- Armatol, A;
- Armengaud, E;
- Armstrong, W;
- Augier, C;
- Avignone, FT;
- Azzolini, O;
- Bandac, IC;
- Barabash, AS;
- Bari, G;
- Barresi, A;
- Baudin, D;
- Bellini, F;
- Benato, G;
- Beretta, M;
- Bergé, L;
- Bourgeois, Ch;
- Biassoni, M;
- Billard, J;
- Boldrini, V;
- Branca, A;
- Brofferio, C;
- Bucci, C;
- Calvo-Mozota, JM;
- Camilleri, J;
- Candela, A;
- Capelli, S;
- Cappelli, L;
- Cardani, L;
- Carniti, P;
- Casali, N;
- Cazes, A;
- Celi, E;
- Chang, C;
- Chapellier, M;
- Charrier, A;
- Chiesa, D;
- Clemenza, M;
- Colantoni, I;
- Collamati, F;
- Copello, S;
- Cremonesi, O;
- Creswick, RJ;
- Cruciani, A;
- D'Addabbo, A;
- D'Imperio, G;
- Dafinei, I;
- Danevich, FA;
- de Combarieu, M;
- De Deo, M;
- De Jesus, M;
- de Marcillac, P;
- Dell'Oro, S;
- Di Domizio, S;
- Dompe, V;
- Drobizhev, A;
- Dumoulin, L;
- Fantini, G;
- Faverzani, M;
- Ferri, E;
- Ferri, F;
- Ferroni, F;
- Figueroa-Feliciano, E;
- Formaggio, J;
- Franceschi, A;
- Fu, C;
- Fu, S;
- Fujikawa, BK;
- Gascon, J;
- Giachero, A;
- Gironi, L;
- Giuliani, A;
- Gorla, P;
- Gotti, C;
- Gras, P;
- Gros, M;
- Guerard, E;
- Gutierrez, TD;
- Han, K;
- Hansen, EV;
- Heeger, KM;
- Helis, DL;
- Huang, HZ;
- Huang, RG;
- Ianni, A;
- Imbert, L;
- Johnston, J;
- Juillard, A;
- Karapetrov, G;
- Keppel, G;
- Khalife, H;
- Kobychev, VV;
- Kolomensky, Yu G;
- Konovalov, SI;
- Liu, Y;
- Loaiza, P;
- Ma, L;
- Madhukuttan, M;
- Mancarella, F;
- Mariam, R;
- Marini, L;
- Marnieros, S;
- Martinez, M;
- Maruyama, RH;
- Mauri, B;
- Mayer, D;
- Mei, Y;
- Milana, S;
- Misiak, D;
- Napolitano, T;
- Nastasi, M;
- Navick, X-F;
- Nikkel, J;
- Nipoti, R;
- Nisi, S;
- Nones, C;
- Norman, EB;
- Novosad, V;
- Nutini, I;
- O'Donnell, T;
- Olivier, G;
- Olivieri, E;
- Oriol, C;
- Ouellet, JL;
- Pagan, S;
- Pagliarone, C;
- Pagnanini, L;
- Pari, P;
- Pattavina, L;
- Paul, B;
- Pavan, M;
- Peng, H;
- Pessina, G;
- Pettinacci, V;
- Pira, C;
- Pirro, S;
- Poda, DV;
- Polakovic, T;
- Polischuk, OG;
- Pozzi, S;
- Previtali, E;
- Puiu, A;
- Ressa, A;
- Reynet, D;
- Rizzoli, R;
- Rosenfeld, C;
- Sanglard, V;
- Scarpaci, JA;
- Schmidt, B;
- Sharma, V;
- Shlegel, VN;
- Singh, V;
- Sisti, M;
- Speller, D;
- Surukuchi, PT;
- Taffarello, L;
- Tellier, O;
- Tomei, C;
- Tretyak, VI;
- Tsymbaliuk, A;
- Velazquez, M;
- Vetter, KJ;
- Wagaarachchi, SL;
- Wang, G;
- Wang, L;
- Welliver, B;
- Wilson, J;
- Wilson, K;
- Winslow, LA;
- Xue, M;
- Yan, L;
- Yang, J;
- Yefremenko, V;
- Yumatov, VI;
- Zarytskyy, MM;
- Zhang, J;
- Zolotarova, AS;
- Zucchelli, S
A scintillating bolometer based on a large cubic Li$_{2}$$^{100}$MoO$_4$
crystal (45 mm side) and a Ge wafer (scintillation detector) has been operated
in the CROSS cryogenic facility at the Canfranc underground laboratory in
Spain. The dual-readout detector is a prototype of the technology that will be
used in the next-generation $0
u2\beta$ experiment CUPID. The measurements
were performed at 18 and 12 mK temperature in a pulse tube dilution
refrigerator. This setup utilizes the same technology as the CUORE cryostat
that will host CUPID and so represents an accurate estimation of the expected
performance. The Li$_{2}$$^{100}$MoO$_4$ bolometer shows a high energy
resolution of 6 keV FWHM at the 2615 keV $\gamma$ line. The detection of
scintillation light for each event triggered by the Li$_{2}$$^{100}$MoO$_4$
bolometer allowed for a full separation ($\sim$8$\sigma$) between
$\gamma$($\beta$) and $\alpha$ events above 2 MeV. The Li$_{2}$$^{100}$MoO$_4$
crystal also shows a high internal radiopurity with $^{228}$Th and $^{226}$Ra
activities of less than 3 and 8 $\mu$Bq/kg, respectively. Taking also into
account the advantage of a more compact and massive detector array, which can
be made of cubic-shaped crystals (compared to the cylindrical ones), this test
demonstrates the great potential of cubic Li$_{2}$$^{100}$MoO$_4$ scintillating
bolometers for high-sensitivity searches for the $^{100}$Mo $0
u2\beta$ decay
in CROSS and CUPID projects.