CUPID (⁸²Se)

(CUORE Upgrade with Particle IDentification)

Other Web pages: INSPIRE

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References

1 - Neutrinoless Double Beta Decay

[1-1]: Final Result on the Neutrinoless Double Beta Decay of $^{82}$Se with CUPID-0, O. Azzolini et al. (CUPID-0), Phys.Rev.Lett. 129 (2022) 111801, arXiv:2206.05130.
[CUPID:2022puj]
[1-2]: Final result of CUPID-0 phase-I in the search for the $^{82}$Se Neutrinoless Double Beta Decay, O. Azzolini et al. (CUPID-0), Phys.Rev.Lett. 123 (2019) 032501, arXiv:1906.05001.
[CUPID:2019gpc]
[1-3]: Search of the neutrino-less double beta decay of $^{82}$Se into the excited states of $^{82}$Kr with CUPID-0, O. Azzolini et al. (CUPID-0), Eur.Phys.J. C78 (2018) 888, arXiv:1807.00665.
[CUPID:2018npf]
[1-4]: First Result on the Neutrinoless Double Beta Decay of $^{82}$Se with CUPID-0, O. Azzolini et al. (CUPID-0), Phys.Rev.Lett. 120 (2018) 232502, arXiv:1802.07791.
[CUPID-0:2018rcs]

2 - Two-Neutrino Double-Beta Decay

[2-1]: Measurement of the $2\nu\beta\beta$ decay rate and spectral shape of $^{100}$Mo from the CUPID-Mo experiment, C. Augier et al., Phys.Rev.Lett. 131 (2023) 162501, arXiv:2307.14086.
[CUPID-Mo:2023lru]
[2-2]: Measurement of the 2$u\beta\beta$ Decay Half-Life of Se-82 with the Global CUPID-0 Background Model, O. Azzolini et al., Phys.Rev.Lett. 131 (2023), arXiv:2306.14654.
[CUPID:2023wyy]
[2-3]: Final Result on the Neutrinoless Double Beta Decay of $^{82}$Se with CUPID-0, O. Azzolini et al. (CUPID-0), Phys.Rev.Lett. 129 (2022) 111801, arXiv:2206.05130.
[CUPID:2022puj]
[2-4]: Final result of CUPID-0 phase-I in the search for the $^{82}$Se Neutrinoless Double Beta Decay, O. Azzolini et al. (CUPID-0), Phys.Rev.Lett. 123 (2019) 032501, arXiv:1906.05001.
[CUPID:2019gpc]
[2-5]: Search of the neutrino-less double beta decay of $^{82}$Se into the excited states of $^{82}$Kr with CUPID-0, O. Azzolini et al. (CUPID-0), Eur.Phys.J. C78 (2018) 888, arXiv:1807.00665.
[CUPID:2018npf]
[2-6]: First Result on the Neutrinoless Double Beta Decay of $^{82}$Se with CUPID-0, O. Azzolini et al. (CUPID-0), Phys.Rev.Lett. 120 (2018) 232502, arXiv:1802.07791.
[CUPID-0:2018rcs]

3 - Detector

[3-1]: The background model of the CUPID-Mo $0\nu\beta\beta$ experiment, C. Augier et al. (CUPID-Mo), Eur.Phys.J.C 83 (2023) 675, arXiv:2305.01402.
[CUPID-Mo:2023vle]
[3-2]: A first test of CUPID prototypal light detectors with NTD-Ge sensors in a pulse-tube cryostat, K. Alfonso et al. (CUPID), JINST 18 (2023) P06033, arXiv:2304.04674.
[CUPID:2023hxo]
[3-3]: Large area photon calorimeter with Ir-Pt bilayer transition-edge sensor for the CUPID experiment, V. Singh et al., Phys.Rev.Applied 20 (2023) 064017, arXiv:2210.15619.
[Singh:2022rck]
[3-4]: Optimization of the first CUPID detector module, A. Armatol et al. (CUPID), Eur.Phys.J.C 82 (2022) 810, arXiv:2202.06279.
[CUPID:2022opf]
[3-5]: A CUPID Li$_{2}$$^{100}$MoO$_4$ scintillating bolometer tested in the CROSS underground facility, CUPID Interest Group, JINST 16 (2021) P02037, arXiv:2011.13806.
[CUPID:2020pra]
[3-6]: Characterization of cubic Li$_{2}$$^{100}$MoO$_4$ crystals for the CUPID experiment, A. Armatol et al., Eur.Phys.J. C81 (2021) 104, arXiv:2011.13656.
[CUPID:2020itw]
[3-7]: A novel technique for the study of pile-up events in cryogenic bolometers, CUPID Interest Group, Phys.Rev.C 104 (2021) 015501, arXiv:2011.11726.
[CUPID:2020cpe]
[3-8]: Pulse Shape Discrimination in CUPID-Mo using Principal Component Analysis, R. Huang et al., JINST 16 (2021) P03032, arXiv:2010.04033.
[CUPID:2020smz]
[3-9]: The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects, E. Armengaud et al., Eur.Phys.J. C80 (2020) 44, arXiv:1909.02994.
[Armengaud:2019loe]
[3-10]: Characterization of Light Production and Transport in Tellurium Dioxide Crystals, R. G. Huang, G. Benato, J. Caravaca, Yu. G. Kolomensky, B. J. Land, G. D. Orebi Gann, B. Schmidt, JINST 14 (2019) P10032, arXiv:1907.10856.
[Huang:2019pov]
[3-11]: CUPID pre-CDR, CUPID Interest Group, arXiv:1907.09376, 2019.
[CUPID:2019imh]
[3-12]: Phonon and light read out of a Li$_2$MoO$_4$ crystal with multiplexed kinetic inductance detectors, N. Casali, L. Cardani, I. Colantoni, A. Cruciani, S. Di Domizio, G. Pettinari, M. Martinez, M. Vignati, Eur.Phys.J. C79 (2019) 724, arXiv:1907.03647.
[Casali:2019baq]
[3-13]: Resolution enhancement with light/heat decorrelation in CUPID-0 bolometric detector, M. Beretta et al., JINST 14 (2019) P08017, arXiv:1901.10434.
[Beretta:2019bmm]
[3-14]: CUPID-0: the first array of enriched scintillating bolometers for 0\nu\beta\betadecay investigations, O. Azzolini et al., Eur.Phys.J. C78 (2018) 428, arXiv:1802.06562.
[CUPID:2018kff]
[3-15]: Enriched TeO$_2$ bolometers with active particle discrimination: towards the CUPID experiment, D.R. Artusa et al., Phys.Lett. B767 (2017) 321-329, arXiv:1610.03513.
[Artusa:2016mat]
[3-16]: R&D towards CUPID (CUORE Upgrade with Particle IDentification), G. Wang et al. (CUPID), arXiv:1504.03612, 2015.
[CUPID:2015tlr]
[3-17]: CUPID: CUORE (Cryogenic Underground Observatory for Rare Events) Upgrade with Particle IDentification, G. Wang et al. (CUPID), arXiv:1504.03599, 2015.
[CUPID:2015yfg]

4 - Talks

[4-1]: Final results from the CUPID-Mo $0\nu\beta\beta$ experiment, Toby Dixon, arXiv:2305.09003, 2023.
[Dixon:2023dkw]
[4-2]: First data from the CUPID-Mo neutrinoless double beta decay experiment, B. Schmidt et al., J.Phys.Conf.Ser. 1468 (2020) 012129, arXiv:1911.10426. TAUP 2019.
[CUPID:2019vfp]
[4-3]: $^{100}$Mo-enriched Li$_2$MoO$_4$ scintillating bolometers for $0\nu 2\beta$ decay search: from LUMINEU to CUPID-0/Mo projects, D.V. Poda, AIP Conf.Proc. 1894 (2017) 020017, arXiv:1709.07846. MEDEX'17 meeting (Prague, May 29 - June 2, 2017).
[Poda:2017bmd]

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