Abstract
Precise characterization of detector time resolution is of crucial importance for next-generation cryogenic-bolometer experiments searching for neutrinoless double-beta decay, such as CUPID, in order to reject background due to pileup of two-neutrino double-beta decay events. In this paper, we describe a technique developed to study the pileup rejection capability of cryogenic bolometers. Our approach, which consists of producing controlled pileup events with a programmable wave-form generator, has the benefit that we can reliably and reproducibly control the time separation and relative energy of the individual components of the generated pileup events. The resulting data allow us to optimize and benchmark analysis strategies to discriminate between individual and pileup pulses. We describe a test of this technique performed with a small array of detectors at the Laboratori Nazionali del Gran Sasso, in Italy; we obtain a 90% rejection efficiency against pulser-generated pileup events with rise time of ∼15ms down to time separation between the individual events of about 2ms.
| Original language | English (US) |
|---|---|
| Article number | 015501 |
| Journal | Physical Review C |
| Volume | 104 |
| Issue number | 1 |
| DOIs | |
| State | Published - Jun 2021 |
ASJC Scopus subject areas
- Nuclear and High Energy Physics
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Novel technique for the study of pileup events in cryogenic bolometers. / Armatol, A.; Armengaud, E.; Armstrong, W.; Augier, C.; Avignone, F. T.; Azzolini, O.; Barabash, A.; Bari, G.; Barresi, A.; Baudin, D.; Bellini, F.; Benato, G.; Beretta, M.; Bergé, L.; Biassoni, M.; Billard, J.; Boldrini, V.; Branca, A.; Brofferio, C.; Bucci, C.; Camilleri, J.; 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, R. J.; Cruciani, A.; D'Addabbo, A.; D'Imperio, G.; Dafinei, I.; Danevich, F. A.; De Combarieu, M.; De Jesus, M.; De Marcillac, P.; Dell'Oro, S.; Di Domizio, S.; Dompè, 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, B. K.; Gascon, J.; Giachero, A.; Gironi, L.; Giuliani, A.; Gorla, P.; Gotti, C.; Gras, P.; Gros, M.; Gutierrez, T. D.; Han, K.; Hansen, E. V.; Heeger, K. M.; Helis, D. L.; Huang, H. Z.; Huang, R. G.; Imbert, L.; Johnston, J.; Juillard, A.; Karapetrov, G.; Keppel, G.; Khalife, H.; Kobychev, V. V.; Kolomensky, Yu G.; Konovalov, S.; Liu, Y.; Loaiza, P.; Ma, L.; Madhukuttan, M.; Mancarella, F.; Mariam, R.; Marini, L.; Marnieros, S.; Martinez, M.; Maruyama, R. H.; 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, E. B.; Novosad, V.; Nutini, I.; O'Donnell, T.; Olivieri, E.; Oriol, C.; Ouellet, J. L.; 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, D. V.; Polakovic, T.; Polischuk, O. G.; Pozzi, S.; Previtali, E.; Puiu, A.; Ressa, A.; Rizzoli, R.; Rosenfeld, C.; Rusconi, C.; Sanglard, V.; Scarpaci, J.; Schmidt, B.; Sharma, V.; Shlegel, V.; Singh, V.; Sisti, M.; Speller, D.; Surukuchi, P. T.; Taffarello, L.; Tellier, O.; Tomei, C.; Tretyak, V. I.; Tsymbaliuk, A.; Velazquez, M.; Vetter, K. J.; Wagaarachchi, S. L.; Wang, G.; Wang, L.; Welliver, B.; Wilson, J.; Wilson, K.; Winslow, L. A.; Xue, M.; Yan, L.; Yang, J.; Yefremenko, V.; Yumatov, V.; Zarytskyy, M. M.; Zhang, J.; Zolotarova, A.; Zucchelli, S.
In: Physical Review C, Vol. 104, No. 1, 015501, 06.2021.Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Novel technique for the study of pileup events in cryogenic bolometers
AU - Armatol, A.
AU - Armengaud, E.
AU - Armstrong, W.
AU - Augier, C.
AU - Avignone, F. T.
AU - Azzolini, O.
AU - Barabash, A.
AU - Bari, G.
AU - Barresi, A.
AU - Baudin, D.
AU - Bellini, F.
AU - Benato, G.
AU - Beretta, M.
AU - Bergé, L.
AU - Biassoni, M.
AU - Billard, J.
AU - Boldrini, V.
AU - Branca, A.
AU - Brofferio, C.
AU - Bucci, C.
AU - Camilleri, J.
AU - Capelli, S.
AU - Cappelli, L.
AU - Cardani, L.
AU - Carniti, P.
AU - Casali, N.
AU - Cazes, A.
AU - Celi, E.
AU - Chang, C.
AU - Chapellier, M.
AU - Charrier, A.
AU - Chiesa, D.
AU - Clemenza, M.
AU - Colantoni, I.
AU - Collamati, F.
AU - Copello, S.
AU - Cremonesi, O.
AU - Creswick, R. J.
AU - Cruciani, A.
AU - D'Addabbo, A.
AU - D'Imperio, G.
AU - Dafinei, I.
AU - Danevich, F. A.
AU - De Combarieu, M.
AU - De Jesus, M.
AU - De Marcillac, P.
AU - Dell'Oro, S.
AU - Di Domizio, S.
AU - Dompè, V.
AU - Drobizhev, A.
AU - Dumoulin, L.
AU - Fantini, G.
AU - Faverzani, M.
AU - Ferri, E.
AU - Ferri, F.
AU - Ferroni, F.
AU - Figueroa-Feliciano, E.
AU - Formaggio, J.
AU - Franceschi, A.
AU - Fu, C.
AU - Fu, S.
AU - Fujikawa, B. K.
AU - Gascon, J.
AU - Giachero, A.
AU - Gironi, L.
AU - Giuliani, A.
AU - Gorla, P.
AU - Gotti, C.
AU - Gras, P.
AU - Gros, M.
AU - Gutierrez, T. D.
AU - Han, K.
AU - Hansen, E. V.
AU - Heeger, K. M.
AU - Helis, D. L.
AU - Huang, H. Z.
AU - Huang, R. G.
AU - Imbert, L.
AU - Johnston, J.
AU - Juillard, A.
AU - Karapetrov, G.
AU - Keppel, G.
AU - Khalife, H.
AU - Kobychev, V. V.
AU - Kolomensky, Yu G.
AU - Konovalov, S.
AU - Liu, Y.
AU - Loaiza, P.
AU - Ma, L.
AU - Madhukuttan, M.
AU - Mancarella, F.
AU - Mariam, R.
AU - Marini, L.
AU - Marnieros, S.
AU - Martinez, M.
AU - Maruyama, R. H.
AU - Mauri, B.
AU - Mayer, D.
AU - Mei, Y.
AU - Milana, S.
AU - Misiak, D.
AU - Napolitano, T.
AU - Nastasi, M.
AU - Navick, X. F.
AU - Nikkel, J.
AU - Nipoti, R.
AU - Nisi, S.
AU - Nones, C.
AU - Norman, E. B.
AU - Novosad, V.
AU - Nutini, I.
AU - O'Donnell, T.
AU - Olivieri, E.
AU - Oriol, C.
AU - Ouellet, J. L.
AU - Pagan, S.
AU - Pagliarone, C.
AU - Pagnanini, L.
AU - Pari, P.
AU - Pattavina, L.
AU - Paul, B.
AU - Pavan, M.
AU - Peng, H.
AU - Pessina, G.
AU - Pettinacci, V.
AU - Pira, C.
AU - Pirro, S.
AU - Poda, D. V.
AU - Polakovic, T.
AU - Polischuk, O. G.
AU - Pozzi, S.
AU - Previtali, E.
AU - Puiu, A.
AU - Ressa, A.
AU - Rizzoli, R.
AU - Rosenfeld, C.
AU - Rusconi, C.
AU - Sanglard, V.
AU - Scarpaci, J.
AU - Schmidt, B.
AU - Sharma, V.
AU - Shlegel, V.
AU - Singh, V.
AU - Sisti, M.
AU - Speller, D.
AU - Surukuchi, P. T.
AU - Taffarello, L.
AU - Tellier, O.
AU - Tomei, C.
AU - Tretyak, V. I.
AU - Tsymbaliuk, A.
AU - Velazquez, M.
AU - Vetter, K. J.
AU - Wagaarachchi, S. L.
AU - Wang, G.
AU - Wang, L.
AU - Welliver, B.
AU - Wilson, J.
AU - Wilson, K.
AU - Winslow, L. A.
AU - Xue, M.
AU - Yan, L.
AU - Yang, J.
AU - Yefremenko, V.
AU - Yumatov, V.
AU - Zarytskyy, M. M.
AU - Zhang, J.
AU - Zolotarova, A.
AU - Zucchelli, S.
N1 - Funding Information: The CUPID Collaboration thanks the directors and staff of the Laboratori Nazionali del Gran Sasso and the technical staff of our laboratories. This work was supported by the Istituto Nazionale di Fisica Nucleare (INFN); by the European Research Council (ERC) under the European Union Horizon 2020 program (H2020/2014-2020) with the ERC Advanced Grant No. 742345 (ERC-2016-ADG, project CROSS) and the Marie Sklodowska-Curie Grant Agreement No. 754496; by the Italian Ministry of University and Research (MIUR) through the grant Progetti di ricerca di Rilevante Interesse Nazionale (PRIN 2017, Grant No. 2017FJZMCJ); by the US National Science Foundation under Grants No. NSF-PHY-1401832, No. NSF-PHY-1614611, and No. NSF-PHY-1913374. This material is also based upon work supported by the US Department of Energy (DOE) Office of Science under Contracts No. DE-AC02-05CH11231 and NO. DE-AC02-06CH11357; and by the DOE Office of Science, Office of Nuclear Physics under Contracts No. DE-FG02-08ER41551, No. DE-SC0011091, No. DE-SC0012654, No. DE-SC0019316, No. DE-SC0019368, and No. DE-SC0020423. This work was also supported by the Russian Science Foundation under Grant No. 18-12-00003 and the National Research Foundation of Ukraine under Grant No. 2020.02/0011. This research used resources of the National Energy Research Scientific Computing Center (NERSC). This work makes use of both the diana data analysis and apollo data acquisition software packages, which were developed by the CUORICINO, CUORE, LUCIFER and CUPID-0 Collaborations. Publisher Copyright: © 2021 American Physical Society.
PY - 2021/6
Y1 - 2021/6
N2 - Precise characterization of detector time resolution is of crucial importance for next-generation cryogenic-bolometer experiments searching for neutrinoless double-beta decay, such as CUPID, in order to reject background due to pileup of two-neutrino double-beta decay events. In this paper, we describe a technique developed to study the pileup rejection capability of cryogenic bolometers. Our approach, which consists of producing controlled pileup events with a programmable wave-form generator, has the benefit that we can reliably and reproducibly control the time separation and relative energy of the individual components of the generated pileup events. The resulting data allow us to optimize and benchmark analysis strategies to discriminate between individual and pileup pulses. We describe a test of this technique performed with a small array of detectors at the Laboratori Nazionali del Gran Sasso, in Italy; we obtain a 90% rejection efficiency against pulser-generated pileup events with rise time of ∼15ms down to time separation between the individual events of about 2ms.
AB - Precise characterization of detector time resolution is of crucial importance for next-generation cryogenic-bolometer experiments searching for neutrinoless double-beta decay, such as CUPID, in order to reject background due to pileup of two-neutrino double-beta decay events. In this paper, we describe a technique developed to study the pileup rejection capability of cryogenic bolometers. Our approach, which consists of producing controlled pileup events with a programmable wave-form generator, has the benefit that we can reliably and reproducibly control the time separation and relative energy of the individual components of the generated pileup events. The resulting data allow us to optimize and benchmark analysis strategies to discriminate between individual and pileup pulses. We describe a test of this technique performed with a small array of detectors at the Laboratori Nazionali del Gran Sasso, in Italy; we obtain a 90% rejection efficiency against pulser-generated pileup events with rise time of ∼15ms down to time separation between the individual events of about 2ms.
UR - http://www.scopus.com/inward/record.url?scp=85109302693&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85109302693&partnerID=8YFLogxK
U2 - 10.1103/PhysRevC.104.015501
DO - 10.1103/PhysRevC.104.015501
M3 - Article
AN - SCOPUS:85109302693
VL - 104
JO - Physical Review C
JF - Physical Review C
SN - 2469-9985
IS - 1
M1 - 015501
ER -