0 ν β β decay experiment.en_US
dc.publisherSpringer Berlin Heidelbergen_US
dc.relation.isversionofhttps://doi.org/10.1140/epjc/s10052-023-11830-2en_US
dc.rightsCreative Commons Attributionen_US
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.titleThe background model of the CUPID-Mo 0νββ experimenten_US
dc.typeArticleen_US
dc.identifier.citationThe European Physical Journal C. 2023 Jul 28;83(7):675en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
dc.relation.journalThe European Physical Journal Cen_US
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.updated2023-09-10T03:10:56Z
dc.language.rfc3066en
dc.rights.holderThe Author(s)
dspace.embargo.termsN
dspace.date.submission2023-09-10T03:10:56Z
mit.licensePUBLISHER_CC
mit.metadata.statusAuthority Work and Publication Information Neededen_US


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