<?xml version="1.0" encoding="UTF-8"?><rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcq="http://purl.org/dc/terms/"><records count="1" morepages="false" start="1" end="1"><record rownumber="1"><dc:product_type>Journal Article</dc:product_type><dc:title>A first test of CUPID prototypal light detectors with NTD-Ge sensors in a pulse-tube cryostat</dc:title><dc:creator>Alfonso, K.; Armatol, A.; Augier, C.; Avignone, F.T.; Azzolini, O.; Balata, M.; Barabash, A.S.; Bari, G.; Barresi, A.; Baudin, D.; Bellini, F.; Benato, G.; Berest, V.; Beretta, M.; Bettelli, M.; Biassoni, M.; Billard, J.; Boldrini, V.; Branca, A.; Brofferio, C.; Bucci, C.; Camilleri, J.; Campani, A.; Capelli, C.; Capelli, S.; Cappelli, L.; Cardani, L.; Carniti, P.; Casali, N.; Celi, E.; Chang, C.; Chiesa, D.; Clemenza, M.; Colantoni, I.; Copello, S.; Craft, E.; Cremonesi, O.; Creswick, R.J.; Cruciani, A.; D'Addabbo, A.; D'Imperio, G.; Dabagov, S.; Dafinei, I.; Danevich, F.A.; De Jesus, M.; de Marcillac, P.; Dell'Oro, S.; Di Domizio, S.; Di Lorenzo, S.; Dixon, T.; Dompé, V.; Drobizhev, A.; Dumoulin, L.; Fantini, G.; Faverzani, M.; Ferri, E.; Ferri, F.; Ferroni, F.; Figueroa-Feliciano, E.; Foggetta, L.; Formaggio, J.; Franceschi, A.; Fu, C.; Fu, S.; Fujikawa, B.K.; Gallas, A.; Gascon, J.; Ghislandi, S.; Giachero, A.; Gianvecchio, A.; Girola, M.; Gironi, L.; Giuliani, A.; Gorla, P.; Gotti, C.; Grant, C.; Gras, P.; Guillaumon, P.V.; Gutierrez, T.D.; Han, K.; Hansen, E.V.; Heeger, K.M.; Helis, D.L.; Huang, H.Z.; Imbert, L.; Johnston, J.; Juillard, A.; Karapetrov, G.; Keppel, G.; Khalife, H.; Kobychev, V.V.; Kolomensky, Yu.G.; Konovalov, S.I.; Kowalski, R.; Langford, T.; Lefevre, M.; Liu, R.; Liu, Y.; Loaiza, P.; Ma, L.; Madhukuttan, M.; Mancarella, F.; Marini, L.; Marnieros, S.; Martinez, M.; Maruyama, R.H.; Mas, Ph.; Mayer, D.; Mazzitelli, G.; Mei, Y.; Milana, S.; Morganti, S.; Napolitano, T.; Nastasi, M.; Nikkel, J.; Nisi, S.; Nones, C.; Norman, E.B.; Novosad, V.; Nutini, I.; O'Donnell, T.; Olivieri, E.; Olmi, M.; Ouellet, J.L.; Pagan, S.; Pagliarone, C.; Pagnanini, L.; Pattavina, L.; Pavan, M.; Peng, H.; Pessina, G.; Pettinacci, V.; Pira, C.; Pirro, S.; Poda, D.V.; Polischuk, O.G.; Ponce, I.; Pozzi, S.; Previtali, E.; Puiu, A.; Quitadamo, S.; Ressa, A.; Rizzoli, R.; Rosenfeld, C.; Rosier, P.; Scarpaci, J.A.; Schmidt, B.; Sharma, V.; Shlegel, V.N.; Singh, V.; Sisti, M.; Slocum, P.; Speller, D.; Surukuchi, P.T.; Taffarello, L.; Tomei, C.; Torres, J.A.; Tretyak, V.I.; Tsymbaliuk, A.; Velazquez, M.; Vetter, K.J.; Wagaarachchi, S.L.; Wang, G.; Wang, L.; Wang, R.; Welliver, B.; Wilson, J.; Wilson, K.; Winslow, L.A.; Xue, M.; Yan, L.; Yang, J.; Yefremenko, V.; Umatov, V.I.; Zarytskyy, M.M.; Zhang, J.; Zolotarova, A.; Zucchelli, S.</dc:creator><dc:corporate_author/><dc:editor/><dc:description>Abstract                          CUPID is a next-generation bolometric experiment aiming at  searching for neutrinoless double-beta decay with ∼250 kg of  isotopic mass of              100              Mo. It will operate at ∼10 mK in a  cryostat currently hosting a similar-scale bolometric array for the  CUORE experiment at the Gran Sasso National Laboratory  (Italy). CUPID will be based on large-volume scintillating  bolometers consisting of              100              Mo-enriched Li              2              MoO              4              crystals,  facing thin Ge-wafer-based bolometric light detectors. In the CUPID  design, the detector structure is novel and needs to be  validated. In particular, the CUORE cryostat presents a high level  of mechanical vibrations due to the use of pulse tubes and the  effect of vibrations on the detector performance must be  investigated. In this paper we report the first test of the  CUPID-design bolometric light detectors with NTD-Ge sensors in a  dilution refrigerator equipped with a pulse tube in an above-ground  lab. Light detectors are characterized in terms of sensitivity,  energy resolution, pulse time constants, and noise power  spectrum. Despite the challenging noisy environment due to  pulse-tube-induced vibrations, we demonstrate that all the four  tested light detectors comply with the CUPID goal in terms of  intrinsic energy resolution of 100 eV RMS baseline noise. Indeed,  we have measured 70–90 eV RMS for the four devices, which show an  excellent reproducibility.  We have also obtained high energy  resolutions at the 356 keV line from a              133              Ba source, as good  as Ge semiconductor              γ              detectors in this energy range.</dc:description><dc:publisher/><dc:date>2023-06-01</dc:date><dc:nsf_par_id>10451316</dc:nsf_par_id><dc:journal_name>Journal of Instrumentation</dc:journal_name><dc:journal_volume>18</dc:journal_volume><dc:journal_issue>06</dc:journal_issue><dc:page_range_or_elocation>P06033</dc:page_range_or_elocation><dc:issn>1748-0221</dc:issn><dc:isbn/><dc:doi>https://doi.org/10.1088/1748-0221/18/06/P06033</dc:doi><dcq:identifierAwardId>1913374</dcq:identifierAwardId><dc:subject/><dc:version_number/><dc:location/><dc:rights/><dc:institution/><dc:sponsoring_org>National Science Foundation</dc:sponsoring_org></record></records></rdf:RDF>