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164 results on '"M. Faverzani"'

1. Optimization of the first CUPID detector module

Author

CUPID Collaboration, K. Alfonso, A. Armatol, C. Augier, F. T. Avignone, O. Azzolini, M. Balata, A. S. Barabash, G. Bari, A. Barresi, D. Baudin, F. Bellini, G. Benato, M. Beretta, M. Bettelli, M. Biassoni, J. Billard, V. Boldrini, A. Branca, C. Brofferio, C. Bucci, J. Camilleri, A. Campani, C. Capelli, S. Capelli, L. Cappelli, L. Cardani, P. Carniti, N. Casali, E. Celi, C. Chang, D. Chiesa, M. Clemenza, I. Colantoni, S. Copello, E. Craft, O. Cremonesi, R. J. Creswick, A. Cruciani, A. D’Addabbo, G. D’Imperio, S. Dabagov, I. Dafinei, F. A. Danevich, M. De Jesus, P. de Marcillac, S. Dell’Oro, S. Di Domizio, S. Di Lorenzo, T. Dixon, V. Dompè, A. Drobizhev, L. Dumoulin, G. Fantini, M. Faverzani, E. Ferri, F. Ferri, F. Ferroni, E. Figueroa-Feliciano, L. Foggetta, J. Formaggio, A. Franceschi, C. Fu, S. Fu, B. K. Fujikawa, A. Gallas, J. Gascon, S. Ghislandi, A. Giachero, A. Gianvecchio, L. Gironi, A. Giuliani, P. Gorla, C. Gotti, C. Grant, P. Gras, P. V. Guillaumon, T. D. Gutierrez, K. Han, E. V. Hansen, K. M. Heeger, D. L. Helis, H. Z. Huang, L. Imbert, J. Johnston, A. Juillard, G. Karapetrov, G. Keppel, H. Khalife, V. V. Kobychev, Yu. G. Kolomensky, S. I. Konovalov, R. Kowalski, T. Langford, M. Lefevre, R. Liu, Y. Liu, P. Loaiza, L. Ma, M. Madhukuttan, F. Mancarella, L. Marini, S. Marnieros, M. Martinez, R. H. Maruyama, Ph. Mas, B. Mauri, D. Mayer, G. Mazzitelli, Y. Mei, S. Milana, S. Morganti, T. Napolitano, M. Nastasi, J. Nikkel, S. Nisi, C. Nones, E. B. Norman, V. Novosad, I. Nutini, T. O’Donnell, E. Olivieri, M. Olmi, J. L. Ouellet, S. Pagan, C. Pagliarone, L. Pagnanini, L. Pattavina, M. Pavan, H. Peng, G. Pessina, V. Pettinacci, C. Pira, S. Pirro, D. V. Poda, O. G. Polischuk, I. Ponce, S. Pozzi, E. Previtali, A. Puiu, S. Quitadamo, A. Ressa, R. Rizzoli, C. Rosenfeld, P. Rosier, J. Scarpaci, B. Schmidt, V. Sharma, V. N. Shlegel, V. Singh, M. Sisti, P. Slocum, D. Speller, P. T. Surukuchi, L. Taffarello, C. Tomei, J. A. Torres, V. I. Tretyak, A. Tsymbaliuk, M. Velazquez, K. J. Vetter, S. L. Wagaarachchi, G. Wang, L. Wang, R. Wang, B. Welliver, J. Wilson, K. Wilson, L. A. Winslow, M. Xue, L. Yan, J. Yang, V. Yefremenko, V. I. Umatov, M. M. Zarytskyy, J. Zhang, A. Zolotarova, and S. Zucchelli

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract CUPID will be a next generation experiment searching for the neutrinoless double $$\beta $$ β decay, whose discovery would establish the Majorana nature of the neutrino. Based on the experience achieved with the CUORE experiment, presently taking data at LNGS, CUPID aims to reach a background free environment by means of scintillating Li $$_{2}$$ 2 $$^{100}$$ 100 MoO $$_4$$ 4 crystals coupled to light detectors. Indeed, the simultaneous heat and light detection allows us to reject the dominant background of $$\alpha $$ α particles, as proven by the CUPID-0 and CUPID-Mo demonstrators. In this work we present the results of the first test of the CUPID baseline module. In particular, we propose a new optimized detector structure and light sensors design to enhance the engineering and the light collection, respectively. We characterized the heat detectors, achieving an energy resolution of (5.9 ± 0.2) keV FWHM at the Q-value of $$^{100}$$ 100 Mo (about 3034 keV). We studied the light collection of the baseline CUPID design with respect to an alternative configuration which features gravity-assisted light detectors’ mounting. In both cases we obtained an improvement in the light collection with respect to past measures and we validated the particle identification capability of the detector, which ensures an $$\alpha $$ α particle rejection higher than 99.9%, fully satisfying the requirements for CUPID.

Published
2022
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2. Search for double-beta decay of $$\mathrm {^{130}Te}$$ 130 Te to the $$0^+$$ 0 + states of $$\mathrm {^{130}Xe}$$ 130 Xe with CUORE

Author

D. Q. Adams, C. Alduino, K. Alfonso, F. T. III Avignone, O. Azzolini, G. Bari, F. Bellini, G. Benato, M. Biassoni, A. Branca, C. Brofferio, C. Bucci, J. Camilleri, A. Caminata, A. Campani, L. Canonica, X. G. Cao, S. Capelli, L. Cappelli, L. Cardani, P. Carniti, N. Casali, E. Celi, D. Chiesa, M. Clemenza, S. Copello, C. Cosmelli, O. Cremonesi, R. J. Creswick, A. D’Addabbo, I. Dafinei, C. J. Davis, S. Dell’Oro, S. Di Domizio, V. Dompè, D. Q. Fang, G. Fantini, M. Faverzani, E. Ferri, F. Ferroni, E. Fiorini, M. A. Franceschi, S. J. Freedman, S. H. Fu, B. K. Fujikawa, A. Giachero, L. Gironi, A. Giuliani, P. Gorla, C. Gotti, T. D. Gutierrez, K. Han, K. M. Heeger, R. G. Huang, H. Z. Huang, J. Johnston, G. Keppel, Yu. G. Kolomensky, C. Ligi, L. Ma, Y. G. Ma, L. Marini, R. H. Maruyama, D. Mayer, Y. Mei, N. Moggi, S. Morganti, T. Napolitano, M. Nastasi, J. Nikkel, C. Nones, E. B. Norman, A. Nucciotti, I. Nutini, T. O’Donnell, J. L. Ouellet, S. Pagan, C. E. Pagliarone, L. Pagnanini, M. Pallavicini, L. Pattavina, M. Pavan, G. Pessina, V. Pettinacci, C. Pira, S. Pirro, S. Pozzi, E. Previtali, A. Puiu, C. Rosenfeld, C. Rusconi, M. Sakai, S. Sangiorgio, B. Schmidt, N. D. Scielzo, V. Sharma, V. Singh, M. Sisti, D. Speller, P. T. Surukuchi, L. Taffarello, F. Terranova, C. Tomei, K. J. Vetter, M. Vignati, S. L. Wagaarachchi, B. S. Wang, B. Welliver, J. Wilson, K. Wilson, L. A. Winslow, S. Zimmermann, and S. Zucchelli

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract The CUORE experiment is a large bolometric array searching for the lepton number violating neutrino-less double beta decay ( $$0\nu \beta \beta $$ 0 ν β β ) in the isotope $$\mathrm {^{130}Te}$$ 130 Te . In this work we present the latest results on two searches for the double beta decay (DBD) of $$\mathrm {^{130}Te}$$ 130 Te to the first $$0^{+}_2$$ 0 2 + excited state of $$\mathrm {^{130}Xe}$$ 130 Xe : the $$0\nu \beta \beta $$ 0 ν β β decay and the Standard Model-allowed two-neutrinos double beta decay ( $$2\nu \beta \beta $$ 2 ν β β ). Both searches are based on a 372.5 kg $$\times $$ × yr TeO $$_2$$ 2 exposure. The de-excitation gamma rays emitted by the excited Xe nucleus in the final state yield a unique signature, which can be searched for with low background by studying coincident events in two or more bolometers. The closely packed arrangement of the CUORE crystals constitutes a significant advantage in this regard. The median limit setting sensitivities at 90% Credible Interval (C.I.) of the given searches were estimated as $$\mathrm {S^{0\nu }_{1/2} = 5.6 \times 10^{24} \, \mathrm {yr}}$$ S 1 / 2 0 ν = 5.6 × 10 24 yr for the $${0\nu \beta \beta }$$ 0 ν β β decay and $$\mathrm {S^{2\nu }_{1/2} = 2.1 \times 10^{24} \, \mathrm {yr}}$$ S 1 / 2 2 ν = 2.1 × 10 24 yr for the $${2\nu \beta \beta }$$ 2 ν β β decay. No significant evidence for either of the decay modes was observed and a Bayesian lower bound at $$90\%$$ 90 % C.I. on the decay half lives is obtained as: $$\mathrm {(T_{1/2})^{0\nu }_{0^+_2} > 5.9 \times 10^{24} \, \mathrm {yr}}$$ ( T 1 / 2 ) 0 2 + 0 ν > 5.9 × 10 24 yr for the $$0\nu \beta \beta $$ 0 ν β β mode and $$\mathrm {(T_{1/2})^{2\nu }_{0^+_2} > 1.3 \times 10^{24} \, \mathrm {yr}}$$ ( T 1 / 2 ) 0 2 + 2 ν > 1.3 × 10 24 yr for the $$2\nu \beta \beta $$ 2 ν β β mode. These represent the most stringent limits on the DBD of $$^{130}$$ 130 Te to excited states and improve by a factor $$\sim 5$$ ∼ 5 the previous results on this process.

Published
2021
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3. A novel approach for nearly-coincident events rejection

Author

M. Borghesi, M. De Gerone, M. Faverzani, M. Fedkevych, E. Ferri, G. Gallucci, A. Giachero, A. Nucciotti, and A. Puiu

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract We present a novel technique, called DSVP (Discrimination through Singular Vectors Projections), to discriminate spurious events within a dataset. The purpose of this paper is to lay down a general procedure which can be tailored for a broad variety of applications. After describing the general concept, we apply the algorithm to the problem of identifying nearly coincident events in low temperature microcalorimeters in order to push the time resolution close to its intrinsic limit. In fact, from simulated datasets it was possible to achieve an effective time resolution even shorter than the sampling time of the system considered. The obtained results are contextualized in the framework of the HOLMES experiment, which aims at directly measuring the neutrino mass with the calorimetric approach, allowing to significally improve its statistical sensitivity.

Published
2021
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4. Characterization of cubic Li $$_{2}$$ 2 $$^{100}$$ 100 MoO $$_4$$ 4 crystals for the CUPID experiment

Author

The CUPID Collaboration, A. Armatol, E. Armengaud, W. Armstrong, C. Augier, F. T. Avignone, O. Azzolini, A. Barabash, G. Bari, A. Barresi, D. Baudin, F. Bellini, G. Benato, M. Beretta, L. Bergé, M. Biassoni, J. Billard, V. Boldrini, A. Branca, C. Brofferio, C. Bucci, J. Camilleri, S. Capelli, L. Cappelli, L. Cardani, P. Carniti, N. Casali, A. Cazes, E. Celi, C. Chang, M. Chapellier, A. Charrier, D. Chiesa, M. Clemenza, I. Colantoni, F. Collamati, S. Copello, O. Cremonesi, R. J. Creswick, A. Cruciani, A. D’Addabbo, G. D’Imperio, I. Dafinei, F. A. Danevich, M. de Combarieu, M. De Jesus, P. de Marcillac, S. Dell’Oro, S. Di Domizio, V. Dompè, A. Drobizhev, L. Dumoulin, G. Fantini, M. Faverzani, E. Ferri, F. Ferri, F. Ferroni, E. Figueroa-Feliciano, J. Formaggio, A. Franceschi, C. Fu, S. Fu, B. K. Fujikawa, J. Gascon, A. Giachero, L. Gironi, A. Giuliani, P. Gorla, C. Gotti, P. Gras, M. Gros, T. D. Gutierrez, K. Han, E. V. Hansen, K. M. Heeger, D. L. Helis, H. Z. Huang, R. G. Huang, L. Imbert, J. Johnston, A. Juillard, G. Karapetrov, G. Keppel, H. Khalife, V. V. Kobychev, Yu. G. Kolomensky, S. Konovalov, Y. Liu, P. Loaiza, L. Ma, M. Madhukuttan, F. Mancarella, R. Mariam, L. Marini, S. Marnieros, M. Martinez, R. H. Maruyama, B. Mauri, D. Mayer, Y. Mei, S. Milana, D. Misiak, T. Napolitano, M. Nastasi, X. F. Navick, J. Nikkel, R. Nipoti, S. Nisi, C. Nones, E. B. Norman, V. Novosad, I. Nutini, T. O’Donnell, E. Olivieri, C. Oriol, J. L. Ouellet, S. Pagan, C. Pagliarone, L. Pagnanini, P. Pari, L. Pattavina, B. Paul, M. Pavan, H. Peng, G. Pessina, V. Pettinacci, C. Pira, S. Pirro, D. V. Poda, T. Polakovic, O. G. Polischuk, S. Pozzi, E. Previtali, A. Puiu, A. Ressa, R. Rizzoli, C. Rosenfeld, C. Rusconi, V. Sanglard, J. A. Scarpaci, B. Schmidt, V. Sharma, V. Shlegel, V. Singh, M. Sisti, D. Speller, P. T. Surukuchi, L. Taffarello, O. Tellier, C. Tomei, V. I. Tretyak, A. Tsymbaliuk, M. Velazquez, K. J. Vetter, S. L. Wagaarachchi, G. Wang, L. Wang, B. Welliver, J. Wilson, K. Wilson, L. A. Winslow, M. Xue, L. Yan, J. Yang, V. Yefremenko, V. Yumatov, M. M. Zarytskyy, J. Zhang, A. Zolotarova, and S. Zucchelli

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract The CUPID Collaboration is designing a tonne-scale, background-free detector to search for double beta decay with sufficient sensitivity to fully explore the parameter space corresponding to the inverted neutrino mass hierarchy scenario. One of the CUPID demonstrators, CUPID-Mo, has proved the potential of enriched Li $$_{2}$$ 2 $$^{100}$$ 100 MoO $$_4$$ 4 crystals as suitable detectors for neutrinoless double beta decay search. In this work, we characterised cubic crystals that, compared to the cylindrical crystals used by CUPID-Mo, are more appealing for the construction of tightly packed arrays. We measured an average energy resolution of ( $$6.7\pm 0.6$$ 6.7 ± 0.6 ) keV FWHM in the region of interest, approaching the CUPID target of 5 keV FWHM. We assessed the identification of $$\alpha $$ α particles with and without a reflecting foil that enhances the scintillation light collection efficiency, proving that the baseline design of CUPID already ensures a complete suppression of this $$\alpha $$ α -induced background contribution. We also used the collected data to validate a Monte Carlo simulation modelling the light collection efficiency, which will enable further optimisations of the detector.

Published
2021
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5. Double-beta decay of $$^{130}\hbox {Te}$$ 130Te to the first $$0^+$$ 0+ excited state of $$^{130}\hbox {Xe}$$ 130Xe with CUORE-0

Author

C. Alduino, K. Alfonso, D. R. Artusa, F. T. Avignone III, O. Azzolini, T. I. Banks, G. Bari, J. W. Beeman, F. Bellini, A. Bersani, M. Biassoni, C. Brofferio, C. Bucci, A. Camacho, A. Caminata, L. Canonica, X. G. Cao, S. Capelli, L. Cappelli, L. Carbone, L. Cardani, P. Carniti, N. Casali, L. Cassina, D. Chiesa, N. Chott, M. Clemenza, S. Copello, C. Cosmelli, O. Cremonesi, R. J. Creswick, J. S. Cushman, A. D’Addabbo, I. Dafinei, C. J. Davis, S. Dell’Oro, M. M. Deninno, S. Di Domizio, M. L. Di Vacri, A. Drobizhev, D. Q. Fang, M. Faverzani, J. Feintzeig, G. Fernandes, E. Ferri, F. Ferroni, E. Fiorini, M. A. Franceschi, S. J. Freedman, B. K. Fujikawa, A. Giachero, L. Gironi, A. Giuliani, L. Gladstone, P. Gorla, C. Gotti, T. D. Gutierrez, E. E. Haller, K. Han, E. Hansen, K. M. Heeger, R. Hennings-Yeomans, K. P. Hickerson, H. Z. Huang, R. Kadel, G. Keppel, Yu. G. Kolomensky, A. Leder, C. Ligi, K. E. Lim, X. Liu, Y. G. Ma, M. Maino, L. Marini, M. Martinez, R. H. Maruyama, Y. Mei, N. Moggi, S. Morganti, P. J. Mosteiro, T. Napolitano, C. Nones, E. B. Norman, A. Nucciotti, T. O’Donnell, F. Orio, J. L. Ouellet, C. E. Pagliarone, M. Pallavicini, V. Palmieri, L. Pattavina, M. Pavan, G. Pessina, V. Pettinacci, G. Piperno, C. Pira, S. Pirro, S. Pozzi, E. Previtali, C. Rosenfeld, C. Rusconi, S. Sangiorgio, D. Santone, N. D. Scielzo, V. Singh, M. Sisti, A. R. Smith, L. Taffarello, M. Tenconi, F. Terranova, C. Tomei, S. Trentalange, M. Vignati, S. L. Wagaarachchi, B. S. Wang, H. W. Wang, J. Wilson, L. A. Winslow, T. Wise, A. Woodcraft, L. Zanotti, G. Q. Zhang, B. X. Zhu, S. Zimmermann, and S. Zucchelli

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract We report on a search for double beta decay of $$^{130}\hbox {Te}$$ 130Te to the first $$0^{+}$$ 0+ excited state of $$^{130}\hbox {Xe}$$ 130Xe using a $$9.8\,\hbox {kg}\cdot \hbox {yr}$$ 9.8kg·yr exposure of $$^{130}\hbox {Te}$$ 130Te collected with the CUORE-0 experiment. In this work we exploit different topologies of coincident events to search for both the neutrinoless and two-neutrino double beta decay modes. We find no evidence for either mode and place lower bounds on the half-lives: $$T^{0\nu }_{0^+_1}>7.9\cdot 10^{23}\hbox {yr}$$ T01+0ν>7.9·1023yr and $$T^{2\nu }_{0^+_1}>2.4\cdot 10^{23}\hbox {yr}$$ T01+2ν>2.4·1023yr ($$90\%\,\hbox {CL}$$ 90%CL ). Combining our results with those obtained by the CUORICINO experiment, we achieve the most stringent constraints available for these processes: $$T^{0\nu }_{0^+_1}>1.4\cdot 10^{24}\hbox {yr}$$ T01+0ν>1.4·1024yr and $$T^{2\nu }_{0^+_1}>2.5\cdot 10^{23}\hbox {yr}$$ T01+2ν>2.5·1023yr ($$90\%\,\hbox {CL}$$ 90%CL ).

Published
2019
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6. High-resolution high-speed microwave-multiplexed low temperature microcalorimeters for the HOLMES experiment

Author

B. Alpert, D. Becker, D. Bennet, M. Biasotti, M. Borghesi, G. Gallucci, M. De Gerone, M. Faverzani, E. Ferri, J. Fowler, J. Gard, A. Giachero, J. Hays–Wehle, G. Hilton, J. Mates, A. Nucciotti, A. Orlando, G. Pessina, A. Puiu, C. Reintsema, D. Schmidt, D. Swetz, J. Ullom, and L. Vale

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract We present the first performance results obtained with microwave multiplexed Transition Edge Sensors prototypes specifically designed for the HOLMES experiment, a project aimed at directly measuring the electron neutrino mass through the calorimetric measurement of the $$^{163}$$ 163 Ho electron capture spectrum. The detectors required for such an experiment feature a high energy resolution at the Q–value of the transition, around $$\sim $$ ∼ 2.8 keV, and a fast response time combined with the compatibility to be multiplexed in large arrays in order to collect a large statistics while keeping the pile-up contribution as small as possible. In addition, the design has to be suitable for future ion-implantation of $$^{163}$$ 163 Ho. The results obtained in these tests allowed us to identify the optimal detector design among several prototypes. The chosen detector achieved an energy resolution of (4.5 ± 0.3) eV on the chlorine K$$_\alpha $$ α line, at $$\sim $$ ∼ 2.6 keV, obtained with an exponential rise time of 14 $$\upmu $$ μ s. The achievements described in this paper pose a milestone for the HOLMES detectors, setting a baseline for the subsequent developments, aiming to the actual ion-implantation of the $$^{163}$$ 163 Ho nuclei. In the first section the HOLMES experiment is outlined along with its physics goal, while in the second section the HOLMES detectors are described; the experimental set-up and the calibration source used for the measurements described in this paper are reported in Sects. 3 and 4, respectively; finally, the details of the data analysis and the results obtained are reported in Sect. 6.

Published
2019
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7. Low energy analysis techniques for CUORE

Author

C. Alduino, K. Alfonso, D. R. Artusa, F. T. Avignone, O. Azzolini, G. Bari, J. W. Beeman, F. Bellini, G. Benato, A. Bersani, M. Biassoni, A. Branca, C. Brofferio, C. Bucci, A. Camacho, A. Caminata, L. Canonica, X. G. Cao, S. Capelli, L. Cappelli, L. Cardani, P. Carniti, N. Casali, L. Cassina, D. Chiesa, N. Chott, M. Clemenza, S. Copello, C. Cosmelli, O. Cremonesi, R. J. Creswick, J. S. Cushman, A. D’Addabbo, D. D’Aguanno, I. Dafinei, C. J. Davis, S. Dell’Oro, M. M. Deninno, S. Di Domizio, M. L. Di Vacri, A. Drobizhev, D. Q. Fang, M. Faverzani, E. Ferri, F. Ferroni, E. Fiorini, M. A. Franceschi, S. J. Freedman, B. K. Fujikawa, A. Giachero, L. Gironi, A. Giuliani, L. Gladstone, P. Gorla, C. Gotti, T. D. Gutierrez, E. E. Haller, K. Han, E. Hansen, K. M. Heeger, R. Hennings-Yeomans, H. Z. Huang, R. Kadel, G. Keppel, Yu. G. Kolomensky, A. Leder, C. Ligi, K. E. Lim, Y. G. Ma, M. Maino, L. Marini, M. Martinez, R. H. Maruyama, Y. Mei, N. Moggi, S. Morganti, P. J. Mosteiro, T. Napolitano, M. Nastasi, C. Nones, E. B. Norman, V. Novati, A. Nucciotti, T. O’Donnell, J. L. Ouellet, C. E. Pagliarone, M. Pallavicini, V. Palmieri, L. Pattavina, M. Pavan, G. Pessina, G. Piperno, C. Pira, S. Pirro, S. Pozzi, E. Previtali, C. Rosenfeld, C. Rusconi, M. Sakai, S. Sangiorgio, D. Santone, B. Schmidt, J. Schmidt, N. D. Scielzo, V. Singh, M. Sisti, A. R. Smith, L. Taffarello, F. Terranova, C. Tomei, M. Vignati, S. L. Wagaarachchi, B. S. Wang, H. W. Wang, B. Welliver, J. Wilson, L. A. Winslow, T. Wise, A. Woodcraft, L. Zanotti, G. Q. Zhang, S. Zimmermann, and S. Zucchelli

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract CUORE is a tonne-scale cryogenic detector operating at the Laboratori Nazionali del Gran Sasso (LNGS) that uses tellurium dioxide bolometers to search for neutrinoless double-beta decay of $$^{130}$$ 130 Te. CUORE is also suitable to search for low energy rare events such as solar axions or WIMP scattering, thanks to its ultra-low background and large target mass. However, to conduct such sensitive searches requires improving the energy threshold to 10 keV. In this paper, we describe the analysis techniques developed for the low energy analysis of CUORE-like detectors, using the data acquired from November 2013 to March 2015 by CUORE-0, a single-tower prototype designed to validate the assembly procedure and new cleaning techniques of CUORE. We explain the energy threshold optimization, continuous monitoring of the trigger efficiency, data and event selection, and energy calibration at low energies in detail. We also present the low energy background spectrum of CUORE-0 below $$60 \, \mathrm {keV}$$ 60 keV . Finally, we report the sensitivity of CUORE to WIMP annual modulation using the CUORE-0 energy threshold and background, as well as an estimate of the uncertainty on the nuclear quenching factor from nuclear recoils inCUORE-0.

Published
2017
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8. The projected background for the CUORE experiment

Author

C. Alduino, K. Alfonso, D. R. Artusa, F. T. Avignone, O. Azzolini, T. I. Banks, G. Bari, J. W. Beeman, F. Bellini, G. Benato, A. Bersani, M. Biassoni, A. Branca, C. Brofferio, C. Bucci, A. Camacho, A. Caminata, L. Canonica, X. G. Cao, S. Capelli, L. Cappelli, L. Carbone, L. Cardani, P. Carniti, N. Casali, L. Cassina, D. Chiesa, N. Chott, M. Clemenza, S. Copello, C. Cosmelli, O. Cremonesi, R. J. Creswick, J. S. Cushman, A. D’Addabbo, I. Dafinei, C. J. Davis, S. Dell’Oro, M. M. Deninno, S. Di Domizio, M. L. Di Vacri, A. Drobizhev, D. Q. Fang, M. Faverzani, G. Fernandes, E. Ferri, F. Ferroni, E. Fiorini, M. A. Franceschi, S. J. Freedman, B. K. Fujikawa, A. Giachero, L. Gironi, A. Giuliani, L. Gladstone, P. Gorla, C. Gotti, T. D. Gutierrez, E. E. Haller, K. Han, E. Hansen, K. M. Heeger, R. Hennings-Yeomans, K. P. Hickerson, H. Z. Huang, R. Kadel, G. Keppel, Yu. G. Kolomensky, A. Leder, C. Ligi, K. E. Lim, Y. G. Ma, M. Maino, L. Marini, M. Martinez, R. H. Maruyama, Y. Mei, N. Moggi, S. Morganti, P. J. Mosteiro, T. Napolitano, M. Nastasi, C. Nones, E. B. Norman, V. Novati, A. Nucciotti, T. O’Donnell, J. L. Ouellet, C. E. Pagliarone, M. Pallavicini, V. Palmieri, L. Pattavina, M. Pavan, G. Pessina, V. Pettinacci, G. Piperno, C. Pira, S. Pirro, S. Pozzi, E. Previtali, C. Rosenfeld, C. Rusconi, M. Sakai, S. Sangiorgio, D. Santone, B. Schmidt, J. Schmidt, N. D. Scielzo, V. Singh, M. Sisti, A. R. Smith, L. Taffarello, M. Tenconi, F. Terranova, C. Tomei, S. Trentalange, M. Vignati, S. L. Wagaarachchi, B. S. Wang, H. W. Wang, B. Welliver, J. Wilson, L. A. Winslow, T. Wise, A. Woodcraft, L. Zanotti, G. Q. Zhang, B. X. Zhu, S. Zimmermann, S. Zucchelli, and M. Laubenstein

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract The Cryogenic Underground Observatory for Rare Events (CUORE) is designed to search for neutrinoless double beta decay of $$^{130}$$ 130 Te with an array of 988 TeO $$_2$$ 2 bolometers operating at temperatures around 10 mK. The experiment is currently being commissioned in Hall A of Laboratori Nazionali del Gran Sasso, Italy. The goal of CUORE is to reach a 90% C.L. exclusion sensitivity on the $$^{130}$$ 130 Te decay half-life of 9 $$\times $$ × 10 $$^{25}$$ 25 years after 5 years of data taking. The main issue to be addressed to accomplish this aim is the rate of background events in the region of interest, which must not be higher than 10 $$^{-2}$$ - 2 counts/keV/kg/year. We developed a detailed Monte Carlo simulation, based on results from a campaign of material screening, radioassays, and bolometric measurements, to evaluate the expected background. This was used over the years to guide the construction strategies of the experiment and we use it here to project a background model for CUORE. In this paper we report the results of our study and our expectations for the background rate in the energy region where the peak signature of neutrinoless double beta decay of $$^{130}$$ 130 Te is expected.

Published
2017
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9. CUORE sensitivity to $$0\nu \beta \beta $$ 0 ν β β decay

Author

C. Alduino, K. Alfonso, D. R. Artusa, F. T. Avignone, O. Azzolini, T. I. Banks, G. Bari, J. W. Beeman, F. Bellini, G. Benato, A. Bersani, M. Biassoni, A. Branca, C. Brofferio, C. Bucci, A. Camacho, A. Caminata, L. Canonica, X. G. Cao, S. Capelli, L. Cappelli, L. Carbone, L. Cardani, P. Carniti, N. Casali, L. Cassina, D. Chiesa, N. Chott, M. Clemenza, S. Copello, C. Cosmelli, O. Cremonesi, R. J. Creswick, J. S. Cushman, A. D’Addabbo, I. Dafinei, C. J. Davis, S. Dell’Oro, M. M. Deninno, S. Di Domizio, M. L. Di Vacri, A. Drobizhev, D. Q. Fang, M. Faverzani, G. Fernandes, E. Ferri, F. Ferroni, E. Fiorini, M. A. Franceschi, S. J. Freedman, B. K. Fujikawa, A. Giachero, L. Gironi, A. Giuliani, L. Gladstone, P. Gorla, C. Gotti, T. D. Gutierrez, E. E. Haller, K. Han, E. Hansen, K. M. Heeger, R. Hennings-Yeomans, K. P. Hickerson, H. Z. Huang, R. Kadel, G. Keppel, Yu. G. Kolomensky, A. Leder, C. Ligi, K. E. Lim, Y. G. Ma, M. Maino, L. Marini, M. Martinez, R. H. Maruyama, Y. Mei, N. Moggi, S. Morganti, P. J. Mosteiro, T. Napolitano, M. Nastasi, C. Nones, E. B. Norman, V. Novati, A. Nucciotti, T. O’Donnell, J. L. Ouellet, C. E. Pagliarone, M. Pallavicini, V. Palmieri, L. Pattavina, M. Pavan, G. Pessina, V. Pettinacci, G. Piperno, C. Pira, S. Pirro, S. Pozzi, E. Previtali, C. Rosenfeld, C. Rusconi, M. Sakai, S. Sangiorgio, D. Santone, B. Schmidt, J. Schmidt, N. D. Scielzo, V. Singh, M. Sisti, A. R. Smith, L. Taffarello, M. Tenconi, F. Terranova, C. Tomei, S. Trentalange, M. Vignati, S. L. Wagaarachchi, B. S. Wang, H. W. Wang, B. Welliver, J. Wilson, L. A. Winslow, T. Wise, A. Woodcraft, L. Zanotti, G. Q. Zhang, B. X. Zhu, S. Zimmermann, and S. Zucchelli

Subjects
Astrophysics, QB460-466, Nuclear and particle physics. Atomic energy. Radioactivity, QC770-798
Abstract

Abstract We report a study of the CUORE sensitivity to neutrinoless double beta ( $$0\nu \beta \beta $$ 0 ν β β ) decay. We used a Bayesian analysis based on a toy Monte Carlo (MC) approach to extract the exclusion sensitivity to the $$0\nu \beta \beta $$ 0 ν β β decay half-life ( $$T_{1/2}^{\,0\nu }$$ T 1 / 2 0 ν ) at $$90\%$$ 90 % credibility interval (CI) – i.e. the interval containing the true value of $$T_{1/2}^{\,0\nu }$$ T 1 / 2 0 ν with $$90\%$$ 90 % probability – and the $$3~\sigma $$ 3 σ discovery sensitivity. We consider various background levels and energy resolutions, and describe the influence of the data division in subsets with different background levels. If the background level and the energy resolution meet the expectation, CUORE will reach a $$90\%$$ 90 % CI exclusion sensitivity of $$2\cdot 10^{25}$$ 2 · 10 25 year with 3 months, and $$9\cdot 10^{25}$$ 9 · 10 25 year with 5 years of live time. Under the same conditions, the discovery sensitivity after 3 months and 5 years will be $$7\cdot 10^{24}$$ 7 · 10 24 year and $$4\cdot 10^{25}$$ 4 · 10 25 year, respectively.

Published
2017
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10. Searching for Neutrinoless Double-Beta Decay of 130Te with CUORE

Author

D. R. Artusa, F. T. Avignone, O. Azzolini, M. Balata, T. I. Banks, G. Bari, J. Beeman, F. Bellini, A. Bersani, M. Biassoni, C. Brofferio, C. Bucci, X. Z. Cai, A. Camacho, L. Canonica, X. G. Cao, S. Capelli, L. Carbone, L. Cardani, M. Carrettoni, N. Casali, D. Chiesa, N. Chott, M. Clemenza, S. Copello, C. Cosmelli, O. Cremonesi, R. J. Creswick, I. Dafinei, A. Dally, V. Datskov, A. De Biasi, M. M. Deninno, S. Di Domizio, M. L. di Vacri, L. Ejzak, D. Q. Fang, H. A. Farach, M. Faverzani, G. Fernandes, E. Ferri, F. Ferroni, E. Fiorini, M. A. Franceschi, S. J. Freedman, B. K. Fujikawa, A. Giachero, L. Gironi, A. Giuliani, J. Goett, P. Gorla, C. Gotti, T. D. Gutierrez, E. E. Haller, K. Han, K. M. Heeger, R. Hennings-Yeomans, H. Z. Huang, R. Kadel, K. Kazkaz, G. Keppel, Yu. G. Kolomensky, Y. L. Li, C. Ligi, X. Liu, Y. G. Ma, C. Maiano, M. Maino, M. Martinez, R. H. Maruyama, Y. Mei, N. Moggi, S. Morganti, T. Napolitano, S. Nisi, C. Nones, E. B. Norman, A. Nucciotti, T. O’Donnell, F. Orio, D. Orlandi, J. L. Ouellet, M. Pallavicini, V. Palmieri, L. Pattavina, M. Pavan, M. Pedretti, G. Pessina, V. Pettinacci, G. Piperno, C. Pira, S. Pirro, E. Previtali, V. Rampazzo, C. Rosenfeld, C. Rusconi, E. Sala, S. Sangiorgio, N. D. Scielzo, M. Sisti, A. R. Smith, L. Taffarello, M. Tenconi, F. Terranova, W. D. Tian, C. Tomei, S. Trentalange, G. Ventura, M. Vignati, B. S. Wang, H. W. Wang, L. Wielgus, J. Wilson, L. A. Winslow, T. Wise, A. Woodcraft, L. Zanotti, C. Zarra, B. X. Zhu, and S. Zucchelli

Subjects
Physics, QC1-999
Abstract

Neutrinoless double-beta (0νββ) decay is a hypothesized lepton-number-violating process that offers the only known means of asserting the possible Majorana nature of neutrino mass. The Cryogenic Underground Observatory for Rare Events (CUORE) is an upcoming experiment designed to search for 0νββ decay of 130Te using an array of 988 TeO2 crystal bolometers operated at 10 mK. The detector will contain 206 kg of 130Te and have an average energy resolution of 5 keV; the projected 0νββ decay half-life sensitivity after five years of livetime is 1.6 × 1026 y at 1σ (9.5 × 1025 y at the 90% confidence level), which corresponds to an upper limit on the effective Majorana mass in the range 40–100 meV (50–130 meV). In this paper, we review the experimental techniques used in CUORE as well as its current status and anticipated physics reach.

Published
2015
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11. Search for Double-Beta Decay of $\mathrm{^{130}Te}$ to the $0^+$ States of $\mathrm{^{130}Xe}$ with CUORE

Author

CUORE Collaboration, Adams, D. Q., Alduino, C., Alfonso, K., Avignone III, F. T., Azzolini, O., Bari, G., Bellini, F., Benato, G., Branca, M. Biassoni A., Brofferio, C., Bucci, C., Camilleri, J., Caminata, A., Campani, A., Canonica, L., Cao, X. G., Capelli, S., Cappelli, L., Cardani, L., Casali, P. Carniti N., Celi, E., Copello, D. Chiesa M. Clemenza S., Cosmelli, C., Cremonesi, O., Creswick, R. J., D'Addabbo, A., Dafinei, I., Davis, C. J., Di Domizio, S. Dell'Oro S., Dompè, V., Fang, D. Q., Fantini, G., Ferri, M. Faverzani E., Ferroni, F., Fiorini, E., Franceschi, M. A., Freedman, S. J., Fu, S. H., Fujikawa, B. K., Giachero, A., Gironi, L., Giuliani, A., Gorla, P., Gotti, C., Gutierrez, T. D., Han, K., Heeger, K. M., Huang, R. G., Huang, H. Z., Johnston, J., Keppel, G., Kolomensky, Yu. G., Ligi, C., Ma, L., Ma, Y. G., Marini, L., Maruyama, R. H., Mayer, D., Mei, Y., Moggi, N., Morganti, S., Napolitano, T., Nastasi, M., Nikkel, J., Nones, C., Norman, E. B., Nucciotti, A., Nutini, I., O'Donnell, T., Ouellet, J. L., Pagan, S., Pagliarone, C. E., Pagnanini, L., Pallavicini, M., Pattavina, L., Pavan, M., Pessina, G., Pettinacci, V., Pira, C., Pirro, S., Pozzi, S., Previtali, E., Puiu, A., Rosenfeld, C., Rusconi, C., Sakai, M., Sangiorgio, S., Schmidt, B., Scielzo, N. D., Sharma, V., Singh, V., Sisti, M., Speller, D., Surukuchi, P. T., Taffarello, L., Terranova, F., Tomei, C., Vetter, K. J., Vignati, M., Wagaarachchi, S. L., Wang, B. S., Welliver, B., Wilson, J., Wilson, K., Winslow, L. A., Zimmermann, S., and Zucchelli, S.

Subjects
Nuclear Experiment
Abstract

The CUORE experiment is a large bolometric array searching for the lepton number violating neutrino-less double beta decay ($0\nu\beta\beta$) in the isotope $\mathrm{^{130}Te}$. In this work we present the latest results on two searches for the double beta decay (DBD) of $\mathrm{^{130}Te}$ to the first $0^{+}_2$ excited state of $\mathrm{^{130}Xe}$: the $0\nu\beta\beta$ decay and the Standard Model-allowed two-neutrinos double beta decay ($2\nu\beta\beta$). Both searches are based on a 372.5 kg$\times$yr TeO$_2$ exposure. The de-excitation gamma rays emitted by the excited Xe nucleus in the final state yield a unique signature, which can be searched for with low background by studying coincident events in two or more bolometers. The closely packed arrangement of the CUORE crystals constitutes a significant advantage in this regard. The median limit setting sensitivities at 90\% Credible Interval (C.I.) of the given searches were estimated as $\mathrm{S^{0\nu}_{1/2} = 5.6 \times 10^{24} \: \mathrm{yr}}$ for the ${0\nu\beta\beta}$ decay and $\mathrm{S^{2\nu}_{1/2} = 2.1 \times 10^{24} \: \mathrm{yr}}$ for the ${2\nu\beta\beta}$ decay. No significant evidence for either of the decay modes was observed and a Bayesian lower bound at $90\%$ C.I. on the decay half lives is obtained as: $\mathrm{(T_{1/2})^{0\nu}_{0^+_2} > 5.9 \times 10^{24} \: \mathrm{yr}}$ for the $0\nu\beta\beta$ mode and $\mathrm{(T_{1/2})^{2\nu}_{0^+_2} > 1.3 \times 10^{24} \: \mathrm{yr}}$ for the $2\nu\beta\beta$ mode. These represent the most stringent limits on the DBD of $^{130}$Te to excited states and improve by a factor $\sim5$ the previous results on this process., Comment: 13 pages, 6 figures

Published
2021
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12. Search for Double-Beta Decay of $\mathrm{^{130}Te}$ to the $0^+$ States of $\mathrm{^{130}Xe}$ with CUORE

Author

Collaboration, CUORE, Adams, DQ, Alduino, C, Alfonso, K, III, FT Avignone, Azzolini, O, Bari, G, Bellini, F, Benato, G, Branca, M Biassoni A, Brofferio, C, Bucci, C, Camilleri, J, Caminata, A, Campani, A, Canonica, L, Cao, XG, Capelli, S, Cappelli, L, Cardani, L, Casali, P Carniti N, Celi, E, Copello, D Chiesa M Clemenza S, Cosmelli, C, Cremonesi, O, Creswick, RJ, D'Addabbo, A, Dafinei, I, Davis, CJ, Domizio, S Dell'Oro S Di, Dompè, V, Fang, DQ, Fantini, G, Ferri, M Faverzani E, Ferroni, F, Fiorini, E, Franceschi, MA, Freedman, SJ, Fu, SH, Fujikawa, BK, Giachero, A, Gironi, L, Giuliani, A, Gorla, P, Gotti, C, Gutierrez, TD, Han, K, Heeger, KM, Huang, RG, Huang, HZ, Johnston, J, Keppel, G, Kolomensky, Yu G, Ligi, C, Ma, L, Ma, YG, Marini, L, Maruyama, RH, Mayer, D, Mei, Y, Moggi, N, Morganti, S, Napolitano, T, Nastasi, M, Nikkel, J, Nones, C, Norman, EB, Nucciotti, A, Nutini, I, O'Donnell, T, Ouellet, JL, Pagan, S, Pagliarone, CE, Pagnanini, L, Pallavicini, M, Pattavina, L, Pavan, M, Pessina, G, Pettinacci, V, Pira, C, Pirro, S, Pozzi, S, Previtali, E, Puiu, A, Rosenfeld, C, Rusconi, C, Sakai, M, Sangiorgio, S, Schmidt, B, Scielzo, ND, Sharma, V, Singh, V, Sisti, M, Speller, D, Surukuchi, PT, Taffarello, L, Terranova, F, Tomei, C, Vetter, KJ, and Vignati, M

Subjects
nucl-ex
Abstract

The CUORE experiment is a large bolometric array searching for the leptonnumber violating neutrino-less double beta decay ($0u\beta\beta$) in theisotope $\mathrm{^{130}Te}$. In this work we present the latest results on twosearches for the double beta decay (DBD) of $\mathrm{^{130}Te}$ to the first$0^{+}_2$ excited state of $\mathrm{^{130}Xe}$: the $0u\beta\beta$ decay andthe Standard Model-allowed two-neutrinos double beta decay ($2u\beta\beta$).Both searches are based on a 372.5 kg$\times$yr TeO$_2$ exposure. Thede-excitation gamma rays emitted by the excited Xe nucleus in the final stateyield a unique signature, which can be searched for with low background bystudying coincident events in two or more bolometers. The closely packedarrangement of the CUORE crystals constitutes a significant advantage in thisregard. The median limit setting sensitivities at 90\% Credible Interval (C.I.)of the given searches were estimated as $\mathrm{S^{0u}_{1/2} = 5.6 \times10^{24} \: \mathrm{yr}}$ for the ${0u\beta\beta}$ decay and$\mathrm{S^{2u}_{1/2} = 2.1 \times 10^{24} \: \mathrm{yr}}$ for the${2u\beta\beta}$ decay. No significant evidence for either of the decay modeswas observed and a Bayesian lower bound at $90\%$ C.I. on the decay half livesis obtained as: $\mathrm{(T_{1/2})^{0u}_{0^+_2} > 5.9 \times 10^{24} \:\mathrm{yr}}$ for the $0u\beta\beta$ mode and$\mathrm{(T_{1/2})^{2u}_{0^+_2} > 1.3 \times 10^{24} \: \mathrm{yr}}$ for the$2u\beta\beta$ mode. These represent the most stringent limits on the DBD of$^{130}$Te to excited states and improve by a factor $\sim5$ the previousresults on this process.

Published
2021

13. Status of the HOLMES Experiment

Author

M. De Gerone, B. Alpert, M. Balata, D. T. Becker, D. A. Bennett, A. Bevilacqua, M. Borghesi, G. Ceruti, G. De Bodin De Galembert, R. Dressler, M. Faverzani, M. Fedkevych, E. Ferri, J. W. Fowler, G. Gallucci, J. D. Gard, F. Gatti, A. Giachero, G. C. Hilton, U. Köster, M. Lusignoli, P. Manfrinetti, J. A. B. Mates, E. Maugeri, S. Nisi, A. Nucciotti, L. Parodi, G. Pessina, S. Ragazzi, C. D. Reintsema, D. R. Schmidt, D. Schumann, F. Siccardi, D. S. Swetz, J. N. Ullom, and L. R. Vale

Subjects
General Materials Science, Condensed Matter Physics, Atomic and Molecular Physics, and Optics
Published
2022
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14. Commissioning of the Ion Implanter for the HOLMES Experiment

Author

M. De Gerone, A. Bevilacqua, M. Biasotti, M. Borghesi, N. Cerboni, G. Ceruti, G. De Bodin&nbsp, Deundefined Galembert, M. Faverzani, M. Fedkevych, E. Ferri, G. Gallucci, F. Gatti, A. Giachero, A. Loundefined, Cicero, E. Maugeri, P. Manfrinetti, A. Nucciotti, L. Parodi, G. Pessina, P. Pollovio, R. Puppo, S. Ragazzi, C. Rossi, D. Schumann, F. Siccardi, De Gerone, M, Bevilacqua, A, Biasotti, M, Borghesi, M, Cerboni, N, Ceruti, G, De Bodin&nbsp, G, Galembert, D, Faverzani, M, Fedkevych, M, Ferri, E, Gallucci, G, Gatti, F, Giachero, A, Lo&nbsp, A, Cicero, Maugeri, E, Manfrinetti, P, Nucciotti, A, Parodi, L, Pessina, G, Pollovio, P, Puppo, R, Ragazzi, S, Rossi, C, Schumann, D, and Siccardi, F

Subjects
Holmium, Ion implanter, Neutrino mass measurement, General Materials Science, Condensed Matter Physics, Atomic and Molecular Physics, and Optics
Abstract

The HOLMES experiment aims to directly measure the ν mass studying the 163Ho electron capture decay spectrum developing arrays of TES-based microcalorimeters implanted with O(300 Bq/detector) Ho atoms. The embedding of the source inside detectors is a crucial step of the experiment. Because the 163Ho production process (neutron irradiation of a 162Er sample) is not perfectly free from impurities, Ho source must be separated from a lot of contaminants. A chemical processing removes every species other than Ho, but it is not sufficient to remove all isotope-related background sources: Indeed, 166mHo beta decay can produce fake signal in the region of interest. For this reason, a dedicated implantation system was set up. It is designed to achieve the separation power better than 5σ at 163/166 a.m.u. allowing an efficient Ho ions implantation inside microcalorimeter absorbers. Its main components are a 50 kV sputter-based ion source, a magnetic dipole and a target chamber. A specially designed co-evaporation system was designed to “grow” the gold microcalorimeter absorber during the implantation process, increasing the maximum achievable activity which can be implanted. The machine performances were evaluated by means of calibration runs using 63Cu/65Cu and Mo beams. A special care was given to the study of the more effective way to populate source plasma with Ho ions obtained from different Ho compounds by sputtering process. In this work, the machine development and commissioning are described.

Published
2022
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15. Development of Quantum Limited Superconducting Amplifiers for Advanced Detection

Author

S. Pagano, C. Barone, M. Borghesi, W. Chung, G. Carapella, A. P. Caricato, I. Carusotto, A. Cian, D. Di Gioacchino, E. Enrico, P. Falferi, L. Fasolo, M. Faverzani, E. Ferri, G. Filatrella, C. Gatti, A. Giachero, D. Giubertoni, A. Greco, C. Kutlu, A. Leo, C. Ligi, G. Maccarrone, B. Margesin, G. Maruccio, A. Matlashov, C. Mauro, R. Mezzena, A. G. Monteduro, A. Nucciotti, L. Oberto, V. Pierro, L. Piersanti, M. Rajteri, A. Rettaroli, S. Rizzato, Y. K. Semertzidis, S. Uchaikin, A. Vinante, Pagano, Sergio, Barone, Carlo, Borghesi, Matteo, Chung, Woohyun, Carapella, Giovanni, Caricato, Anna Paola, Carusotto, Iacopo, Cian, Alessandro, Di Gioacchino, Daniele, Enrico, Emanuele, Falferi, Paolo, Fasolo, Luca, Faverzani, Marco, Ferri, Elena, Filatrella, Giovanni, Gatti, Claudio, Giachero, Andrea, Giubertoni, Damiano, Greco, Angelo, Kutlu, Caglar, Leo, Angelo, Ligi, C., Maccarrone, Giovanni, Margesin, Benno, Maruccio, Giuseppe, Matlashov, Andrei, Mauro, Costantino, Mezzena, Renato, Monteduro, Anna Grazia, Nucciotti, Angelo, Oberto, Luca, Pierro, Vincenzo, Piersanti, Luca, Rajteri, Mauro, Rizzato, Silvia, Semertzidis, Yannis K, Uchaikin, Sergey V., Vinante, Andrea, Pagano, S, Barone, C, Borghesi, M, Chung, W, Carapella, G, Caricato, A, Carusotto, I, Cian, A, Di Gioacchino, D, Enrico, E, Falferi, P, Fasolo, L, Faverzani, M, Ferri, E, Filatrella, G, Gatti, C, Giachero, A, Giubertoni, D, Greco, A, Kutlu, C, Leo, A, Ligi, C, Maccarrone, G, Margesin, B, Maruccio, G, Matlashov, A, Mauro, C, Mezzena, R, Monteduro, A, Nucciotti, A, Oberto, L, Pierro, V, Piersanti, L, Rajteri, M, Rizzato, S, Semertzidis, Y, Uchaikin, S, and Vinante, A

Subjects
Josephson junctions, Superconducting microwave devices, Microwave amplifiers, Physics, superconducting microwave device, Condensed Matter Physics, Electronic, Optical and Magnetic Materials, Physics, Superconducting microwave devices,Bandwidth, Power transmission lines, Josephson junctions, Microwave amplifiers, Inductance, Bandwidth, Josephson junction, Power transmission lines, Superconducting device noise, microwave amplifier, Electrical and Electronic Engineering, Inductance
Abstract

Ultralow-noise microwave amplification and detection play a central role in different applications, going from fundamental physics experiments to the deployment of quantum technologies. In many applications the necessity of reading multiple detectors, or cavities or qubits, calls for large bandwidth amplifiers with the lowest possible noise. Current technologies are based on High Electron Mobility Transistors and Josephson Parametric Amplifiers. Both have limitations, the former in terms of the minimum noise, the latter in terms of bandwidth. Superconducting Traveling Wave Parametric Amplifiers (TWPAs) have the potential of offering quantum limited noise and large bandwidth. These amplifiers are based on the parametric amplification of microwaves traveling along a transmission line with embedded nonlinear elements. We are developing superconducting TWPAs based both on Josephson junction arrays (Traveling Wave Josephson Parametric mplifiers) and on nonlinear kinetic inductance (Dispersion Engineered Traveling Wave Kinetic Inductance Amplifiers). Our goal is to achieve large bandwidth (in the 5 to 10 GHz range), large gain (more than 20 dB), large saturation power (more than -50 dBm), and near quantum limited noise (noise temperature less than 600 mK). Current achievements in the design and development of the high performance TWPAs are here reported and discussed, together with current limitations and possible future developments.

Published
2022
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16. Development and commissioning of the ion implanter for the HOLMES experiment

Author

M. De Gerone, A. Bevilacqua, M. Borghesi, N. Cerboni, G. Ceruti, G. De Bodin De Galembert, M. Faverzani, M. Fedkevych, E. Ferri, G. Gallucci, F. Gatti, A. Giachero, E. Maugeri, P. Manfrinetti, A. Nucciotti, L. Parodi, G. Pessina, S. Ragazzi, D. Schumann, F. Siccardi, De Gerone, M, Bevilacqua, A, Borghesi, M, Cerboni, N, Ceruti, G, De Bodin De Galembert, G, Faverzani, M, Fedkevych, M, Ferri, E, Gallucci, G, Gatti, F, Giachero, A, Maugeri, E, Manfrinetti, P, Nucciotti, A, Parodi, L, Pessina, G, Ragazzi, S, Schumann, D, and Siccardi, F

Subjects
Nuclear and High Energy Physics, Holmium, Ion implanter, Instrumentation, Ion source
Abstract

The HOLMES experiment aims to directly measure the ν mass studying the 163Ho electron capture decay spectrum, using arrays of TES-based micro-calorimeters implanted with O(102 Bq/detector) 163Ho atoms. The neutron irradiation of 162Er enriched samples, used for the production of 163Ho, also generates radioactive contaminants. Chemical processes have been developed to extract the Ho fraction with high efficiency. The radioactive Ho isotope 166mHo is also present in the final sample and could significantly contribute to background events in the final spectrum. For this reason a dedicated implantation/mass separator has been set up and commissioned. It is designed to achieve more than 5 σ separation 163/166 u simultaneously allowing an efficient 163Ho atoms embedding inside micro-calorimeter absorbers. Its main components are a 50 kV sputter-based ion source, a magnetic dipole and a target chamber. A specially designed co-evaporation system has been implemented to deposit gold on the detector absorbers during implantation to overcome the 163Ho source saturation problem. The system performances in terms of achievable beam current, profile and mass separation have been evaluated by means of calibration runs using Cu, Mo, Au and 165Ho beams. An intensive study was done to optimize the target containing 163Ho in order to achieve a large fraction of ionized Ho in the beam. In this work, the machine development and commissioning will be described.

Published
2023

17. Progress in the development of a KITWPA for the DARTWARS project

Author

M. Borghesi, C. Barone, S. Capelli, G. Carapella, A.P. Caricato, I. Carusotto, A. Cian, D. Di Gioacchino, E. Enrico, P. Falferi, L. Fasolo, M. Faverzani, E. Ferri, G. Filatrella, C. Gatti, A. Giachero, D. Giubertoni, V. Granata, A. Greco, C. Guarcello, D. Labranca, A. Leo, C. Ligi, G. Maccarrone, F. Mantegazzini, B. Margesin, G. Maruccio, C. Mauro, R. Mezzena, A.G. Monteduro, A. Nucciotti, L. Oberto, L. Origo, S. Pagano, V. Pierro, L. Piersanti, M. Rajteri, A. Rettaroli, S. Rizzato, A. Vinante, M. Zannoni, Borghesi, M, Barone, C, Capelli, S, Carapella, G, Caricato, A, Carusotto, I, Cian, A, Di Gioacchino, D, Enrico, E, Falferi, P, Fasolo, L, Faverzani, M, Ferri, E, Filatrella, G, Gatti, C, Giachero, A, Giubertoni, D, Granata, V, Greco, A, Guarcello, C, Labranca, D, Leo, A, Ligi, C, Maccarrone, G, Mantegazzini, F, Margesin, B, Maruccio, G, Mauro, C, Mezzena, R, Monteduro, A, Nucciotti, A, Oberto, L, Origo, L, Pagano, S, Pierro, V, Piersanti, L, Rajteri, M, Rettaroli, A, Rizzato, S, Vinante, A, and Zannoni, M

Subjects
Superconductivity (cond-mat.supr-con), Nuclear and High Energy Physics, Quantum Physics, KITWPA, Condensed Matter - Superconductivity, Superconducting circuit, Parametric amplifier, Readout, Superconducting circuits, FOS: Physical sciences, Quantum Physics (quant-ph), Instrumentation
Abstract

DARTWARS (Detector Array Readout with Traveling Wave AmplifieRS) is a three years project that aims to develop high-performing innovative Traveling Wave Parametric Amplifiers (TWPAs) for low temperature detectors and qubit readout (C-band). The practical development follows two different promising approaches, one based on the Josephson junctions (TWJPA) and the other one based on the kinetic inductance of a high-resistivity superconductor (KITWPA). This paper presents the advancements made by the DARTWARS collaboration to produce a first working prototype of a KITWPA., 3 pages, 4 figures. Proceeding of Pisa15th Meeting conference

Published
2022

18. An updated overview of the HOLMES status

Author

M. Borghesi, B. Alpert, M. Balata, D. Becker, D. Bennet, E. Celasco, N. Cerboni, M. De Gerone, R. Dressler, M. Faverzani, M. Fedkevych, E. Ferri, J. Fowler, G. Gallucci, J. Gard, F. Gatti, A. Giachero, G. Hilton, U. Koster, D. Labranca, M. Lusignoli, J. Mates, E. Maugeri, S. Nisi, A. Nucciotti, L. Origo, G. Pessina, S. Ragazzi, C. Reintsema, D. Schmidt, D. Schumann, D. Swetz, J. Ullom, L. Vale, Borghesi, M, Alpert, B, Balata, M, Becker, D, Bennet, D, Celasco, E, Cerboni, N, De Gerone, M, Dressler, R, Faverzani, M, Fedkevych, M, Ferri, E, Fowler, J, Gallucci, G, Gard, J, Gatti, F, Giachero, A, Hilton, G, Koster, U, Labranca, D, Lusignoli, M, Mates, J, Maugeri, E, Nisi, S, Nucciotti, A, Origo, L, Pessina, G, Ragazzi, S, Reintsema, C, Schmidt, D, Schumann, D, Swetz, D, Ullom, J, and Vale, L

Subjects
Nuclear and High Energy Physics, Low temperature detector, Microwave multixplexing readout, Neutrino ma, TES, Instrumentation
Abstract

HOLMES is an ERC project started in 2014 that will perform a model independent measurement of the neutrino mass with a sensitivity of the order of 1 eV. In order to reach its goal sensitivity, HOLMES will use 1000 low temperature microcalorimeters, each implanted with an activity of 300 Bq of 163Ho, performing thus a calorimetric measurement. This contribution presents the recent results achieved that lay the grounds for the low-activity phase of the HOLMES experiment, that will lead to its first limit on the neutrino mass.

Published
2023
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19. Preface

Author

M Sisti, A. Giachero, Emanuele Ferri, M Faverzani, A. Puiu, and A Nucciotti

Subjects
Physics, General Materials Science, Cryogenics, Condensed Matter Physics, Engineering physics, Atomic and Molecular Physics, and Optics
Published
2020
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20. Pulse Shape Analysis in Low-temperature Calorimeters Read-Out by NTD Thermistors

Author

M. Biassoni, C. Brofferio, P. Carniti, M. Faverzani, E. Ferri, S. Ghislandi, A. Giachero, C. Gotti, I. Nutini, G. Pessina, S. Quitadamo, Biassoni, M, Brofferio, C, Carniti, P, Faverzani, M, Ferri, E, Ghislandi, S, Giachero, A, Gotti, C, Nutini, I, Pessina, G, and Quitadamo, S

Subjects
Neutron Trasmutation Doped (NTD) thermistor, Low-temperature calorimeter, Bolometer, General Materials Science, Pulse shape, Condensed Matter Physics, Atomic and Molecular Physics, and Optics, Thermal capacitance
Abstract

We present the application of a simplified thermal model for the description of the response function of low-temperature calorimeters consisting of $$\hbox {TeO}_2$$ TeO 2 crystals read-out by NTD thermistors operated at temperatures $$T \sim 10$$ T ∼ 10 mK. Relying on both the analysis of the NTD load curves (from which we measured the main thermal conductances of the system) (Biassoni et al. in J Low Temp Phys 206:80–96, 2022) and on the analysis of the shape of thermal pulses acquired at different temperatures, we identified and quantified the physical parameters that determine the characteristic time constants of the pulses. In particular, we identified three different contributions to the heat capacity of the detector: the crystal phonon system (scaling as $$T^3$$ T 3 ), the NTD electron system (scaling as T) and a term related to the metalization process of the NTD electrodes (scaling as $$T^{-2}$$ T - 2 ).

Published
2022

21. CUORE opens the door to tonne-scale cryogenics experiments

Author

L. Canonica, L. Marini, Kevin Hickerson, J. Schmidt, Massimiliano Clemenza, Carlo Cosmelli, S. Copello, L. Gladstone, M. Guerzoni, L. Ma, J. Johnston, A. Leder, M. Iannone, Irene Nutini, Paolo Carniti, Vladimir Datskov, R. J. Creswick, M. M. Deninno, G. Fantini, F. Bellini, I. C. Bandac, Yu-Gang Ma, D. Santone, V. Sharma, C. Brofferio, P. J. Mosteiro, A. Caminata, Ezio Previtali, B. Welliver, Evelyn Ferri, H. Z. Huang, G. Keppel, K. E. Lim, X. G. Cao, F. Bragazzi, Ettore Fiorini, V. Novati, C. Rusconi, N. Chott, T. Wise, C. Crescentini, R. Gaigher, L. Zanotti, Andrea Giachero, C. Maiano, N. Moggi, C. Martinez Amaya, S. S. Nagorny, A. Pelosi, G. Piperno, D. Q. Adams, L. Risegari, K. Alfonso, F. Terranova, Davide Chiesa, C. Rosenfeld, Deqing Fang, S. Pagan, S. Dell'Oro, M. L. Di Vacri, D. Mayer, Samuele Sangiorgio, Stefano Nisi, P. T. Surukuchi, S. Morganti, S. Zucchelli, J. Camilleri, A. Nucciotti, M. Sisti, P. Gorla, E. V. Hansen, F. Ferroni, C. Tomei, Elena Sala, L. Ioannucci, D. Speller, F. Alessandria, M. I. Martínez, Eugene E. Haller, C. Alduino, F. Rimondi, G. Ceruti, K. Wilson, L. Taffarello, Marisa Pedretti, R. Hennings-Yeomans, S. Pirro, Carlo Ligi, M. Faverzani, M. Beretta, Y. Mei, M. Tessaro, Jeffrey W. Beeman, M. Capodiferro, A. Bersani, N. D. Scielzo, M. Barucci, L. Cappelli, D. Biare, C. J. Davis, A. Camacho, Jonathan Ouellet, D. Conventi, J. Wallig, K. M. Heeger, L. Pagnanini, A. Giuliani, G. Bari, M. Cariello, Lindley Winslow, A. Campani, S. L. Wagaarachchi, M. Maino, Guoqiang Zhang, M. Carrettoni, R. Mazza, A. Branca, A. Bryant, J. Nikkel, C. Pira, H.W. Wang, M. Perego, T. I. Banks, S. Zimmermann, Ke Han, Reina H. Maruyama, S. Ghislandi, T. O'Donnell, S. Di Domizio, Simone Capelli, R. W. Kadel, Stuart J. Freedman, G. Ventura, A. Drobizhev, C. Bulfon, C. Zarra, Laura Cardani, V. Dompè, M. Balata, L. Di Paolo, A. D'Addabbo, L. Pattavina, B. K. Fujikawa, Stefano Pozzi, Alan R. Smith, D. Orlandi, Larissa M. Ejzak, M. Vignati, B. X. Zhu, V. Pettinacci, L. Kogler, E. Celi, L. Tatananni, S.H. Fu, E. Andreotti, M. A. Franceschi, R. Cereseto, I. Dafinei, M. Sakai, D. D'Aguanno, F. Stivanello, R. G. Huang, D. Schaeffer, C. Guandalini, F. Orio, Vasundhara Singh, B. Schmidt, B. S. Wang, O. Azzolini, Kai Vetter, M. Olcese, Jeremy S. Cushman, V. Palmieri, Eric B. Norman, M. Guetti, T. Napolitano, M. Biassoni, F. Del Corso, R. Faccini, Giovanni Benato, A. Buccheri, C. Salvioni, Yu. G. Kolomensky, R. Pedrotta, Lorenzo Cassina, C. Nones, A. Puiu, Marco Pallavicini, S. Quitadamo, G. Pessina, James R. Wilson, R. Liu, Massimiliano Nastasi, M. Pavan, E. Olivieri, L. Gironi, F. T. Avignone, Claudio Gotti, N. Casali, F. Reindl, Oliviero Cremonesi, J. Goett, M. Tenconi, C. Pagliarone, C. Rossi, A. Chiarini, C. Bucci, T. D. Gutierrez, Adams, D, Alduino, C, Alessandria, F, Alfonso, K, Andreotti, E, Avignone, F, Azzolini, O, Balata, M, Bandac, I, Banks, T, Bari, G, Barucci, M, Beeman, J, Bellini, F, Benato, G, Beretta, M, Bersani, A, Biare, D, Biassoni, M, Bragazzi, F, Branca, A, Brofferio, C, Bryant, A, Buccheri, A, Bucci, C, Bulfon, C, Camacho, A, Camilleri, J, Caminata, A, Campani, A, Canonica, L, Cao, X, Capelli, S, Capodiferro, M, Cappelli, L, Cardani, L, Cariello, M, Carniti, P, Carrettoni, M, Casali, N, Cassina, L, Celi, E, Cereseto, R, Ceruti, G, Chiarini, A, Chiesa, D, Chott, N, Clemenza, M, Conventi, D, Copello, S, Cosmelli, C, Cremonesi, O, Crescentini, C, Creswick, R, Cushman, J, D'Addabbo, A, D'Aguanno, D, Dafinei, I, Datskov, V, Davis, C, Corso, F, Dell'Oro, S, Deninno, M, Di Domizio, S, Dompe, V, Di Vacri, M, Di Paolo, L, Drobizhev, A, Ejzak, L, Faccini, R, Fang, D, Fantini, G, Faverzani, M, Ferri, E, Ferroni, F, Fiorini, E, Franceschi, M, Freedman, S, Fu, S, Fujikawa, B, Gaigher, R, Ghislandi, S, Giachero, A, Gironi, L, Giuliani, A, Gladstone, L, Goett, J, Gorla, P, Gotti, C, Guandalini, C, Guerzoni, M, Guetti, M, Gutierrez, T, Haller, E, Han, K, Hansen, E, Heeger, K, Hennings-Yeomans, R, Hickerson, K, Huang, R, Huang, H, Iannone, M, Ioannucci, L, Johnston, J, Kadel, R, Keppel, G, Kogler, L, Kolomensky, Y, Leder, A, Ligi, C, Lim, K, Liu, R, Ma, L, Ma, Y, Maiano, C, Maino, M, Marini, L, Martinez, M, Amaya, C, Maruyama, R, Mayer, D, Mazza, R, Mei, Y, Moggi, N, Morganti, S, Mosteiro, P, Nagorny, S, Napolitano, T, Nastasi, M, Nikkel, J, Nisi, S, Nones, C, Norman, E, Novati, V, Nucciotti, A, Nutini, I, O'Donnell, T, Olcese, M, Olivieri, E, Orio, F, Orlandi, D, Ouellet, J, Pagan, S, Pagliarone, C, Pagnanini, L, Pallavicini, M, Palmieri, V, Pattavina, L, Pavan, M, Pedretti, M, Pedrotta, R, Pelosi, A, Perego, M, Pessina, G, Pettinacci, V, Piperno, G, Pira, C, Pirro, S, Pozzi, S, Previtali, E, Puiu, A, Quitadamo, S, Reindl, F, Rimondi, F, Risegari, L, Rosenfeld, C, Rossi, C, Rusconi, C, Sakai, M, Sala, E, Salvioni, C, Sangiorgio, S, Santone, D, Schaeffer, D, Schmidt, B, Schmidt, J, Scielzo, N, Sharma, V, Singh, V, Sisti, M, Smith, A, Speller, D, Stivanello, F, Surukuchi, P, Taffarello, L, Tatananni, L, Tenconi, M, Terranova, F, Tessaro, M, Tomei, C, Ventura, G, Vetter, K, Vignati, M, Wagaarachchi, S, Wallig, J, Wang, B, Wang, H, Welliver, B, Wilson, J, Wilson, K, Winslow, L, Wise, T, Zanotti, L, Zarra, C, Zhang, G, Zhu, B, Zimmermann, S, Zucchelli, S, Adams D.Q., Alduino C., Alessandria F., Alfonso K., Andreotti E., Avignone F.T., Azzolini O., Balata M., Bandac I., Banks T.I., Bari G., Barucci M., Beeman J.W., Bellini F., Benato G., Beretta M., Bersani A., Biare D., Biassoni M., Bragazzi F., Branca A., Brofferio C., Bryant A., Buccheri A., Bucci C., Bulfon C., Camacho A., Camilleri J., Caminata A., Campani A., Canonica L., Cao X.G., Capelli S., Capodiferro M., Cappelli L., Cardani L., Cariello M., Carniti P., Carrettoni M., Casali N., Cassina L., Celi E., Cereseto R., Ceruti G., Chiarini A., Chiesa D., Chott N., Clemenza M., Conventi D., Copello S., Cosmelli C., Cremonesi O., Crescentini C., Creswick R.J., Cushman J.S., D'Addabbo A., D'Aguanno D., Dafinei I., Datskov V., Davis C.J., Del Corso F., Dell'Oro S., Deninno M.M., Di Domizio S., Dompe V., Di Vacri M.L., Di Paolo L., Drobizhev A., Ejzak L., Faccini R., Fang D.Q., Fantini G., Faverzani M., Ferri E., Ferroni F., Fiorini E., Franceschi M.A., Freedman S.J., Fu S.H., Fujikawa B.K., Gaigher R., Ghislandi S., Giachero A., Gironi L., Giuliani A., Gladstone L., Goett J., Gorla P., Gotti C., Guandalini C., Guerzoni M., Guetti M., Gutierrez T.D., Haller E.E., Han K., Hansen E.V., Heeger K.M., Hennings-Yeomans R., Hickerson K.P., Huang R.G., Huang H.Z., Iannone M., Ioannucci L., Johnston J., Kadel R., Keppel G., Kogler L., Kolomensky Y.G., Leder A., Ligi C., Lim K.E., Liu R., Ma L., Ma Y.G., Maiano C., Maino M., Marini L., Martinez M., Amaya C.M., Maruyama R.H., Mayer D., Mazza R., Mei Y., Moggi N., Morganti S., Mosteiro P.J., Nagorny S.S., Napolitano T., Nastasi M., Nikkel J., Nisi S., Nones C., Norman E.B., Novati V., Nucciotti A., Nutini I., O'Donnell T., Olcese M., Olivieri E., Orio F., Orlandi D., Ouellet J.L., Pagan S., Pagliarone C.E., Pagnanini L., Pallavicini M., Palmieri V., Pattavina L., Pavan M., Pedretti M., Pedrotta R., Pelosi A., Perego M., Pessina G., Pettinacci V., Piperno G., Pira C., Pirro S., Pozzi S., Previtali E., Puiu A., Quitadamo S., Reindl F., Rimondi F., Risegari L., Rosenfeld C., Rossi C., Rusconi C., Sakai M., Sala E., Salvioni C., Sangiorgio S., Santone D., Schaeffer D., Schmidt B., Schmidt J., Scielzo N.D., Sharma V., Singh V., Sisti M., Smith A.R., Speller D., Stivanello F., Surukuchi P.T., Taffarello L., Tatananni L., Tenconi M., Terranova F., Tessaro M., Tomei C., Ventura G., Vetter K.J., Vignati M., Wagaarachchi S.L., Wallig J., Wang B.S., Wang H.W., Welliver B., Wilson J., Wilson K., Winslow L.A., Wise T., Zanotti L., Zarra C., Zhang G.Q., Zhu B.X., Zimmermann S., Zucchelli S., Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, and CUORE

Subjects
Cryostat, Nuclear and High Energy Physics, Physics - Instrumentation and Detectors, Physics::Instrumentation and Detectors, FOS: Physical sciences, Cryogenic temperatures, Dilution refrigerator, Low temperature calorimeter, Neutrinoless double beta decay, Rare event searches, Ton-scale detector, Cryogenic temperatures, Neutrinoless double beta decay, Dilution refrigerator, Ton-scale detector, Low temperature calorimeter, Rare event searches, cryogenics, CUORE performance, Cryogenics, Rare event searche, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], 7. Clean energy, 01 natural sciences, CUORE, double-beta decay: (0neutrino), Double beta decay, 0103 physical sciences, Cryogenic particle detectors, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], Nuclear Experiment (nucl-ex), Aerospace engineering, 010306 general physics, Nuclear Experiment, activity report, Physics, 010308 nuclear & particles physics, business.industry, Astrophysics::Instrumentation and Methods for Astrophysics, Cryogenic temperature, Instrumentation and Detectors (physics.ins-det), CUORE performance, Semiconductor detector, cryogenics: design, cryogenics, Neutrino, business, performance
Abstract

The past few decades have seen major developments in the design and operation of cryogenic particle detectors. This technology offers an extremely good energy resolution - comparable to semiconductor detectors - and a wide choice of target materials, making low temperature calorimetric detectors ideal for a variety of particle physics applications. Rare event searches have continued to require ever greater exposures, which has driven them to ever larger cryogenic detectors, with the CUORE experiment being the first to reach a tonne-scale, mK-cooled, experimental mass. CUORE, designed to search for neutrinoless double beta decay, has been operational since 2017 at a temperature of about 10 mK. This result has been attained by the use of an unprecedentedly large cryogenic infrastructure called the CUORE cryostat: conceived, designed and commissioned for this purpose. In this article the main characteristics and features of the cryogenic facility developed for the CUORE experiment are highlighted. A brief introduction of the evolution of the field and of the past cryogenic facilities are given. The motivation behind the design and development of the CUORE cryogenic facility is detailed as are the steps taken toward realization, commissioning, and operation of the CUORE cryostat. The major challenges overcome by the collaboration and the solutions implemented throughout the building of the cryogenic facility will be discussed along with the potential improvements for future facilities. The success of CUORE has opened the door to a new generation of large-scale cryogenic facilities in numerous fields of science. Broader implications of the incredible feat achieved by the CUORE collaboration on the future cryogenic facilities in various fields ranging from neutrino and dark matter experiments to quantum computing will be examined., Comment: 45 pages, 14 figures

Published
2022
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22. Multiplexed Superconducting Detectors for a Neutrino Mass Experiment

Author

E. Ferri, B. Alpert, M. Balata, D. T. Becker, D. A. Bennett, M. Borghesi, M. De Gerone, R. Dressler, M. Faverzani, M. Fedkevych, J. Fowler, G. Gallucci, J. D. Gard, F. Gatti, A. Giachero, G. C. Hilton, U. Koester, M. Lusignoli, J. A. B. Mates, E. Maugeri, E. Nisi, A. Nucciotti, G. Pessina, S. Ragazzi, C. D. Reintsema, M. Ribeiro-Gomes, D. R. Schmidt, D. Schumann, D. S. Swetz, J. N. Ullom, L. R. Vale, Ferri, E, Alpert, B, Balata, M, Becker, D, Bennett, D, Borghesi, M, De Gerone, M, Dressler, R, Faverzani, M, Fedkevych, M, Fowler, J, Gallucci, G, Gard, J, Gatti, F, Giachero, A, Hilton, G, Koster, U, Lusignoli, M, Mates, J, Maugeri, E, Nisi, S, Nucciotti, A, Pessina, G, Ragazzi, S, Reintsema, C, Ribeiro Gomes, M, Schmidt, D, Schumann, D, Swetz, D, Ullom, J, and Vale, L

Subjects
Neutrino source, Resonator, Detector, Gold, Electrical and Electronic Engineering, Energy resolution, Condensed Matter Physics, Electronic, Optical and Magnetic Materials, Microwave theory and technique, Sensor
Abstract

One of the major challenges in nowadays particle physics and astrophysics is the determination of the absolute neutrino mass scale. A powerful tool to evaluate the effective neutrino mass is the calorimetric measurement of the energy released in a nuclear decay involving neutrino. In order to reach a sensitivity on the neutrino mass of the order of 1 eV, not only detectors characterized by high performances (i.e. energy and time resolution of eV at keV and 1 s, respectively) are needed but also many detectors working in parallel are required. Microwave frequency readout provide an effective technique to read out large arrays of low temperature detectors allowing to reach a multiplex factor of the order of thousands. This technique is the one used to read out the 1000 Transition Edge Sensors of HOLMES, an experiment that aims at measuring the electron neutrino mass by means of the electron capture (EC) decay of 163Ho with an expected sensitivity of the order of 1 eV. In this contribution we present the characterization of the microwave-multiplexed readout system, and the results obtained with the detectors specifically designed for HOLMES.

Published
2022

23. Machine Learning Techniques for Pile-Up Rejection in Cryogenic Calorimeters

Author

G. Fantini, A. Armatol, E. Armengaud, W. Armstrong, C. Augier, F. T. Avignone, O. Azzolini, A. Barabash, G. Bari, A. Barresi, D. Baudin, F. Bellini, G. Benato, M. Beretta, L. Bergé, M. Biassoni, J. Billard, V. Boldrini, A. Branca, C. Brofferio, C. Bucci, J. Camilleri, S. Capelli, L. Cappelli, L. Cardani, P. Carniti, N. Casali, A. Cazes, E. Celi, C. Chang, M. Chapellier, A. Charrier, D. Chiesa, M. Clemenza, I. Colantoni, F. Collamati, S. Copello, F. Cova, O. Cremonesi, R. J. Creswick, A. Cruciani, A. D’Addabbo, G. D’Imperio, I. Dafinei, F. A. Danevich, M. de Combarieu, M. De Jesus, P. de Marcillac, S. Dell’Oro, S. Di Domizio, V. Dompè, A. Drobizhev, L. Dumoulin, M. Fasoli, M. Faverzani, E. Ferri, F. Ferri, F. Ferroni, E. Figueroa-Feliciano, J. Formaggio, A. Franceschi, C. Fu, S. Fu, B. K. Fujikawa, J. Gascon, A. Giachero, L. Gironi, A. Giuliani, P. Gorla, C. Gotti, P. Gras, M. Gros, T. D. Gutierrez, K. Han, E. V. Hansen, K. M. Heeger, D. L. Helis, H. Z. Huang, R. G. Huang, L. Imbert, J. Johnston, A. Juillard, G. Karapetrov, G. Keppel, H. Khalife, V. V. Kobychev, Yu. G. Kolomensky, S. Konovalov, Y. Liu, P. Loaiza, L. Ma, M. Madhukuttan, F. Mancarella, R. Mariam, L. Marini, S. Marnieros, M. Martinez, R. H. Maruyama, B. Mauri, D. Mayer, Y. Mei, S. Milana, D. Misiak, T. Napolitano, M. Nastasi, X. F. Navick, J. Nikkel, R. Nipoti, S. Nisi, C. Nones, E. B. Norman, V. Novosad, I. Nutini, T. O’Donnell, E. Olivieri, C. Oriol, J. L. Ouellet, S. Pagan, C. Pagliarone, L. Pagnanini, P. Pari, L. Pattavina, B. Paul, M. Pavan, H. Peng, G. Pessina, V. Pettinacci, C. Pira, S. Pirro, D. V. Poda, T. Polakovic, O. G. Polischuk, S. Pozzi, E. Previtali, A. Puiu, A. Ressa, R. Rizzoli, C. Rosenfeld, C. Rusconi, V. Sanglard, J. Scarpaci, B. Schmidt, V. Sharma, V. Shlegel, V. Singh, M. Sisti, D. Speller, P. T. Surukuchi, L. Taffarello, O. Tellier, C. Tomei, V. I. Tretyak, A. Tsymbaliuk, A. Vedda, M. Velazquez, K. J. Vetter, S. L. Wagaarachchi, G. Wang, L. Wang, B. Welliver, J. Wilson, K. Wilson, L. A. Winslow, M. Xue, L. Yan, J. Yang, V. Yefremenko, V. Yumatov, M. M. Zarytskyy, J. Zhang, A. Zolotarova, S. Zucchelli, Fantini, G, Armatol, A, Armengaud, E, Armstrong, W, Augier, C, Avignone, FT, Azzolini, O, Barabash, A, Bari, G, Barresi, A, Baudin, D, Bellini, F, Benato, G, Beretta, M, Berge, 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, Cova, F, Cremonesi, O, Creswick, RJ, Cruciani, A, D'Addabbo, A, D'Imperio, G, Dafinei, I, Danevich, FA, de Combarieu, M, De Jesus, M, de Marcillac, P, Dell'Oro, S, Di Domizio, S, Dompe, V, Drobizhev, A, Dumoulin, L, Fasoli, M, Faverzani, M, Ferri, E, Ferri, F, Ferroni, F, 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, Gutierrez, TD, Han, K, Hansen, EV, Heeger, KM, Helis, DL, Huang, HZ, Huang, RG, Imbert, L, Johnston, J, Juillard, A, Karapetrov, G, Keppel, G, Khalife, H, Kobychev, VV, Kolomensky, YG, Konovalov, S, 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, XF, Nikkel, J, Nipoti, R, Nisi, S, Nones, C, Norman, EB, Novosad, V, Nutini, I, O'Donnell, T, 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, Rizzoli, R, Rosenfeld, C, Rusconi, C, Sanglard, V, Scarpaci, J, Schmidt, B, Sharma, V, Shlegel, V, Singh, V, Sisti, M, Speller, D, Surukuchi, PT, Taffarello, L, Tellier, O, Tomei, C, Tretyak, VI, Tsymbaliuk, A, Vedda, 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, V, Zarytskyy, MM, Zhang, J, Zolotarova, A, Zucchelli, S, Laboratoire de Cryogénie (LC), Service de physique de l'état condensé (SPEC - UMR3680), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS)-Institut Rayonnement Matière de Saclay (IRAMIS), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Avignone, F, Bergé, L, Creswick, R, D’Addabbo, A, D’Imperio, G, Danevich, F, Dell’Oro, S, Domizio, S, Dompè, V, Figueroa-Feliciano, E, Fujikawa, B, Gutierrez, T, Hansen, E, Heeger, K, Helis, D, Huang, H, Huang, R, Kobychev, V, Kolomensky, Y, Maruyama, R, Navick, X, Norman, E, O’Donnell, T, Ouellet, J, Poda, D, Polischuk, O, Surukuchi, P, Tretyak, V, Vetter, K, Wagaarachchi, S, Winslow, L, and Zarytskyy, M

Subjects
neural network, Convolutional neural network, hierarchy, crystal, Cryogenic calorimeters, neutrino, Machine learning, CUPID, calorimeter, [INFO]Computer Science [cs], General Materials Science, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], Neutrinoless double beta decay, neutrinoless, Pile-up, CUORE, background, double-beta decay, Condensed Matter Physics, Atomic and Molecular Physics, and Optics, Gran Sasso, injection, cryogenics, efficiency, mass, readout, Convolutional neural networks, upgrade, Cryogenic calorimeter, performance, Majorana
Abstract

CUORE Upgrade with Particle IDentification (CUPID) is a foreseen ton-scale array of Li2MoO4 (LMO) cryogenic calorimeters with double readout of heat and light signals. Its scientific goal is to fully explore the inverted hierarchy of neutrino masses in the search for neutrinoless double beta decay of 100Mo. Pile-up of standard double beta decay of the candidate isotope is a relevant background. We generate pile-up heat events via injection of Joule heater pulses with a programmable waveform generator in a small array of LMO crystals operated underground in the Laboratori Nazionali del Gran Sasso, Italy. This allows to label pile-up pulses and control both time difference and underlying amplitudes of individual heat pulses in the data. We present the performance of supervised learning classifiers on data and the attained pile-up rejection efficiency.

Published
2022
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24. Detector Array Readout with Traveling Wave Amplifiers

Author

A. Giachero, C. Barone, M. Borghesi, G. Carapella, A. P. Caricato, I. Carusotto, W. Chang, A. Cian, D. Di Gioacchino, E. Enrico, P. Falferi, L. Fasolo, M. Faverzani, E. Ferri, G. Filatrella, C. Gatti, D. Giubertoni, A. Greco, C. Kutlu, A. Leo, C. Ligi, G. Maccarrone, B. Margesin, G. Maruccio, A. Matlashov, C. Mauro, R. Mezzena, A. G. Monteduro, A. Nucciotti, L. Oberto, S. Pagano, V. Pierro, L. Piersanti, M. Rajteri, S. Rizzato, Y. K. Semertzidis, S. Uchaikin, A. Vinante, Giachero, A., Barone, C., Borghesi, M., Carapella, G., Caricato, A. P., Carusotto, I., Chang, W., Cian, A., Di Gioacchino, D., Enrico, E., Falferi, P., Fasolo, L., Faverzani, M., Ferri, E., Filatrella, G., Gatti, C., Giubertoni, D., Greco, A., Kutlu, C., Leo, A., Ligi, C., Maccarrone, G., Margesin, B., Maruccio, Giuseppe, Matlashov, A., Mauro, C., Mezzena, R., Monteduro, A. G., Nucciotti, A., Oberto, L., Pagano, S., Pierro, V., Piersanti, L., Rajteri, M., Rizzato, S., Semertzidis, Y. K., Uchaikin, S., Vinante, A., Giachero, A, Barone, C, Borghesi, M, Carapella, G, Caricato, A, Carusotto, I, Chang, W, Cian, A, Gioacchino, D, Enrico, E, Falferi, P, Fasolo, L, Faverzani, M, Ferri, E, Filatrella, G, Gatti, C, Giubertoni, D, Greco, A, Kutlu, C, Leo, A, Ligi, C, Maccarrone, G, Margesin, B, Maruccio, G, Matlashov, A, Mauro, C, Mezzena, R, Monteduro, A, Nucciotti, A, Oberto, L, Pagano, S, Pierro, V, Piersanti, L, Rajteri, M, Rizzato, S, Semertzidis, Y, Uchaikin, S, and Vinante, A

Subjects
Quantum Physics, Quantum noise, Parametric amplifer, Traveling wave, Detector array read out, Qubits read out, Physics::Instrumentation and Detectors, Condensed Matter - Superconductivity, FOS: Physical sciences, Condensed Matter Physics, Parametric amplifier, Atomic and Molecular Physics, and Optics, Superconductivity (cond-mat.supr-con), General Materials Science, Quantum Physics (quant-ph), FIS/04 - FISICA NUCLEARE E SUBNUCLEARE
Abstract

Reducing noise to the quantum limit over a large bandwidth is a fundamental requirement for future applications operating at millikelvin temperatures, such as the neutrino mass measurement, the next-generation X-ray observatory, the CMB measurement, the dark matter and axion detection, and the rapid high-fidelity readout of superconducting qubits. The read out sensitivity of arrays of microcalorimeter detectors, resonant axion-detectors, and qubits, is currently limited by the noise temperature and bandwidth of the cryogenic amplifiers. The Detector Array Readout with Traveling Wave Amplifiers project has the goal of developing high-performing innovative traveling wave parametric amplifiers with a high gain, a high saturation power, and a quantum-limited or nearly quantum-limited noise. The practical development follows two different promising approaches, one based on the Josephson junctions and the other one based on the kinetic inductance of a high-resistivity superconductor. In this contribution, we present the aims of the project, the adopted design solutions and preliminary results from simulations and measurements.

Published
2022

25. A Thermal Model for Low Temperature TeO 2 Calorimeters

Author

S. Quitadamo, C. Brofferio, M. Faverzani, M. Biassoni, G. Pessina, Evelyn Ferri, Irene Nutini, Paolo Carniti, C. Gotti, A. Giachero, S. Ghislandi, Biassoni, M, Brofferio, C, Carniti, P, Faverzani, M, Ferri, E, Ghislandi, S, Giachero, A, Gotti, C, Nutini, I, Pessina, G, and Quitadamo, S

Subjects
Bolometer response function, NTD, Materials science, Low-temperature calorimeter, Thermodynamics, General Materials Science, Thermal model, Neutrinoless double beta decay, Condensed Matter Physics, Atomic and Molecular Physics, and Optics
Abstract

In this paper, we present the application of a simplified thermal model in order to extract some of the fundamental parameters needed to understand the response function of low-temperature calorimeters consisting of TeO 2 crystals read-out by neutron transmutation doped (NTD) thermistors operated at temperatures T∼ 10 mK. To this aim, four detectors were hosted in two different holders, one made of copper and the other made of Stratasys VeroClear TM, a 3D-printed plastic material very similar to acrylic. The static characterization of the detectors through the analysis of their load curves at different temperatures, guided by the thermal model, enabled the identification of the main thermal link to the heat sink of the two systems: the glue between the crystal and the copper frame (scaling as T3) for the detectors in the copper holder, and the NTD gold read-out wires (scaling as T2.5) for the detectors in the plastic holder. As a subdominant contribution, we could also extract the electron–phonon decoupling characteristic of our NTDs, described by a thermal conductance scaling as T4.

Published
2022

26. Ultra low noise readout with traveling wave parametric amplifiers: The DARTWARS project

Author

A. Rettaroli, C. Barone, M. Borghesi, S. Capelli, G. Carapella, A.P. Caricato, I. Carusotto, A. Cian, D. Di Gioacchino, E. Enrico, P. Falferi, L. Fasolo, M. Faverzani, E. Ferri, G. Filatrella, C. Gatti, A. Giachero, D. Giubertoni, V. Granata, A. Greco, C. Guarcello, D. Labranca, A. Leo, C. Ligi, G. Maccarrone, F. Mantegazzini, B. Margesin, G. Maruccio, C. Mauro, R. Mezzena, A.G. Monteduro, A. Nucciotti, L. Oberto, L. Origo, S. Pagano, V. Pierro, L. Piersanti, M. Rajteri, S. Rizzato, A. Vinante, M. Zannoni, Rettaroli, A, Barone, C, Borghesi, M, Capelli, S, Carapella, G, Caricato, A, Carusotto, I, Cian, A, Di Gioacchino, D, Enrico, E, Falferi, P, Fasolo, L, Faverzani, M, Ferri, E, Filatrella, G, Gatti, C, Giachero, A, Giubertoni, D, Granata, V, Greco, A, Guarcello, C, Labranca, D, Leo, A, Ligi, C, Maccarrone, G, Mantegazzini, F, Margesin, B, Maruccio, G, Mauro, C, Mezzena, R, Monteduro, A, Nucciotti, A, Oberto, L, Origo, L, Pagano, S, Pierro, V, Piersanti, L, Rajteri, M, Rizzato, S, Vinante, A, and Zannoni, M

Subjects
Quantum Physics, Nuclear and High Energy Physics, Josephson junctions, Microwaves, Low noise, Parametric amplification, Detector arrays, Superconductors, FOS: Physical sciences, Detector array, Josephson junction, Superconductor, Quantum Physics (quant-ph), Microwave, Instrumentation
Abstract

The DARTWARS project has the goal of developing high-performing innovative travelling wave parametric amplifiers with high gain, large bandwidth, high saturation power, and nearly quantum-limited noise. The target frequency region for its applications is 5 - 10 GHz, with an expected noise temperature of about 600 mK. The development follows two different approaches, one based on Josephson junctions and one based on kinetic inductance of superconductors. This contribution mainly focuses on the Josephson travelling wave parametric amplifier, presenting its design, preliminary measurements and the test of homogeneity of arrays of Josephson junctions., 4 pages, 5 figures. Proceeding of Pisa15th Meeting conference. arXiv admin note: text overlap with arXiv:2111.03409

Published
2023
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27. Optimization of a single module of CUPID

Author

Alberto Ressa, A. Armatol, E. Armengaud, W. Armstrong, C. Augier, F. T. Avignone, O. Azzolini, A. Barabash, G. Bari, A. Barresi, D. Baudin, F. Bellini, G. Benato, M. Beretta, L. Bergé, M. Biassoni, J. Billard, V. Boldrini, A. Branca, C. Brofferio, C. Bucci, J. Camilleri, S. Capelli, L. Cappelli, L. Cardani, P. Carniti, N. Casali, A. Cazes, E. Celi, A. Chang, M. Chapellier, A. Charrier, D. Chiesa, M. Clemenza, I. Colantoni, F. Collamati, S. Copello, O. Cremonesi, R. J. Creswick, A. Cruciani, A. D’ Addabbo, G. D’ Imperio, I. Dafinei, F. A. Danevich, M. de Combarieu, M. De Jesus, P. de Marcillac, S. Dell’Oro, S. Di Domizio, V. Dompè, A. Drobizhev, L. Dumoulin, G. Fantini, M. Faverzani, E. Ferri, F. Ferri, F. Ferroni, E. Figueroa-Feliciano, J. Formaggio, A. Franceschi, C. Fu, S. Fu, B. K. Fujikawa, J. Gascon, A. Giachero, L. Gironi, A. Giuliani, P. Gorla, C. Gotti, P. Gras, M. Gros, T. D. Gutierrez, K. Han, E. V. Hansen, K. M. Heeger, B. L. Helis, H.Z. Huang, R. G. Huang, L. Imbert, J. Johnston, A. Juillard, G. Karapetrov, G. Keppel, H. Khalife, V. V. Kobychev, Yu. G. Kolomensky, S. Konovalov, Y. Liu, P. Loaiza, L. Ma, M. Madhukuttan, F. Mancarella, R. Mariam, L. Marini, S. Marnieros, M. Martinez, R. H. Maruyama, B. Mauri, D. Mayer, Y. Mei, S. Milana, D. Misiak, T. Napolitano, M. Nastasi, X. F. Navick, J. Nikkel, R. Nipoti, S. Nisi, C. Nones, C. B. Norman, V. Novosad, I. Nutini, T. O’Donnell, E. Olivieri, C. Oriol, J. L. Ouellet, S. Pagan, C. Pagliarone, L. Pagnanini, P. Pari, L. Pattavina, B. Paul, M. Pavan, H. Peng, G. Pessina, V. Pettinacci, C. Pira, S. Pirro, D. V. Poda, T. Polakovic, O. G. Polischuk, S. Pozzi, E. Previtali, A. Puiu, A. Ressa, R. Rizzoli, C. Rosenfeld, C. Rusconi, V. Sanglard, J. Scarpaci, B. Schmidt, V. Sharma, V. Shlegel, V. Singh, M. Sisti, D. Speller, P. T. Surukuchi, L. Taffarello, O. Tellier, C. Tomei, V. I. Tretyak, A. Tsymbaliuk, M. Velazquez, K. J. Vetter, S. L. Wagaarachchi, G. Wang, L. Wang, B. Welliver, J. Wilson, K. Wilson, L. A. Winslow, M. Xue, L. Yan, J. Yang, V. Yefremenko, V. Yumatov, M. M. Zarytskyy, J. Zhang, A. Zolotarova, S. Zucchelli, Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Science et Ingénierie des Matériaux et Procédés (SIMaP), Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), and CUPID

Subjects
photon yield, History, tector design, helium background, energy resolution, lithium, molybdenum nuclide, molybdenum oxygen, scintillation counter, crystal bolometer, CUORE performance, photon yield, Physics::Instrumentation and Detectors, Astrophysics::Instrumentation and Methods for Astrophysics, energy resolution, helium background, molybdenum oxygen, CUORE performance, Computer Science Applications, Education, Gran Sasso, double-beta decay: (0neutrino), lithium, crystal bolometer, molybdenum nuclide, calorimeter: cryogenics, High Energy Physics::Experiment, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], activity report, scintillation counter, detector: design, performance, tector design
Abstract

CUPID is the next generation experiment which will use scintillating cryogenic calorimeters to search for the neutrinoless double β decay. This unobserved process would shed light on the nature of the neutrino, which up to our knowledge could be a Majorana or a Dirac particle, and would give us an important hint to explain the lack of antimatter in the universe. This ambitious search needs a detector with unique characteristics such as an extremely low background level and an excellent energy resolution. CUPID is now in advanced R&D state to optimize the detector design in order to completely exploit the potentialities of scintillating cryogenic calorimeters. In the following I will describe the test performed at the LNGS (Laboratori Nazionali del Gran Sasso) of a single module of the future CUPID detector. In this contribution we present the performance obtained with a novel assembly concept, proving that it matches the requirements for CUPID.

Published
2021
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28. Expected sensitivity to $^{128}$Te neutrinoless double beta decay with the CUORE TeO$_2$ cryogenic bolometers

Author

V. Dompè, D. Q. Adams, C. Alduino, K. Alfonso, F. T. Avignone, O. Azzolini, G. Bari, F. Bellini, G. Benato, M. Beretta, M. Biassoni, A. Branca, C. Brofferio, C. Bucci, J. Camilleri, A. Caminata, A. Campani, L. Canonica, X. G. Cao, S. Capelli, L. Cappelli, L. Cardani, P. Carniti, N. Casali, E. Celi, D. Chiesa, M. Clemenza, S. Copello, O. Cremonesi, R. J. Creswick, A. D’Addabbo, I. Dafinei, S. Dell’Oro, S. Di Domizio, S. Di Lorenzo, D. Q. Fang, G. Fantini, M. Faverzani, E. Ferri, F. Ferroni, E. Fiorini, M. A. Franceschi, S. J. Freedman, S. H. Fu, B. K. Fujikawa, S. Ghislandi, A. Giachero, L. Gironi, A. Giuliani, P. Gorla, C. Gotti, T. D. Gutierrez, K. Han, E. V. Hansen, K. M. Heeger, R. G. Huang, H. Z. Huang, J. Johnston, G. Keppel, Yu G. Kolomensky, R. Kowalski, C. Ligi, R. Liu, L. Ma, Y. G. Ma, L. Marini, R. H. Maruyama, D. Mayer, Y. Mei, N. Moggi, S. Morganti, T. Napolitano, M. Nastasi, J. Nikkel, C. Nones, E. B. Norman, A. Nucciotti, I. Nutini, T. O’Donnell, M. Olmi, J. L. Ouellet, S. Pagan, C. E. Pagliarone, L. Pagnanini, M. Pallavicini, L. Pattavina, M. Pavan, G. Pessina, V. Pettinacci, C. Pira, S. Pirro, S. Pozzi, E. Previtali, A. Puiu, S. Quitadamo, A. Ressa, C. Rosenfeld, C. Rusconi, M. Sakai, S. Sangiorgio, B. Schmidt, N. D. Scielzo, V. Sharma, V. Singh, M. Sisti, D. Speller, P. T. Surukuchi, L. Taffarello, F. Terranova, C. Tomei, K. J. Vetter, M. Vignati, S. L. Wagaarachchi, B. S. Wang, B. Welliver, J. Wilson, K. Wilson, L. A. Winslow, S. Zimmermann, S. Zucchelli, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Dompe, V, Adams, D, Alduino, C, Alfonso, K, Avignone, F, Azzolini, O, Bari, G, Bellini, F, Benato, G, Beretta, M, Biassoni, M, Branca, A, Brofferio, C, Bucci, C, Camilleri, J, Caminata, A, Campani, A, Canonica, L, Cao, X, Capelli, S, Cappelli, L, Cardani, L, Carniti, P, Casali, N, Celi, E, Chiesa, D, Clemenza, M, Copello, S, Cremonesi, O, Creswick, R, D'Addabbo, A, Dafinei, I, Dell'Oro, S, Di Domizio, S, Di Lorenzo, S, Fang, D, Fantini, G, Faverzani, M, Ferri, E, Ferroni, F, Fiorini, E, Franceschi, M, Freedman, S, Fu, S, Fujikawa, B, Ghislandi, S, Giachero, A, Gironi, L, Giuliani, A, Gorla, P, Gotti, C, Gutierrez, T, Han, K, Hansen, E, Heeger, K, Huang, R, Huang, H, Johnston, J, Keppel, G, Kolomensky, Y, Kowalski, R, Ligi, C, Liu, R, Ma, L, Ma, Y, Marini, L, Maruyama, R, Mayer, D, Mei, Y, Moggi, N, Morganti, S, Napolitano, T, Nastasi, M, Nikkel, J, Nones, C, Norman, E, Nucciotti, A, Nutini, I, O'Donnell, T, Olmi, M, Ouellet, J, Pagan, S, Pagliarone, C, Pagnanini, L, Pallavicini, M, Pattavina, L, Pavan, M, Pessina, G, Pettinacci, V, Pira, C, Pirro, S, Pozzi, S, Previtali, E, Puiu, A, Quitadamo, S, Ressa, A, Rosenfeld, C, Rusconi, C, Sakai, M, Sangiorgio, S, Schmidt, B, Scielzo, N, Sharma, V, Singh, V, Sisti, M, Speller, D, Surukuchi, P, Taffarello, L, Terranova, F, Tomei, C, Vetter, K, Vignati, M, Wagaarachchi, S, Wang, B, Welliver, B, Wilson, J, Wilson, K, Winslow, L, Zimmermann, S, Zucchelli, S, Adams, DQ, Avignone, FT, Cao, XG, Creswick, RJ, Fang, DQ, Franceschi, MA, Freedman, SJ, Fu, SH, Fujikawa, BK, Gutierrez, TD, Hansen, EV, Heeger, KM, Huang, RG, Huang, HZ, Kolomensky, YG, Ma, YG, Maruyama, RH, Norman, EB, Ouellet, JL, Pagliarone, CE, Scielzo, ND, Surukuchi, PT, Vetter, KJ, Wagaarachchi, SL, Wang, BS, and Winslow, LA

Subjects
CUORE, Physics::Instrumentation and Detectors, Astrophysics::Instrumentation and Methods for Astrophysics, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], Condensed Matter Physics, Cryogenic bolometer, Atomic and Molecular Physics, and Optics, CUORE, Cryogenic Bolometers, Cryogenic bolometers, General Materials Science, High Energy Physics::Experiment, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], Neutrinoless double beta decay, Tellurium, Nuclear Experiment, 128-Te
Abstract

The CUORE experiment is a ton-scale array of $$\hbox {TeO}_2$$ TeO 2 cryogenic bolometers located at the underground Laboratori Nazionali del Gran Sasso of Istituto Nazionale di Fisica Nucleare (INFN), in Italy. The CUORE detector consists of 988 crystals operated as source and detector at a base temperature of $$\sim 10$$ ∼ 10 mK. Such cryogenic temperature is reached and maintained by means of a custom built cryogen-free dilution cryostat, designed with the aim of minimizing the vibrational noise and the environmental radioactivity. The primary goal of CUORE is the search for neutrinoless double beta decay of $$^{130}\hbox {Te}$$ 130 Te , but thanks to its large target mass and ultra-low background it is suitable for the study of other rare processes as well, such as the neutrinoless double beta decay of $$^{128}\hbox {Te}$$ 128 Te . This tellurium isotope is an attractive candidate for the search of this process, due to its high natural isotopic abundance of 31.75%. The transition energy at (866.7 ± 0.7) keV lies in a highly populated region of the energy spectrum, dominated by the contribution of the two-neutrino double beta decay of $$^{130}\hbox {Te}$$ 130 Te . As the first ton-scale infrastructure operating cryogenic $$\hbox {TeO}_2$$ TeO 2 bolometers in stable conditions, CUORE is able to achieve a factor $$>10$$ > 10 higher sensitivity to the neutrinoless double beta decay of this isotope with respect to past direct experiments.

Published
2021
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29. Development of Microwave Kinetic Inductance Detectors for IR Single-Photon Counting

Author

Evelyn Ferri, Andrea Vinante, A. Nucciotti, M. Faverzani, Benno Margesin, Andrea Giachero, A. Puiu, Renato Mezzena, Mezzena, R, Faverzani, M, Ferri, E, Giachero, A, Margesin, B, Nucciotti, A, Puiu, A, and Vinante, A

Subjects
Materials science, Microwave kinetic inductance detector, chemistry.chemical_element, 01 natural sciences, Kinetic inductance, 010305 fluids & plasmas, law.invention, Resonator, law, 0103 physical sciences, General Materials Science, Ti/TiN multilayer films, 010306 general physics, Laser diode, business.industry, Microwave kinetic inductance detectors, Detector, Condensed Matter Physics, Atomic and Molecular Physics, and Optics, Photon counting, Single-photon detector, Capacitor, chemistry, Optoelectronics, business, Tin, Microwave
Abstract

We have developed microwave kinetic inductance detectors suitable for near-IR single-photon counting. Our films are made of titanium and titanium nitride, deposited in a multilayer structure Ti/TiN/Ti/TiN with a total thickness of 44nm. The film has a transition temperature of 1.2K and a surface kinetic inductance of 34pH/sq. The resonator was designed with lumped elements and consists of two blocks of interdigitated capacitors connected by a meandered stripe inductor. The resonator resonance frequency is 6.8GHz, and the internal quality factor is 125,000. The detector is read out with the usual homodyne scheme and calibrated with light pulses produced by a laser diode with wavelength 1550nm. For the 0- and 1-photon peaks, we measure a FWHM energy resolution of 0.44eV and 0.56eV, respectively. This resolution is sufficient to resolve events with up to 4 photons.

Published
2019
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30. A design for an electromagnetic filter for precision energy measurements at the tritium endpoint

Author

C. L. Chang, A. Molinero-Vela, A. Nucciotti, M. Messina, Emanuele Ferri, C. Pérez de los Heros, R. Santorelli, A. D. Ferella, Kathryn M. Zurek, Jorge Pedrós, Yevgeny Raitses, Sergio Pastor, A. Puiu, Carlo Mancini-Terracciano, Jan Conrad, Christopher George Tully, Nicola D'Ambrosio, Fang Zhao, J. Carabe-Lopez, Auke-Pieter Colijn, Mariangela Lisanti, Michele Biasotti, N. Rossi, C. Gentile, C. F. Strid, G. Cavoto, Carlo Mariani, E. Monticone, W. Chung, K. Schaeffner, A. Boscá, L. E. Marcucci, M. Rajteri, Francesco Pandolfi, Andrea Giachero, Ofelia Pisanti, S. Gariazzo, P. Garcia-Abia, G. Garcia Gomez-Tejedor, Jon E. Gudmundsson, Antonio D. Polosa, Gianpiero Mangano, A. G. Cocco, Yonit Hochberg, Javier Martínez, P. F. de Salas, M. Faverzani, Fernando Calle, Flavio Gatti, Maria Grazia Betti, Yonatan Kahn, Betti, M, Biasotti, M, Boscá, A, Calle, F, Carabe-Lopez, J, Cavoto, G, Chang, C, Chung, W, Cocco, A, Colijn, A, Conrad, J, D’Ambrosio, N, de Salas, P, Faverzani, M, Ferella, A, Ferri, E, Garcia-Abia, P, Gomez-Tejedor, G, Gariazzo, S, Gatti, F, Gentile, C, Giachero, A, Gudmundsson, J, Hochberg, Y, Kahn, Y, Lisanti, M, Mancini-Terracciano, C, Mangano, G, Marcucci, L, Mariani, C, Martínez, J, Messina, M, Molinero-Vela, A, Monticone, E, Nucciotti, A, Pandolfi, F, Pastor, S, Pedrós, J, de los Heros, C, Pisanti, O, Polosa, A, Puiu, A, Raitses, Y, Rajteri, M, Rossi, N, Santorelli, R, Schaeffner, K, Strid, C, Tully, C, Zhao, F, Zurek, K, Simons Foundation, John Templeton Foundation, Betti, M. G., Biasotti, M., Bosca, A., Calle, F., Carabe-Lopez, J., Cavoto, G., Chang, C., Chung, W., Cocco, A. G., Colijn, A. P., Conrad, J., D'Ambrosio, N., de Salas, P. F., Faverzani, M., Ferella, A., Ferri, E., Garcia-Abia, P., Gomez-Tejedor, G. G., Gariazzo, S., Gatti, F., Gentile, C., Giachero, A., Gudmundsson, J. E., Hochberg, Y., Kahn, Y., Lisanti, M., Mancini-Terracciano, C., Mangano, G., Marcucci, L. E., Mariani, C., MARTINEZ DE AGUIRRE, JAVIER MIGUEL, Messina, M., Molinero-Vela, A., Monticone, E., Nucciotti, A., Pandolfi, F., Pastor, S., Pedros, J., de los Heros, C. P., Pisanti, O., Polosa, A. D., Puiu, A., Raitses, Y., Rajteri, M., Rossi, N., Santorelli, R., Schaeffner, K., Strid, C. F., Tully, C. G., Zhao, Pengfei, and Zurek, K. M.

Subjects
Nuclear and High Energy Physics, Physics - Instrumentation and Detectors, FOS: Physical sciences, Electron, 7. Clean energy, 01 natural sciences, Partícules (Física nuclear), Hamiltonian system, Neutrino mass, Relic neutrino, 0103 physical sciences, Transverse drift filter, 010306 general physics, Instrumentation and Methods for Astrophysics (astro-ph.IM), PTOLEMY, Physics, Magnetic moment, 010308 nuclear & particles physics, CNB, Cosmic Neutrino Background, Instrumentation and Detectors (physics.ins-det), Filter (signal processing), Computational physics, Energy conservation, Harmonic, Astrophysics - Instrumentation and Methods for Astrophysics, Neutrino ma, Energy (signal processing), Voltage
Abstract

We present a detailed description of the electromagnetic filter for the PTOLEMY project to directly detect the Cosmic Neutrino Background (CNB). Starting with an initial estimate for the orbital magnetic moment, the higher-order drift process of E×B is configured to balance the gradient-B drift motion of the electron in such a way as to guide the trajectory into the standing voltage potential along the mid-plane of the filter. As a function of drift distance along the length of the filter, the filter zooms in with exponentially increasing precision on the transverse velocity component of the electron kinetic energy. This yields a linear dimension for the total filter length that is exceptionally compact compared to previous techniques for electromagnetic filtering. The parallel velocity component of the electron kinetic energy oscillates in an electrostatic harmonic trap as the electron drifts along the length of the filter. An analysis of the phase-space volume conservation validates the expected behavior of the filter from the adiabatic invariance of the orbital magnetic moment and energy conservation following Liouville's theorem for Hamiltonian systems., CGT is supported by the Simons Foundation (#377485) and John Templeton Foundation (#58851)

Published
2019
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31. A novel approach for nearly-coincident events rejection

Author

A. Nucciotti, G. Gallucci, M. Borghesi, M. De Gerone, Andrea Giachero, A. Puiu, Emanuele Ferri, M. Fedkevych, M. Faverzani, Borghesi, M, De Gerone, M, Faverzani, M, Fedkevych, M, Ferri, E, Gallucci, G, Giachero, A, Nucciotti, A, and Puiu, A

Subjects
Physics - Instrumentation and Detectors, Physics and Astronomy (miscellaneous), Statistical sensitivity, FOS: Physical sciences, Effective time, QC770-798, Astrophysics, 01 natural sciences, Coincident, Nuclear and particle physics. Atomic energy. Radioactivity, 0103 physical sciences, Limit (mathematics), Nuclear Experiment (nucl-ex), 010306 general physics, Spurious relationship, Nuclear Experiment, Engineering (miscellaneous), Physics, 010308 nuclear & particles physics, Time resolution, Instrumentation and Detectors (physics.ins-det), Resolution (logic), QB460-466, Neutrino mass, time resolution, holmium, Neutrino, Algorithm
Abstract

We present a novel technique, called DSVP (Discrimination through Singular Vectors Projections), to discriminate spurious events within a dataset. The purpose of this paper is to lay down a general procedure which can be tailored for a broad variety of applications. After describing the general concept, we apply the algorithm to the problem of identifying nearly coincident events in low temperature microcalorimeters in order to push the time resolution close to its intrinsic limit. In fact, from simulated datasets it was possible to achieve an effective time resolution even shorter than the sampling time of the system considered. The obtained results are contextualized in the framework of the HOLMES experiment, which aims at directly measuring the neutrino mass with the calorimetric approach, allowing to significally improve its statistical sensitivity.

Published
2021
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32. Measurement of the 2νββ Decay Half-Life of Te130 with CUORE

Author

V. Sharma, D. Speller, Deqing Fang, S. Morganti, J. Nikkel, S. H. Fu, P. T. Surukuchi, S. Zimmermann, Carlo Ligi, R. J. Creswick, A. Campani, L. Gironi, I. Nutini, C. Rosenfeld, J. Camilleri, Oliviero Cremonesi, Kai Vetter, P. Gorla, F. Ferroni, C. Tomei, Massimiliano Clemenza, Carlo Cosmelli, Monica Sisti, F. T. Avignone, B. S. Wang, A. Giuliani, Emanuele Ferri, C. Pagliarone, N. D. Scielzo, C. Brofferio, L. Pattavina, C. J. Davis, Silvia Capelli, S. Pozzi, F. Terranova, C. Nones, A. Puiu, Massimiliano Nastasi, S. Di Domizio, K. Wilson, Davide Chiesa, Lucia Canonica, A. Caminata, Ezio Previtali, Marco Pallavicini, C. Rusconi, B. Welliver, V. Dompè, F. Bellini, Jonathan Ouellet, G. Bari, H. Z. Huang, S. Pagan, Y. Mei, A. D'Addabbo, C. Bucci, L. Marini, T. D. Gutierrez, T. O'Donnell, J. Johnston, S. Copello, N. Moggi, Laura Cardani, Yu. G. Kolomensky, Luigi Cappelli, B. K. Fujikawa, Xiangyu Cao, G. Keppel, Samuele Sangiorgio, K. M. Heeger, A. Nucciotti, C. Alduino, S. Pirro, B. Schmidt, Stefano Zucchelli, S. Dell'Oro, Ke Han, Paolo Carniti, Reina H. Maruyama, Claudio Gotti, Stuart J. Freedman, M. Sakai, O. Azzolini, T. Napolitano, M. Pavan, N. Casali, James R. Wilson, G. Pessina, S. L. Wagaarachchi, V. Pettinacci, M. Vignati, M. Biassoni, I. Dafinei, E. Fiorini, Giovanni Benato, Yudi Ma, L. Pagnanini, Eric B. Norman, L. Taffarello, D. Q. Adams, K. Alfonso, D. Mayer, M. Faverzani, Lindley Winslow, Virendra Singh, L. Ma, C. Pira, G. Fantini, R. G. Huang, A. Branca, M. A. Franceschi, and A. Giachero

Subjects
Physics, Nuclear physics, CUORE, Double beta decay, 0103 physical sciences, General Physics and Astronomy, Half-life, High Energy Physics::Experiment, 010306 general physics, 01 natural sciences, Spectral line
Abstract

We measured two-neutrino double beta decay of $^{130}$Te using an exposure of 300.7 kg$\cdot$yr accumulated with the CUORE detector. Using a Bayesian analysis to fit simulated spectra to experimental data, it was possible to disentangle all the major background sources and precisely measure the two-neutrino contribution. The half-life is in agreement with past measurements with a strongly reduced uncertainty: $T^{2\nu}_{1/2} = 7.71^{+0.08}_{-0.06}\mathrm{(stat.)}^{+0.12}_{-0.15}\mathrm{(syst.)}\times10^{20}$ yr. This measurement is the most precise determination of the $^{130}$Te 2$\nu\beta\beta$ decay half-life to date.

Published
2021
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33. Search for Double-Beta Decay of $\mathrm{^{130}Te}$ to the $0^+$ States of $\mathrm{^{130}Xe}$ with CUORE

Author

Davide Chiesa, S. Di Domizio, Laura Cardani, B. K. Fujikawa, Stefano Pozzi, M. Vignati, Massimiliano Clemenza, Carlo Cosmelli, A. Giuliani, Monica Sisti, C. Pagliarone, V. Sharma, S. Zimmermann, A. Branca, Deqing Fang, S. Dell'Oro, B. Schmidt, L. Pattavina, L. Pagnanini, B. S. Wang, C. Brofferio, Marco Pallavicini, Lindley Winslow, F. Terranova, S. Morganti, O. Azzolini, S. Copello, S. Pagan, Kai Vetter, G. Pessina, Paolo Carniti, C. Rusconi, Carlo Ligi, L. Taffarello, L. Ma, Virendra Singh, Yudi Ma, H. Z. Huang, C. Rosenfeld, S. Pirro, A. Campani, C. Pira, Ettore Fiorini, S. L. Wagaarachchi, Andrea Giachero, P. Gorla, F. Ferroni, J. Camilleri, Xiangyu Cao, C. Tomei, Ke Han, Reina H. Maruyama, Stuart J. Freedman, L. Canonica, L. Marini, D. Q. Adams, Simone Capelli, K. Alfonso, G. Keppel, D. Speller, D. Mayer, C. J. Davis, Y. Mei, C. Nones, A. Puiu, I. Dafinei, Irene Nutini, J. Johnston, V. Pettinacci, A. Caminata, V. Dompè, A. D'Addabbo, J. Nikkel, G. Fantini, K. M. Heeger, Ezio Previtali, P. T. Surukuchi, T. O'Donnell, Yu. G. Kolomensky, N. D. Scielzo, R. G. Huang, B. Welliver, K. Wilson, Jonathan Ouellet, G. Bari, E. Celi, M. A. Franceschi, S. Zucchelli, M. Faverzani, Evelyn Ferri, N. Moggi, Eric B. Norman, L. Cappelli, M. Sakai, T. Napolitano, Samuele Sangiorgio, Oliviero Cremonesi, A. Nucciotti, M. Biassoni, C. Alduino, Claudio Gotti, N. Casali, Giovanni Benato, C. Bucci, T. D. Gutierrez, L. Gironi, F. T. Avignone, F. Bellini, R. J. Creswick, M. Pavan, Massimiliano Nastasi, James R. Wilson, S. H. Fu, Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Département de Physique des Particules (ex SPP) (DPP), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, CUORE, and Département de Physique des Particules (ex SPP) (DPhP)

Subjects
Particle physics, experimental methods, Physics and Astronomy (miscellaneous), FOS: Physical sciences, Dirac Neutrino, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], Neutrinoless Double Beta Decay, 7. Clean energy, 01 natural sciences, Bayesian, decay modes, crystal, CUORE, background: low, bolometer, Double beta decay, Neutrino, 0103 physical sciences, excited state, double-beta decay: (2neutrino), Beta (velocity), Sensitivity (control systems), bayesian analysis, Nuclear Experiment (nucl-ex), Particle Physics, 010306 general physics, Engineering (miscellaneous), Nuclear Experiment, lepton number: violation, excited states, Physics, 010308 nuclear & particles physics, Majorana Neutrino, Gamma ray, sensitivity, Lepton number, gamma ray: emission, Excited state, Double beta decay, excited states, bayesian analysis, CUORE, Neutrinoless Double Beta Decay, Particle Physics, Neutrino, Majorana Neutrino, Dirac Neutrino
Abstract

The CUORE experiment is a large bolometric array searching for the lepton number violating neutrino-less double beta decay ($0\nu\beta\beta$) in the isotope $\mathrm{^{130}Te}$. In this work we present the latest results on two searches for the double beta decay (DBD) of $\mathrm{^{130}Te}$ to the first $0^{+}_2$ excited state of $\mathrm{^{130}Xe}$: the $0\nu\beta\beta$ decay and the Standard Model-allowed two-neutrinos double beta decay ($2\nu\beta\beta$). Both searches are based on a 372.5 kg$\times$yr TeO$_2$ exposure. The de-excitation gamma rays emitted by the excited Xe nucleus in the final state yield a unique signature, which can be searched for with low background by studying coincident events in two or more bolometers. The closely packed arrangement of the CUORE crystals constitutes a significant advantage in this regard. The median limit setting sensitivities at 90\% Credible Interval (C.I.) of the given searches were estimated as $\mathrm{S^{0\nu}_{1/2} = 5.6 \times 10^{24} \: \mathrm{yr}}$ for the ${0\nu\beta\beta}$ decay and $\mathrm{S^{2\nu}_{1/2} = 2.1 \times 10^{24} \: \mathrm{yr}}$ for the ${2\nu\beta\beta}$ decay. No significant evidence for either of the decay modes was observed and a Bayesian lower bound at $90\%$ C.I. on the decay half lives is obtained as: $\mathrm{(T_{1/2})^{0\nu}_{0^+_2} > 5.9 \times 10^{24} \: \mathrm{yr}}$ for the $0\nu\beta\beta$ mode and $\mathrm{(T_{1/2})^{2\nu}_{0^+_2} > 1.3 \times 10^{24} \: \mathrm{yr}}$ for the $2\nu\beta\beta$ mode. These represent the most stringent limits on the DBD of $^{130}$Te to excited states and improve by a factor $\sim5$ the previous results on this process., Comment: 13 pages, 6 figures

Published
2021
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34. Progress in the development of TES microcalorimeter detectors suitable for neutrino mass measurement

Author

Dan Becker, Daniel S. Swetz, A. Nucciotti, Gene C. Hilton, M. De Gerone, Bradley K. Alpert, Andrea Giachero, Flavio Gatti, A. Puiu, G. Gallucci, Leila R. Vale, Johnathon D. Gard, G. Pessina, Joel N. Ullom, M. Borghesi, Douglas A. Bennett, Carl D. Reintsema, M. Fedkevych, D. R. Schmidt, M. Faverzani, John A. B. Mates, Emanuele Ferri, Giachero, A, Alpert, B, Becker, D, Bennett, D, Borghesi, M, De Gerone, M, Faverzani, M, Fedkevych, M, Ferri, E, Gallucci, G, Gard, J, Gatti, F, Hilton, G, Mates, J, Nucciotti, A, Pessina, G, Puiu, A, Reintsema, C, Schmidt, D, Swetz, D, Ullom, J, and Vale, L

Subjects
radiation detector, X-ray detector, Physics - Instrumentation and Detectors, Electron capture, Physics::Instrumentation and Detectors, superconducting microwave device, FOS: Physical sciences, superconducting microwave devices, SQUID, Elementary particle, 01 natural sciences, Multiplexing, Noise (electronics), Optics, radiation detectors, 0103 physical sciences, Electrical and Electronic Engineering, 010306 general physics, Physics, Pixel, business.industry, Bandwidth (signal processing), Detector, Elementary particles, X-ray detectors, Instrumentation and Detectors (physics.ins-det), Condensed Matter Physics, Electronic, Optical and Magnetic Materials, Neutrino, business, Microwave
Abstract

The HOLMES experiment will perform a precise calorimetric measurement of the end point of the Electron Capture (EC) decay spectrum of 163Ho in order to extract information on neutrino mass with a sensitivity below 2 eV. In its final configuration, HOLMES will deploy 1000 detectors of low-temperature microcalorimeters with implanted 163Ho nuclei. The baseline sensors for HOLMES are Mo/Cu TESs (Transition Edge Sensors) on SiNx membrane with gold absorbers. Considering the large number of pixels and an event rate of about 300 Hz/pixel, a large multiplexing factor and a large bandwidth are needed. To fulfill this requirement, HOLMES will exploit recent advances in microwave multiplexing. In this contribution, we present the status of the activities in development, the performances of the developed microwave-multiplexed readout system, and the results obtained with the detectors specifically designed for HOLMES in terms of noise, time, and energy resolutions

Published
2021
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35. Characterization of cubic Li 2100 MoO 4 crystals for the CUPID experiment

Author

Federico Ferri, Stefano Dell'Oro, J. Camilleri, V. Shlegel, N. Casali, R. Rizzoli, F. Bellini, A. Ressa, J. A. Scarpaci, C. Augier, Goran Karapetrov, G. Fantini, P. Gras, M. I. Martínez, F.A. Danevich, L. Pagnanini, P. T. Surukuchi, A. Drobizhev, S. H. Fu, C. Oriol, I. Dafinei, T. O'Donnell, E. Figueroa-Feliciano, P. Loaiza, Jie Yang, S. Copello, Haiping Peng, Oliviero Cremonesi, L. Wang, A. Franceschi, C. Pagliarone, Davide Chiesa, Paolo Carniti, A. Juillard, Andrea Barresi, V.I. Tretyak, E. V. Hansen, M. Xue, S. Zucchelli, C. Pira, O. G. Polischuk, X. F. Navick, R. J. Creswick, L. Marini, K. Wilson, I. Colantoni, D. Misiak, C. Rusconi, J. Billard, D. V. Poda, J. Johnston, Jonathan Ouellet, A. Charrier, A. Cruciani, S. L. Wagaarachchi, G. Bari, F. Collamati, V. Yumatov, J. Gascon, C. C. Chang, Stefano Nisi, Changbo Fu, G. Pessina, S. Pirro, L. Pattavina, S. Marnieros, Jie Zhang, G. Wang, G. D'Imperio, A. Cazes, Yuting Liu, E. Celi, Massimiliano Clemenza, A. Tsymbaliuk, Monica Sisti, Valentyn Novosad, I. Nutini, S. Milana, R. Nipoti, C. Nones, A. Puiu, M. Chapellier, H. Z. Huang, V. G. Yefremenko, R. Mariam, B. Schmidt, G. Keppel, Yu. G. Kolomensky, Luigi Cappelli, D. Mayer, O. Tellier, L. Ma, Y. Mei, R. G. Huang, F. Mancarella, M. Faverzani, L. Dumoulin, M. Madhukuttan, H. Khalife, M. Gros, Kai Vetter, S. Di Domizio, D. Baudin, P. Pari, A. Armatol, Giovanni Benato, M. Beretta, Tomas Polakovic, L. Taffarello, Virendra Singh, Danielle Speller, Laura Cardani, K. M. Heeger, B. K. Fujikawa, E. Olivieri, Eric B. Norman, L. Yan, T. Napolitano, S. Pagan, M. Biassoni, B. Mauri, V. Pettinacci, M. de Combarieu, O. Azzolini, M. M. Zarytskyy, A. Giachero, Claudio Gotti, S. I. Konovalov, L. Gironi, Lindley Winslow, M. Pavan, James Nikkel, F. T. Avignone, Whitney Armstrong, V. Sanglard, L. Imbert, C. Bucci, T. D. Gutierrez, C. Brofferio, A. S. Barabash, Ezio Previtali, B. Welliver, P. de Marcillac, D. L. Helis, A. S. Zolotarova, Ke Han, Reina H. Maruyama, B. Paul, A. Giuliani, Silvia Capelli, Massimiliano Nastasi, James R. Wilson, M. De Jesus, E. Armengaud, V. Sharma, Matias Velázquez, V. V. Kobychev, L. Bergé, A. Branca, C. Rosenfeld, V. Boldrini, P. Gorla, F. Ferroni, C. Tomei, Emanuele Ferri, Joseph A. Formaggio, S. Pozzi, V. Dompè, A. D'Addabbo, Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut Rayonnement Matière de Saclay (IRAMIS), Service de physique de l'état condensé (SPEC - UMR3680), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Science et Ingénierie des Matériaux et Procédés (SIMaP), Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), CUPID, Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS), 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., Berge 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., J.Creswick R., Cruciani A., D'Addabbo A., D'Imperio G., Dafinei I., A.Danevich F., deCombarieu M., DeJesus M., deMarcillac P., Dell'Oro S., DiDomizio 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 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 Y.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., V.Poda D., Polakovic T., Polischuk O.G., Pozzi S., Previtali E., Puiu A., Ressa A., Rizzoli R., Rosenfeld C., Rusconi C., Sanglard V., Scarpaci J.A., 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., Armatol, A, Armengaud, E, Armstrong, W, Augier, C, Avignone, F, Azzolini, O, Barabash, A, Bari, G, Barresi, A, Baudin, D, Bellini, F, Benato, G, Beretta, M, Berge, 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, J. Creswick, R, Cruciani, A, D'Addabbo, A, D'Imperio, G, Dafinei, I, A. Danevich, F, Decombarieu, M, Dejesus, M, Demarcillac, P, Dell'Oro, S, Didomizio, 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, B, Gascon, J, Giachero, A, Gironi, L, Giuliani, A, Gorla, P, Gotti, C, Gras, P, Gros, M, Gutierrez, T, Han, K, Hansen, E, Heeger, K, Helis, D, Huang, H, Huang, R, Imbert, L, Johnston, J, Juillard, A, Karapetrov, G, Keppel, G, Khalife, H, Kobychev, V, Kolomensky, Y, Konovalov, S, Liu, Y, Loaiza, P, Ma, L, Madhukuttan, M, Mancarella, F, Mariam, R, Marini, L, Marnieros, S, Martinez, M, Maruyama, R, Mauri, B, Mayer, D, Mei, Y, Milana, S, Misiak, D, Napolitano, T, Nastasi, M, Navick, X, Nikkel, J, Nipoti, R, Nisi, S, Nones, C, Norman, E, Novosad, V, Nutini, I, O'Donnell, T, Olivieri, E, Oriol, C, Ouellet, J, Pagan, S, Pagliarone, C, Pagnanini, L, Pari, P, Pattavina, L, Paul, B, Pavan, M, Peng, H, Pessina, G, Pettinacci, V, Pira, C, Pirro, S, V. Poda, D, Polakovic, T, Polischuk, O, 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, Taffarello, L, Tellier, O, Tomei, C, Tretyak, V, Tsymbaliuk, A, Velazquez, M, Vetter, K, Wagaarachchi, S, Wang, G, Wang, L, Welliver, B, Wilson, J, Wilson, K, Winslow, L, Xue, M, Yan, L, Yang, J, Yefremenko, V, Yumatov, V, Zarytskyy, M, Zhang, J, Zolotarova, A, and Zucchelli, S

Subjects
Mo-100, Physics - Instrumentation and Detectors, Physics and Astronomy (miscellaneous), background: induced, Physics::Instrumentation and Detectors, Monte Carlo method, measurement methods, bolometers, neutrinoless double beta decay, energy resolution, Parameter space, 01 natural sciences, Nuclear Experiment (nucl-ex), Double Beta Decay, Nuclear Experiment, background: suppression, Physics, Detector, Instrumentation and Detectors (physics.ins-det), Scintillators, scintillation and light emission processes (solid, gas and liquid scintillators), molybdenum: oxygen, Double-beta decay detector, Low Temperature Detector, lithium, Scintillation counter, Neutrino, photon: yield, numerical calculations: Monte Carlo, bolometers, FOS: Physical sciences, Cryogenic detector, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], neutrinoless double beta decay, Particle identification method, double-beta decay: (0neutrino), Double beta decay, CUPID, 0103 physical sciences, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], 010306 general physics, Engineering (miscellaneous), scintillation counter, Scintillation, molybdenum: nuclide, 010308 nuclear & particles physics, bibliography, crystal: geometry, Computational physics, efficiency, FIS/04 - FISICA NUCLEARE E SUBNUCLEARE, Energy (signal processing)
Abstract

The CUPID Collaboration is designing a tonne-scale, background-free detector to search for double beta decay with sufficient sensitivity to fully explore the parameter space corresponding to the inverted neutrino mass hierarchy scenario. One of the CUPID demonstrators, CUPID-Mo, has proved the potential of enriched Li$$_{2}$$ 2 $$^{100}$$ 100 MoO$$_4$$ 4 crystals as suitable detectors for neutrinoless double beta decay search. In this work, we characterised cubic crystals that, compared to the cylindrical crystals used by CUPID-Mo, are more appealing for the construction of tightly packed arrays. We measured an average energy resolution of ($$6.7\pm 0.6$$ 6.7 ± 0.6 ) keV FWHM in the region of interest, approaching the CUPID target of 5 keV FWHM. We assessed the identification of $$\alpha $$ α particles with and without a reflecting foil that enhances the scintillation light collection efficiency, proving that the baseline design of CUPID already ensures a complete suppression of this $$\alpha $$ α -induced background contribution. We also used the collected data to validate a Monte Carlo simulation modelling the light collection efficiency, which will enable further optimisations of the detector.

Published
2021
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36. Novel technique for the study of pileup events in cryogenic bolometers

Author

Valentyn Novosad, Andrea Giachero, R. Nipoti, Jie Zhang, H. Z. Huang, V. G. Yefremenko, G. Keppel, D. Mayer, C. Nones, A. Puiu, S. Nisi, A. Armatol, K. Wilson, I. Colantoni, A. Barresi, P. Loaiza, C. Oriol, G. Pessina, V. Sanglard, L. Imbert, M. Faverzani, M. Beretta, S. Copello, C. Pagliarone, F.A. Danevich, A. Branca, Jonathan Ouellet, T. O'Donnell, Paolo Carniti, Massimiliano Clemenza, G. Bari, S. Di Domizio, Kai Vetter, C. Rosenfeld, D. L. Helis, Monica Sisti, Federico Ferri, H. Khalife, V. Boldrini, P. Gorla, P. Pari, F. Ferroni, Tomas Polakovic, B. Schmidt, Stefano Dell'Oro, A. Charrier, J. Billard, C. Tomei, S. H. Fu, N. Casali, Laura Cardani, G. Wang, Jie Yang, B. K. Fujikawa, R. J. Creswick, Davide Chiesa, P. Gras, M. Chapellier, C. Pira, Joseph A. Formaggio, L. Pagnanini, P. T. Surukuchi, C. Brofferio, L. Wang, Massimiliano Nastasi, Stefano Pozzi, E. Figueroa-Feliciano, Haiping Peng, V. Shlegel, V. Sharma, E. V. Hansen, A. S. Barabash, B. Paul, M. Gros, Evelyn Ferri, Oliviero Cremonesi, S. Zucchelli, James Nikkel, Ezio Previtali, J. Gascon, R. Mariam, C. C. Chang, L. Ma, Yu. G. Kolomensky, Luigi Cappelli, L. Taffarello, B. Welliver, A. Giuliani, M. Madhukuttan, Matias Velázquez, C. Augier, S. Marnieros, V. Yumatov, Goran Karapetrov, G. Fantini, A. Cazes, Danielle Speller, James R. Wilson, A. Cruciani, X. F. Navick, S. Pirro, V. V. Kobychev, J. Camilleri, A. Franceschi, Changbo Fu, C. Rusconi, J. A. Scarpaci, A. Juillard, L. Bergé, R. Rizzoli, M. M. Zarytskyy, V. Dompè, G. D'Imperio, Irene Nutini, A. D'Addabbo, P. de Marcillac, M. De Jesus, O. G. Polischuk, F. Bellini, A. Ressa, D. Baudin, M. Xue, M. Pavan, Lindley Winslow, A. Drobizhev, I. Dafinei, S. L. Wagaarachchi, F. Collamati, V. Pettinacci, Simone Capelli, E. Olivieri, S. I. Konovalov, Eric B. Norman, L. Pattavina, M. I. Martínez, T. Napolitano, L. Marini, V.I. Tretyak, D. Misiak, D. V. Poda, J. Johnston, M. Biassoni, E. Armengaud, Vasundhara Singh, S. Milana, O. Azzolini, L. Gironi, F. T. Avignone, Whitney Armstrong, Y. Liu, C. Bucci, T. D. Gutierrez, R. G. Huang, F. Mancarella, L. Yan, S. Pagan, B. Mauri, M. de Combarieu, E. Celi, C. Gotti, A. S. Zolotarova, Ke Han, Reina H. Maruyama, A. Tsymbaliuk, Y. Mei, K. M. Heeger, O. Tellier, L. Dumoulin, Giovanni Benato, 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., Berge 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., 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 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 Y.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., Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut Rayonnement Matière de Saclay (IRAMIS), Science et Ingénierie des Matériaux et Procédés (SIMaP), Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), CUPID, Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre National de la Recherche Scientifique (CNRS)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Armatol, A, Armengaud, E, Armstrong, W, Augier, C, Avignone, F, Azzolini, O, Barabash, A, Bari, G, Barresi, A, Baudin, D, Bellini, F, Benato, G, Beretta, M, Berge, 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, Cruciani, A, D'Addabbo, A, D'Imperio, G, Dafinei, I, Danevich, F, De Combarieu, 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, B, Gascon, J, Giachero, A, Gironi, L, Giuliani, A, Gorla, P, Gotti, C, Gras, P, Gros, M, Gutierrez, T, Han, K, Hansen, E, Heeger, K, Helis, D, Huang, H, Huang, R, Imbert, L, Johnston, J, Juillard, A, Karapetrov, G, Keppel, G, Khalife, H, Kobychev, V, Kolomensky, Y, Konovalov, S, Liu, Y, Loaiza, P, Ma, L, Madhukuttan, M, Mancarella, F, Mariam, R, Marini, L, Marnieros, S, Martinez, M, Maruyama, R, Mauri, B, Mayer, D, Mei, Y, Milana, S, Misiak, D, Napolitano, T, Nastasi, M, Navick, X, Nikkel, J, Nipoti, R, Nisi, S, Nones, C, Norman, E, Novosad, V, Nutini, I, O'Donnell, T, Olivieri, E, Oriol, C, Ouellet, J, 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, Polakovic, T, Polischuk, O, 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, Taffarello, L, Tellier, O, Tomei, C, Tretyak, V, Tsymbaliuk, A, Velazquez, M, Vetter, K, Wagaarachchi, S, Wang, G, Wang, L, Welliver, B, Wilson, J, Wilson, K, Winslow, L, Xue, M, Yan, L, Yang, J, Yefremenko, V, Yumatov, V, Zarytskyy, M, Zhang, J, Zolotarova, A, and Zucchelli, S

Subjects
data analysis method, double beta decay, nuclear tests of fundamental interactions, Particle decays, Physics - Instrumentation and Detectors, double beta decay, FOS: Physical sciences, Cryogenics, MESH: numerical calculation, 01 natural sciences, law.invention, benchmark, bolometer, double-beta decay: (0neutrino), law, Double beta decay, 0103 physical sciences, Electronic engineering, MESH: benchmark, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], numerical calculations, 010306 general physics, time resolution, nuclear tests of fundamental interactions, Physics, Signal generator, 010308 nuclear & particles physics, Bolometer, Detector, Time resolution, MESH: data analysis method, Instrumentation and Detectors (physics.ins-det), MESH: bolometer, Gran Sasso, Neutrinoless Double Beta decay, Neutrino Physics, MESH: cryogenics, efficiency, cryogenics, pile-up, Rise time, MESH: Gran Sasso, Benchmark (computing), MESH: double-beta decay: (0neutrino), Neutrinoless double-beta decay, MESH: efficiency, Particle decays, MESH: time resolution, MESH: pile-up
Abstract

International audience; 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 pile-up of two-neutrino double-beta decay events. In this paper, we describe a technique developed to study the pile-up rejection capability of cryogenic bolometers. Our approach, which consists of producing controlled pile-up events with a programmable waveform generator, has the benefit that we can reliably and reproducibly control the time separation and relative energy of the individual components of the generated pile-up events. The resulting data allow us to optimize and benchmark analysis strategies to discriminate between individual and pile-up 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 pile-up events with rise time of ~15 ms down to time separation between the individual events of 2 ms.

Published
2021
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37. A CUPID Li$_2$ $^{100} $MoO$_4$ scintillating bolometer tested in the CROSS underground facility

Author

A. S. Barabash, V. Yumatov, G. D'Imperio, M. De Deo, Ezio Previtali, J. M. Calvo-Mozota, Evelyn Ferri, B. Welliver, L. Gironi, L. Marini, E. Guerard, D. Misiak, D. V. Poda, J. Johnston, V. Dompè, F. T. Avignone, Whitney Armstrong, A. Charrier, O. Tellier, I. Colantoni, A. D'Addabbo, S. Di Domizio, P. Pari, Tomas Polakovic, Massimiliano Clemenza, V. Shlegel, R. Mariam, Yu. G. Kolomensky, Luigi Cappelli, Monica Sisti, M. Pavan, S. Zucchelli, Laura Cardani, P. de Marcillac, C. Augier, Goran Karapetrov, X.-F. Navick, B. K. Fujikawa, Stefano Pozzi, L. Pagnanini, P. T. Surukuchi, O. Azzolini, G. Fantini, Federico Ferri, B. Schmidt, C. Oriol, C. Pagliarone, E. Celi, T. O'Donnell, S. H. Fu, S. Dell'Oro, Giovanni Benato, M. Xue, Yuting Liu, Ch. Bourgeois, C. C. Chang, Stefano Nisi, James R. Wilson, S. Milana, G. Olivier, A. Cruciani, A. Franceschi, Changbo Fu, I. Dafinei, M. Chapellier, C. Gotti, S. Copello, C. Brofferio, S. Pirro, Jie Yang, V. Sharma, D. L. Helis, A. Barresi, J. Camilleri, R. Rizzoli, L. Ma, L. Dumoulin, Davide Chiesa, A. S. Zolotarova, Paolo Carniti, V. Pettinacci, A. Juillard, A. Candela, M. Gros, M. Madhukuttan, I. C. Bandac, M. De Jesus, E. V. Hansen, O. G. Polischuk, A. Drobizhev, Ke Han, F. Bellini, A. Ressa, Reina H. Maruyama, V.I. Tretyak, F.A. Danevich, J. A. Scarpaci, C. Bucci, T. D. Gutierrez, M. Faverzani, Matias Velázquez, P. Loaiza, Kai Vetter, Massimiliano Nastasi, S. I. Konovalov, L. Taffarello, D. Reynet, V. V. Kobychev, L. Bergé, J. Gascon, V. Sanglard, L. Yan, L. Imbert, Virendra Singh, M. M. Zarytskyy, Valentyn Novosad, C. Rosenfeld, Danielle Speller, Andrea Giachero, N. Casali, A. Branca, L. Pattavina, A. Ianni, E. Olivieri, R. J. Creswick, Eric B. Norman, V. Boldrini, P. Gras, K. Wilson, S. Pagan, J. Billard, S. Marnieros, Li Wang, T. Napolitano, R. Nipoti, A. Cazes, P. Gorla, F. Ferroni, E. Figueroa-Feliciano, C. Tomei, C. Pira, Haiping Peng, Oliviero Cremonesi, M. Biassoni, D. Mayer, Jonathan Ouellet, G. Bari, Lindley Winslow, M. de Combarieu, Joseph A. Formaggio, A. Tsymbaliuk, Y. Mei, A. Armatol, K. M. Heeger, R. G. Huang, F. Mancarella, B. Paul, M. I. Martínez, G. Pessina, Jie Zhang, C. Nones, A. Puiu, A. Giuliani, B. Mauri, James Nikkel, Irene Nutini, G. Wang, H. Z. Huang, V. G. Yefremenko, G. Keppel, H. Khalife, E. Armengaud, D. Baudin, M. Beretta, S. L. Wagaarachchi, F. Collamati, Simone Capelli, Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut Rayonnement Matière de Saclay (IRAMIS), Science et Ingénierie des Matériaux et Procédés (SIMaP), Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), CUPID, CROSS, Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Armatol A., Armengaud E., Armstrong W., Augier C., Iii F.T.A., Azzolini O., Bandac I.C., Barabash A.S., Bari G., Barresi A., Baudin D., Bellini F., Benato G., Beretta M., Berge L., Bourgeois C., Biassoni M., Billard J., Boldrini V., Branca A., Brofferio C., Bucci C., Calvo-Mozota J.M., 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 R.J., Cruciani A., D'Addabbo A., D'Imperio G., Dafinei I., Danevich F.A., De Combarieu M., Deo M.D., Jesus M.D., De Marcillac P., Dell'Oro S., Domizio S.D., 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 B.K., Gascon J., Giachero A., Gironi L., Giuliani A., Gorla P., Gotti C., Gras P., Gros M., Guerard E., Gutierrez T.D., Han K., Hansen E.V., Heeger K.M., Helis D.L., Huang H.Z., Huang R.G., Ianni A., Imbert L., Johnston J., Juillard A., Karapetrov G., Keppel G., Khalife H., Kobychev V.V., Kolomensky Y.G., Konovalov S.I., 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., Olivier G., 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., Reynet D., Rizzoli R., Rosenfeld C., Sanglard V., Scarpaci J.A., Schmidt B., Sharma V., Shlegel V.N., 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.I., Zarytskyy M.M., Zhang J., Zolotarova A.S., Zucchelli S., Armatol, A, Armengaud, E, Armstrong, W, Augier, C, Avignone F. T., I, Azzolini, O, Bandac, I, Barabash, A, Bari, G, Barresi, A, Baudin, D, Bellini, F, Benato, G, Beretta, M, Berge, L, Bourgeois, C, Biassoni, M, Billard, J, Boldrini, V, Branca, A, Brofferio, C, Bucci, C, Calvo-Mozota, J, 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, R, Cruciani, A, D'Addabbo, A, D'Imperio, G, Dafinei, I, Danevich, F, De Combarieu, M, Deo, M, Jesus, M, De Marcillac, P, Dell'Oro, S, 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, B, Gascon, J, Giachero, A, Gironi, L, Giuliani, A, Gorla, P, Gotti, C, Gras, P, Gros, M, Guerard, E, Gutierrez, T, Han, K, Hansen, E, Heeger, K, Helis, D, Huang, H, Huang, R, Ianni, A, Imbert, L, Johnston, J, Juillard, A, Karapetrov, G, Keppel, G, Khalife, H, Kobychev, V, Kolomensky, Y, Konovalov, S, Liu, Y, Loaiza, P, Ma, L, Madhukuttan, M, Mancarella, F, Mariam, R, Marini, L, Marnieros, S, Martinez, M, Maruyama, R, Mauri, B, Mayer, D, Mei, Y, Milana, S, Misiak, D, Napolitano, T, Nastasi, M, Navick, X, Nikkel, J, Nipoti, R, Nisi, S, Nones, C, Norman, E, Novosad, V, Nutini, I, O'Donnell, T, Olivier, G, Olivieri, E, Oriol, C, Ouellet, J, 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, Polakovic, T, Polischuk, O, Pozzi, S, Previtali, E, Puiu, A, Ressa, A, Reynet, D, Rizzoli, R, Rosenfeld, C, Sanglard, V, Scarpaci, J, Schmidt, B, Sharma, V, Shlegel, V, Singh, V, Sisti, M, Speller, D, Surukuchi, P, Taffarello, L, Tellier, O, Tomei, C, Tretyak, V, Tsymbaliuk, A, Velazquez, M, Vetter, K, Wagaarachchi, S, Wang, G, Wang, L, Welliver, B, Wilson, J, Wilson, K, Winslow, L, Xue, M, Yan, L, Yang, J, Yefremenko, V, Yumatov, V, Zarytskyy, M, Zhang, J, Zolotarova, A, and Zucchelli, S

Subjects
gas and liquid scintillators), Physics - Instrumentation and Detectors, Accurate estimation, Physics::Instrumentation and Detectors, Bolometer, Analytical chemistry, Double-beta decay, FOS: Physical sciences, Cryogenic detector, Radiopurity, 01 natural sciences, 030218 nuclear medicine & medical imaging, law.invention, Particle identification, Particle identification methods, 03 medical and health sciences, Particle identification method, 0302 clinical medicine, CUORE, law, 0103 physical sciences, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], Detector array, Instrumentation, Mathematical Physics, Event triggered, Physics, Lithium molybdate, 010308 nuclear & particles physics, Astrophysics::Instrumentation and Methods for Astrophysics, Instrumentation and Detectors (physics.ins-det), Scintillators, scintillation and light emission processes (solid, gas and liquid scintillators), Double-beta decay detectors, scintillation and light emission processes (solid, Double-beta decay detector, Cryogenic detectors, Scintillators, Crystal scintillator, Energy (signal processing)
Abstract

A scintillating bolometer based on a large cubic Li$_{2}$$^{100}$MoO$_4$ crystal (45 mm side) and a Ge wafer (scintillation detector) has been operated in the CROSS cryogenic facility at the Canfranc underground laboratory in Spain. The dual-readout detector is a prototype of the technology that will be used in the next-generation $0\nu2\beta$ experiment CUPID. The measurements were performed at 18 and 12 mK temperature in a pulse tube dilution refrigerator. This setup utilizes the same technology as the CUORE cryostat that will host CUPID and so represents an accurate estimation of the expected performance. The Li$_{2}$$^{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 $0\nu2\beta$ decay in CROSS and CUPID projects., Comment: 19 pages, 7 figures, 1 table

Published
2021
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38. Searching for New Physics in two-neutrino double beta decay with CUPID

Author

A Armatol, E Armengaud, W Armstrong, C Augier, F T Avignone, O Azzolini, A Barabash, G Bari, A Barresi, D Baudin, F Bellini, G Benato, M Beretta, L Bergé, M Biassoni, J Billard, V Boldrini, A Branca, C Brofferio, C Bucci, J Camilleri, S Capelli, L Cappelli, L Cardani, P Carniti, N Casali, A Cazes, E Celi, C Chang, M Chapellier, A Charrier, D Chiesa, M Clemenza, I Colantoni, F Collamati, S Copello, O Cremonesi, R J Creswick, A Cruciani, A D’ Addabbo, G D’ Imperio, I Dafinei, F A Danevich, M de Combarieu, M De Jesus, P de Marcillac, S Dell’Oro, S Di Domizio, V Dompè, A Drobizhev, L Dumoulin, G Fantini, M Faverzani, E Ferri, F Ferri, F Ferroni, E Figueroa-Feliciano, J Formaggio, A Franceschi, C Fu, S Fu, B K Fujikawa, J Gascon, S Ghislandi, A Giachero, L Gironi, A Giuliani, P Gorla, C Gotti, P Gras, M Gros, T D Gutierrez, K Han, E V Hansen, K M Heeger, D L Helis, H Z Huang, R G Huang, L Imbert, J Johnston, A Juillard, G Karapetrov, G Keppel, H Khalife, V V Kobychev, J Kotila, Yu G Kolomensky, S Konovalov, Y Liu, P Loaiza, L Ma, M Madhukuttan, F Mancarella, R Mariam, L Marini, S Marnieros, M Martinez, R H Maruyama, B Mauri, D Mayer, Y Mei, S Milana, D Misiak, T Napolitano, M Nastasi, X F Navick, J Nikkel, R Nipoti, S Nisi, C Nones, E B Norman, V Novosad, I Nutini, T O’Donnell, E Olivieri, C Oriol, J L Ouellet, S Pagan, C Pagliarone, L Pagnanini, P Pari, L Pattavina, B Paul, M Pavan, H Peng, G Pessina, V Pettinacci, C Pira, S Pirro, D V Poda, T Polakovic, O G Polischuk, S Pozzi, E Previtali, A Puiu, S Quitadamo, A Ressa, R Rizzoli, C Rosenfeld, C Rusconi, V Sanglard, J Scarpaci, B Schmidt, V Sharma, V Shlegel, V Singh, M Sisti, D Speller, P T Surukuchi, L Taffarello, O Tellier, C Tomei, V I Tretyak, A Tsymbaliuk, M Velazquez, K J Vetter, S L Wagaarachchi, G Wang, L Wang, B Welliver, J Wilson, K Wilson, L A Winslow, M Xue, L Yan, J Yang, V Yefremenko, V Yumatov, M M Zarytskyy, J Zhang, A Zolotarova, S Zucchelli, Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Institut Rayonnement Matière de Saclay (IRAMIS), Science et Ingénierie des Matériaux et Procédés (SIMaP), Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), and Université Grenoble Alpes (UGA)

Subjects
CUPID, Neutrinoless Double Beta Decay, LNGS, Particle Physics, Neutrino, Majorana Neutrino, History, LNGS, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], hiukkasfysiikka, Neutrinoless Double Beta Decay, Education, crystal, CUPID, Neutrino, [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], double-beta decay: (2neutrino), Particle Physics, scintillation counter, symmetry: violation, background, new physics: search for, Majorana Neutrino, neutriinot, sensitivity, violation: Lorentz, Majoron, Computer Science Applications, calorimeter: cryogenics, electron: energy spectrum, symmetry: Lorentz, ydinfysiikka
Abstract

In the past few years, attention has been drawn to the fact that a precision analysis of two-neutrino double beta decay (2υββ) allows the study of interesting physics cases like the emission of Majoron bosons and possible Lorentz symmetry violation. These processes modify the summed-energy distribution of the two electrons emitted in 2υββ. CUPID is a next-generation experiment aiming to exploit 100Mo-enriched scintillating Li2MoO4 crystals, operating as cryogenic calorimeters. Given the relatively fast half-life of 100Mo 2υββ and the large exposure that can be reached by CUPID, we expect to measure with very high precision the 100Mo 2υββ spectrum shape, reaching great sensitivities in the search for distortions induced by the physics beyond the Standard Model. In this contribution, we present the CUPID exclusion sensitivity for such New Physics processes, as well as the preliminary projected background of CUPID.

Published
2021
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39. An acrylic assembly for low-temperature detectors

Author

Stefano Pozzi, S. Quitadamo, M. Biassoni, S. Milana, Emanuele Ferri, S. Ghislandi, M. Faverzani, V. Pettinacci, Irene Nutini, C. Brofferio, Biassoni, M, Brofferio, C, Faverzani, M, Ferri, E, Ghislandi, S, Milana, S, Nutini, I, Pettinacci, V, Pozzi, S, and Quitadamo, S

Subjects
Work (thermodynamics), Materials science, Physics - Instrumentation and Detectors, business.industry, Physics::Instrumentation and Detectors, Detector, Complex system, Plastic materials, General Physics and Astronomy, chemistry.chemical_element, FOS: Physical sciences, Instrumentation and Detectors (physics.ins-det), Applied Physics (physics.app-ph), Physics - Applied Physics, Thermal detector, Copper, chemistry, Inorganic crystals, Thermal detectors, Optoelectronics, business
Abstract

Thermal detectors are a powerful instrument for the search of rare particle physics events. Inorganic crystals are classically used as thermal detectors held in supporting frames made of copper. In this work a novel approach to the operation of thermal detectors is presented, where TeO2 crystals are cooled down to ~ 10 mK in a light structure built with plastic materials. The advantages of this approach are discussed., 8 pages, 9 figures

Published
2021

40. Algorithms for Identification of Nearly-Coincident Events in Calorimetric Sensors

Author

B, Alpert, E, Ferri, D, Bennett, M, Faverzani, J, Fowler, A, Giachero, J, Hays-Wehle, M, Maino, A, Nucciotti, A, Puiu, D, Swetz, and J, Ullom

Subjects
Article
Abstract

For experiments with high arrival rates, reliable identification of nearly-coincident events can be crucial. For calorimetric measurements to directly measure the neutrino mass such as HOLMES, unidentified pulse pile-ups are expected to be a leading source of experimental error. Although Wiener filtering can be used to recognize pile-up, it suffers errors due to pulse-shape variation from detector nonlinearity, readout dependence on sub-sample arrival times, and stability issues from the ill-posed deconvolution problem of recovering Dirac delta-functions from smooth data. Due to these factors, we have developed a processing method that exploits singular value decomposition to (1) separate single-pulse records from piled-up records in training data and (2) construct a model of single-pulse records that accounts for varying pulse shape with amplitude, arrival time, and baseline level, suitable for detecting nearly-coincident events. We show that the resulting processing advances can reduce the required performance specifications of the detectors and readout system or, equivalently, enable larger sensor arrays and better constraints on the neutrino mass.

Published
2020

41. Improved Limit on Neutrinoless Double-Beta Decay in Te130 with CUORE

Author

Yudi Ma, Massimiliano Clemenza, C. Pagliarone, Carlo Cosmelli, B. S. Wang, Silvia Capelli, Massimiliano Nastasi, S. Pirro, N. Chott, C. Brofferio, C. Rosenfeld, V. Novati, Davide Chiesa, A. Caminata, L. Ma, V. Dompè, Ezio Previtali, Marco Pallavicini, A. D'Addabbo, P. Gorla, F. Ferroni, C. Tomei, James R. Wilson, B. Welliver, K. Wilson, Emanuele Ferri, Carlo Ligi, A. Campani, R. G. Huang, I. Nutini, D. Q. Adams, I. Dafinei, M. Sakai, Jonathan Ouellet, G. Bari, K. Alfonso, Giovanni Benato, N. D. Scielzo, C. Nones, E. Fiorini, C. Bucci, Lucia Canonica, S. Di Domizio, A. Puiu, T. D. Gutierrez, C. Rusconi, M. Faverzani, Deqing Fang, C. J. Davis, Laura Cardani, B. K. Fujikawa, L. Zanotti, F. Bellini, S. Morganti, Stefano Dell'Oro, A. Branca, L. Marini, M. Vignati, S. L. Wagaarachchi, S. Pozzi, J. Johnston, L. Pattavina, A. Giachero, V. Sharma, R. J. Creswick, L. Cappelli, B. Schmidt, T. Napolitano, G. Pessina, N. Moggi, A. Giuliani, Stefano Zucchelli, O. Azzolini, M. Biassoni, V. Pettinacci, Samuele Sangiorgio, A. Nucciotti, M. Sisti, S. Copello, C. Alduino, G. Fantini, S. Zimmermann, D. D'Aguanno, L. Pagnanini, L. Gironi, F. T. Avignone, Paolo Carniti, M. A. Franceschi, Eric B. Norman, M. Pavan, J. Nikkel, P. T. Surukuchi, Lindley Winslow, T. O'Donnell, F. Terranova, H. Z. Huang, Y. Mei, Xiangyu Cao, G. Keppel, Oliviero Cremonesi, K. M. Heeger, Ke Han, Reina H. Maruyama, Stuart J. Freedman, N. Casali, Yu. G. Kolomensky, Claudio Gotti, C. Pira, L. Taffarello, Virendra Singh, and Danielle Speller

Subjects
Physics, Semileptonic decay, Particle physics, General Physics and Astronomy, 01 natural sciences, Lower limit, MAJORANA, CUORE, Double beta decay, 0103 physical sciences, Limit (mathematics), Sensitivity (control systems), Neutrino, 010306 general physics
Abstract

We report new results from the search for neutrinoless double-beta decay in ^{130} Te with the CUORE detector. This search benefits from a fourfold increase in exposure, lower trigger thresholds, and analysis improvements relative to our previous results. We observe a background of (1.38±0.07)×10^{-2} counts/(keV kg yr)) in the 0νββ decay region of interest and, with a total exposure of 372.5 kg yr, we attain a median exclusion sensitivity of 1.7×10^{25} yr. We find no evidence for 0νββ decay and set a 90% credibility interval Bayesian lower limit of 3.2×10^{25} yr on the ^{130} Te half-life for this process. In the hypothesis that 0νββ decay is mediated by light Majorana neutrinos, this results in an upper limit on the effective Majorana mass of 75-350 meV, depending on the nuclear matrix elements used.

Published
2020
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42. TES Microcalorimeters for PTOLEMY

Author

Flavio Gatti, Evelyn Ferri, Andrea Giachero, A. Nucciotti, M. Faverzani, R. Filippo, Michele Biasotti, M. Rajteri, A. Puiu, E. Monticone, Rajteri, M, Biasotti, M, Faverzani, M, Ferri, E, Filippo, R, Gatti, F, Giachero, A, Monticone, E, Nucciotti, A, and Puiu, A

Subjects
Physics, Photon, business.industry, Transition-edge sensor, Electron, Condensed Matter Physics, 01 natural sciences, Atomic and Molecular Physics, and Optics, 010305 fluids & plasmas, Cosmic neutrino background, Key point, Optics, 0103 physical sciences, General Materials Science, Thin film, 010306 general physics, business, High electron, Penetration depth, Visible spectrum
Abstract

The PTOLEMY project is devoted to directly detect the cosmic neutrino background. A key point for the project success is the development of a device which is capable of detecting electrons with an energy resolution lower than 0.05eV. Microcalorimeters based on transition-edge sensors are among the best candidates since they already reach 0.11eV of energy resolution for telecomm photons. To further improve the energy resolution, while maintaining a suitable saturation energy, it is necessary to reduce the transition temperature. This could be achieved by proximity effect of a normal-superconducting bilayer. To this aim, TiAu very thin films are under development to demonstrate the feasibility of reaching 0.05eV energy resolution for light pulses of few eV. Thanks to the high electron stopping power of metals, the penetration depth of low energy incident electrons is limited to few nanometers and, with respect to visible light, we expect a high detection efficiency, while keeping similar dark counts and energy resolution.

Published
2020

43. Transition-Edge Sensors for HOLMES

Author

D. A. Bennett, Gene C. Hilton, Michele Biasotti, Daniel Schmidt, Dan Becker, M. De Gerone, John A. B. Mates, A. Nucciotti, Andrea Giachero, Emanuele Ferri, M. Faverzani, Joseph W. Fowler, A. Puiu, Johnathon D. Gard, G. Gallucci, Joel N. Ullom, M. Borghesi, Leila R. Vale, G. Pessina, Daniel S. Swetz, Flavio Gatti, Puiu, A, Becker, D, Bennett, D, Biasotti, M, Borghesi, M, De Gerone, M, Faverzani, M, Ferri, E, Fowler, J, Gallucci, G, Gard, J, Gatti, F, Hilton, G, Giachero, A, Mates, J, Nucciotti, A, Pessina, G, Schmidt, D, Swetz, D, Ullom, J, and Vale, L

Subjects
Physics, Particle physics, Transition-edge sensors, Physics::Instrumentation and Detectors, Electron capture, RF-SQUID, Detector, Order (ring theory), HOLMES, Multiplexing, Condensed Matter Physics, 01 natural sciences, Atomic and Molecular Physics, and Optics, 010305 fluids & plasmas, 0103 physical sciences, General Materials Science, Sensitivity (control systems), Special care, Neutrino, 010306 general physics, Transition edge
Abstract

HOLMES is an experiment aiming at performing a direct measurement of the neutrino mass from the electron capture (EC) spectrum of $$^{163}\hbox {Ho}$$. In order to reach a sensitivity of the order of $$\sim $$1 eV/c$$^2$$ on the neutrino mass, it is necessary to gather as many as $$10^{13}$$ events in the 3-year projected live time of HOLMES, keeping the pileup fraction as low as $$10^{-4}$$. This is not a trivial matter when it comes to low- temperature calorimeters, which usually have a rather slow time response. At the same time, a large number of detectors need to be operated simultaneously, and hence, in order to avoid an extremely large cryogenic facility, multiplexing is required. In this contribution, I will outline the current status and perspective of HOLMES, with special care devoted to the detectors and readout system, which have currently reached their target performance.

Published
2020

44. Perspectives of lowering CUORE thresholds with Optimum Trigger

Author

Monica Sisti, A. Bersani, C. Brofferio, G. Fantini, A. Caminata, Marco Pallavicini, B. Welliver, C. Pagliarone, R. G. Huang, M. Faverzani, Y. u. G. Kolomensky, H. Z. Huang, G. Keppel, Massimiliano Nastasi, Yudi Ma, S. Pozzi, S. L. Wagaarachchi, C. Cosmelli, A. Giuliani, C. Pira, C. Rusconi, Ke Han, A. Branca, N. D. Scielzo, Reina H. Maruyama, N. Casali, Stefano Dell'Oro, Lucia Canonica, F. Bellini, I. Dafinei, V. Novati, T. Wise, V. Pettinacci, Davide Chiesa, Stefano Zucchelli, Laura Cardani, L. Gironi, M. Pavan, B. K. Fujikawa, Y. Mei, V. Singh, D. D'Aguanno, F. T. Avignone, L. Taffarello, R. J. Creswick, C. Rosenfeld, P. Gorla, Danielle Speller, F. Ferroni, C. Tomei, M. Vignati, E. Previtali, Simone Capelli, D. Q. Adams, L. Marini, C. J. Davis, K. Alfonso, T. O'Donnell, B. Schmidt, N. Chott, C. Nones, A. Puiu, Lindley Winslow, S. Zimmermann, Oliviero Cremonesi, J. Johnston, L. Pattavina, Irene Nutini, S. Copello, C. Bucci, Miriam Lucio Martinez, Paolo Carniti, Sergio Di Domizio, S. Pirro, Xi-Guang Cao, E. Fiorini, S. J. Freedman, K. M. Heeger, Luigi Cappelli, T. D. Gutierrez, F. Terranova, K. Wilson, G. Pessina, B. S. Wang, Jonathan Ouellet, G. Bari, O. Azzolini, Evelyn Ferri, N. Moggi, Samuele Sangiorgio, A. Nucciotti, C. Alduino, Jeremy S. Cushman, S. Morganti, L. Zanotti, Carlo Ligi, A. Campani, V. Dompè, A. D'Addabbo, A. Leder, J. S. Wilson, Franceschi, Eric B. Norman, M. Sakai, T. Napolitano, M. Biassoni, Giovanni Benato, A. Drobizhev, C. Gotti, A. Giachero, D. Q. Fang, Massimiliano Clemenza, Centre de Sciences Nucléaires et de Sciences de la Matière (CSNSM), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), and Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay

Subjects
Physics, History, CUORE, 010308 nuclear & particles physics, Physics::Instrumentation and Detectors, WIMP nucleus: scattering, trigger: programming, 01 natural sciences, Large target, tellurium: oxygen, Computer Science Applications, Education, Combinatorics, energy: threshold, Low energy, double-beta decay: (0neutrino), 0103 physical sciences, High Energy Physics::Experiment, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], 010306 general physics, activity report, energy: low
Abstract

Author(s): Dompe, V; Adams, DQ; Alduino, C; Alfonso, K; Avignone, FT; Azzolini, O; Bari, G; Bellini, F; Benato, G; Bersani, A; Biassoni, M; Branca, A; Brofferio, C; Bucci, C; Caminata, A; Campani, A; Canonica, L; Cao, XG; Capelli, S; Cappelli, L; Cardani, L; Carniti, P; Casali, N; Chiesa, D; Chott, N; Clemenza, M; Copello, S; Cosmelli, C; Cremonesi, O; Creswick, RJ; Cushman, JS; D'Addabbo, A; D'Aguanno, D; Dafinei, I; Davis, CJ; Dell'Oro, S; Domizio, SD; Drobizhev, A; Fang, DQ; Fantini, G; Faverzani, M; Ferri, E; Ferroni, F; Fiorini, E; Franceschi, MA; Freedman, SJ; Fujikawa, BK; Giachero, A; Gironi, L; Giuliani, A; Gorla, P; Gotti, C; Gutierrez, TD; Han, K; Heeger, KM; Huang, RG; Huang, HZ; Johnston, J; Keppel, G; Kolomensky, YG; Leder, A; Ligi, C; Ma, YG; Marini, L; Martinez, M; Maruyama, RH; Mei, Y; Moggi, N; Morganti, S; Napolitano, T; Nastasi, M; Nones, C; Norman, EB; Novati, V; Nucciotti, A; Nutini, I; O'Donnell, T; Ouellet, JL; Pagliarone, CE; Pallavicini, M; Pattavina, L; Pavan, M; Pessina, G; Pettinacci, V; Pira, C | Abstract: CUORE is a cryogenic experiment that focuses on the search of neutrinoless double beta decay in 130Te and it is located at the Gran Sasso National Laboratories. Its detector consists of 988 TeO2 crystals operating at a base temperature of ∼10 mK. It is the first ton-scale bolometric experiment ever realized for this purpose. Thanks to its large target mass and ultra-low background, the CUORE detector is also suitable for the search of other rare phenomena. In particular the low energy part of the spectra is interesting for the detection of WIMP-nuclei scattering reactions. One of the most important requirements to perform these studies is represented by the achievement of a stable energy threshold lower than 10 keV. Here, the CUORE capability to accomplish this purpose using a low energy software trigger will be presented and described.

Published
2020
Full Text
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45. Probing the absolute neutrino mass scale with the 163Ho: The HOLMES project

Author

D. A. Bennett, R Dressier, A. Puiu, M. Faverzani, Dorothea Schumann, Joseph W. Fowler, Stefano Nisi, G. Gallucci, John A. B. Mates, Dan Becker, S. Heinitz, Leila R. Vale, V. Ceriale, Joel N. Ullom, G. Pessina, Daniel S. Swetz, Daniel Schmidt, M. Lusignoli, Carl D. Reintsema, S. Ragazzi, Gene C. Hilton, Emanuele Ferri, Bradley K. Alpert, U. Koester, Johnathon D. Gard, M. De Gerone, M. Ribeiro-Gomes, A. Orlando, Michele Biasotti, James P. Hays-Wehle, Flavio Gatti, A. Giachero, Gerone, M, Alpert, B, Becker, D, Bennett, D, Biasotti, M, Ceriale, V, Dressier, R, Faverzani, M, Ferri, E, Fowler, J, Gallucci, G, Gard, J, Gatti, F, Giachero, A, Hays-Wehle, J, Heinitz, S, Hilton, G, Koester, U, Lusignoli, M, Mates, J, Nisi, S, Orlando, A, Pessina, G, Puiu, A, Ragazzi, S, Reintsema, C, Ribeiro-Gomes, M, Schmidt, D, Schumann, D, Swetz, D, Ullom, J, and Vale, L

Subjects
Physics, History, Electron capture, Detector, Computer Science Applications, Education, Computational physics, law.invention, SQUID, Data acquisition, Neutrino mass, law, Sensitivity (control systems), Neutrino, Transition edge sensor, Electron neutrino
Abstract

The HOLMES project aims to directly measure the electron neutrino mass using the electron capture decay (EC) of 163Ho down to the eV scale. It will perform a precise measurement of the end-point of the 163Ho calorimetric energy spectrum to search for the deformation caused by a finite electron neutrino mass. The choice of 163Ho as source is driven by the very low Q-value of the EC reaction (around 2.8 keV), which allows for a high sensitivity while keeping the overall activities to reasonable value (O(102)Hz/detector), thus reducing the pile-up probability. A large array made of thousands of Transition Edge Sensor based micro-calorimeters will be used for a calorimetric measurement of the EC 163Ho spectrum. The calorimetric approach, with the source embedded inside the detector, eliminates systematic uncertainties arising from the use of an external beta-source, and minimizes the effect of the atomic de-excitation process uncertainties. The commissioning of the first implanted sub-array is scheduled for the end of 2017. It will provide useful data about the EC decay of 163Ho together with a first limit on neutrino mass. In this paper the current status of the main tasks will be summarized: the TES array design and engineering, the isotope preparation and embedding, and the development of a high speed multiplexed SQUID read-out system for the data acquisition.

Published
2020

46. Results from the CUORE experiment

Author

D. Q. Adams, C. Alduino, K. Alfonso, F. T. Avignone III, O. Azzolini, G. Bari, F. Bellini, G. Benato, M. Biassoni, A. Branca, C. Brofferio, C. Bucci, J. Camilleri, A. Caminata, A. Campani, L. Canonica, X. G. Cao, S. Capelli, L. Cappelli, L. Cardani, P. Carniti, N. Casali, D. Chiesa, M. Clemenza, S. Copello, C. Cosmelli, O. Cremonesi, R. J. Creswick, A. D'Addabbo, D. D'Aguanno, I. Dafinei, C. J. Davis, F. Del Corso, S. Dell'Oro, S. Di Domizio, V. Dompè, D. Q. Fang, G. Fantini, M. Faverzani, E. Ferri, F. Ferroni, E. Fiorini, M. A. Franceschi, S. J. Freedman, B. K. Fujikawa, A. Giachero, L. Gironi, A. Giuliani, P. Gorla, C. Gotti, T. D. Gutierrez, K. Han, K. M. Heeger, R. G. Huang, H. Z. Huang, J. Johnston, G. Keppel, Yu. G. Kolomensky, C. Ligi, L. Ma, Y. G. Ma, L. Marini, R. H. Maruyama, Y. Mei, N. Moggi, S. Morganti, T. Napolitano, M. Nastasi, J. Nikkel, C. Nones, E. B. Norman, V. Novati, A. Nucciotti, I. Nutini, T. O'Donnell, J. L. Ouellet, C. E. Pagliarone, L. Pagnanini, M. Pallavicini, L. Pattavina, M. Pavan, G. Pessina, V. Pettinacci, C. Pira, S. Pirro, S. Pozzi, E. Previtali, A. Puiu, C. Rosenfeld, C. Rusconi, M. Sakai, S. Sangiorgio, B. Schmidt, N. D. Scielzo, V. Singh, M. Sisti, D. Speller, L. Taffarello, F. Terranova, C. Tomei, M. Vignati, S. L. Wagaarachchi, B. S. Wang, B. Welliver, J. Wilson, K. Wilson, L. A. Winslow, L. Zanotti, S. Zimmermann, S. Zucchelli, Adams, D, Alduino, C, Alfonso, K, Avignone III, F, Azzolini, O, Bari, G, Bellini, F, Benato, G, Biassoni, M, Branca, A, Brofferio, C, Bucci, C, Camilleri, J, Caminata, A, Campani, A, Canonica, L, Cao, X, Capelli, S, Cappelli, L, Cardani, L, Carniti, P, Casali, N, Chiesa, D, Clemenza, M, Copello, S, Cosmelli, C, Cremonesi, O, Creswick, R, D'Addabbo, A, D'Aguanno, D, Dafinei, I, Davis, C, Del Corso, F, Dell'Oro, S, Di Domizio, S, Dompè, V, Fang, D, Fantini, G, Faverzani, M, Ferri, E, Ferroni, F, Fiorini, E, Franceschi, M, Freedman, S, Fujikawa, B, Giachero, A, Gironi, L, Giuliani, A, Gorla, P, Gotti, C, Gutierrez, T, Han, K, Heeger, K, Huang, R, Huang, H, Johnston, J, Keppel, G, Kolomensky, Y, Ligi, C, Ma, L, Ma, Y, Marini, L, Maruyama, R, Mei, Y, Moggi, N, Morganti, S, Napolitano, T, Nastasi, M, Nikkel, J, Nones, C, Norman, E, Novati, V, Nucciotti, A, Nutini, I, O'Donnell, T, Ouellet, J, Pagliarone, C, Pagnanini, L, Pallavicini, M, Pattavina, L, Pavan, M, Pessina, G, Pettinacci, V, Pira, C, Pirro, S, Pozzi, S, Previtali, E, Puiu, A, Rosenfeld, C, Rusconi, C, Sakai, M, Sangiorgio, S, Schmidt, B, Scielzo, N, Singh, V, Sisti, M, Speller, D, Taffarello, L, Terranova, F, Tomei, C, Vignati, M, Wagaarachchi, S, Wang, B, Welliver, B, Wilson, J, Wilson, K, Winslow, L, Zanotti, L, Zimmermann, S, and Zucchelli, S

Subjects
neutrinoless double beta decay
Published
2020

47. Lowering the Energy Threshold of the CUORE Experiment: Benefits in the Surface Alpha Events Reconstruction: Comparison Between Optimum Trigger and Derivative Trigger Performance in the Search for 0 νββ

Author

L. Pattavina, Marco Pallavicini, L. Canonica, L. Marini, S. Di Domizio, C. Bucci, T. D. Gutierrez, G. Pessina, K. Wilson, Stefano Dell'Oro, Jonathan Ouellet, J. Johnston, G. Bari, Laura Cardani, L. Zanotti, J. Nikkel, L. Gironi, F. T. Avignone, H. Z. Huang, B. K. Fujikawa, G. Keppel, Stefano Pozzi, Y. G. Ma, Massimiliano Clemenza, Carlo Cosmelli, Davide Chiesa, C. Nones, A. Puiu, V. Pettinacci, S. Zucchelli, N. D. Scielzo, L. Pagnanini, C. Brofferio, T. O'Donnell, D. Q. Fang, Claudio Gotti, Ke Han, Reina H. Maruyama, M. Vignati, C. Rusconi, Stuart J. Freedman, D. D'Aguanno, Ettore Fiorini, V. Novati, James R. Wilson, Andrea Giachero, C. Rosenfeld, P. Gorla, F. Ferroni, C. Tomei, M. A. Franceschi, C. Pagliarone, D. Q. Adams, R. G. Huang, N. Casali, F. Terranova, Vasundhara Singh, K. Alfonso, C. J. Davis, Monica Sisti, B. Schmidt, Eric B. Norman, B. S. Wang, L. Ma, O. Azzolini, Y. Mei, Lindley Winslow, V. Sharma, T. Napolitano, S. Copello, I. Dafinei, M. Sakai, Paolo Carniti, Silvia Capelli, Xi-Guang Cao, Massimiliano Nastasi, K. M. Heeger, F. Bellini, S. Pirro, L. Cappelli, Oliviero Cremonesi, M. Biassoni, R. J. Creswick, G. Fantini, M. Pavan, V. Dompè, Giovanni Benato, A. D'Addabbo, C. Pira, A. Caminata, Ezio Previtali, S. Morganti, B. Welliver, Carlo Ligi, Evelyn Ferri, N. Moggi, Samuele Sangiorgio, A. Campani, A. Nucciotti, C. Alduino, M. Faverzani, Yu. G. Kolomensky, A. Branca, L. Taffarello, A. Giuliani, Danielle Speller, S. L. Wagaarachchi, N. Chott, Irene Nutini, S. Zimmermann, Campani, A, Adams, D, Alduino, C, Alfonso, K, Avignone, F, Azzolini, O, Bari, G, Bellini, F, Benato, G, Biassoni, M, Branca, A, Brofferio, C, Bucci, C, Caminata, A, Canonica, L, Cao, X, Capelli, S, Cappelli, L, Cardani, L, Carniti, P, Casali, N, Chiesa, D, Chott, N, Clemenza, M, Copello, S, Cosmelli, C, Cremonesi, O, Creswick, R, D'Addabbo, A, D'Aguanno, D, Dafinei, I, Davis, C, Dell'Oro, S, Di Domizio, S, Dompe, V, Fang, D, Fantini, G, Faverzani, M, Ferri, E, Ferroni, F, Fiorini, E, Franceschi, M, Freedman, S, Fujikawa, B, Giachero, A, Gironi, L, Giuliani, A, Gorla, P, Gotti, C, Gutierrez, T, Han, K, Heeger, K, Huang, R, Huang, H, Johnston, J, Keppel, G, Kolomensky, Y, Ligi, C, Ma, Y, Ma, L, Marini, L, Maruyama, R, Mei, Y, Moggi, N, Morganti, S, Napolitano, T, Nastasi, M, Nikkel, J, Nones, C, Norman, E, Novati, V, Nucciotti, A, Nutini, I, O'Donnell, T, Ouellet, J, Pagliarone, C, Pagnanini, L, Pallavicini, M, Pattavina, L, Pavan, M, Pessina, G, Pettinacci, V, Pira, C, Pirro, S, Pozzi, S, Previtali, E, Puiu, A, Rosenfeld, C, Rusconi, C, Sakai, M, Sangiorgio, S, Schmidt, B, Scielzo, N, Sharma, V, Singh, V, Sisti, M, Speller, D, Taffarello, L, Terranova, F, Tomei, C, Vignati, M, Wagaarachchi, S, Wang, B, Welliver, B, Wilson, J, Wilson, K, Winslow, L, Zanotti, L, Zimmermann, S, Zucchelli, S, Campani A., Adams D.Q., Alduino C., Alfonso K., Avignone F.T., Azzolini O., Bari G., Bellini F., Benato G., Biassoni M., Branca A., Brofferio C., Bucci C., Caminata A., Canonica L., Cao X.G., Capelli S., Cappelli L., Cardani L., Carniti P., Casali N., Chiesa D., Chott N., Clemenza M., Copello S., Cosmelli C., Cremonesi O., Creswick R.J., D'Addabbo A., D'Aguanno D., Dafinei I., Davis C.J., Dell'Oro S., Di Domizio S., Dompe V., Fang D.Q., Fantini G., Faverzani M., Ferri E., Ferroni F., Fiorini E., Franceschi M.A., Freedman S.J., Fujikawa B.K., Giachero A., Gironi L., Giuliani A., Gorla P., Gotti C., Gutierrez T.D., Han K., Heeger K.M., Huang R.G., Huang H.Z., Johnston J., Keppel G., Kolomensky Y.G., Ligi C., Ma Y.G., Ma L., Marini L., Maruyama R.H., Mei Y., Moggi N., Morganti S., Napolitano T., Nastasi M., Nikkel J., Nones C., Norman E.B., Novati V., Nucciotti A., Nutini I., O'Donnell T., Ouellet J.L., Pagliarone C.E., Pagnanini L., Pallavicini M., Pattavina L., Pavan M., Pessina G., Pettinacci V., Pira C., Pirro S., Pozzi S., Previtali E., Puiu A., Rosenfeld C., Rusconi C., Sakai M., Sangiorgio S., Schmidt B., Scielzo N.D., Sharma V., Singh V., Sisti M., Speller D., Taffarello L., Terranova F., Tomei C., Vignati M., Wagaarachchi S.L., Wang B.S., Welliver B., Wilson J., Wilson K., Winslow L.A., Zanotti L., Zimmermann S., and Zucchelli S.

Subjects
Particle physics, Bolometers for dark matter research, Physics::Instrumentation and Detectors, trigger algorithm, 01 natural sciences, Coincidence, law.invention, CUORE, WIMP, law, Double beta decay, 0103 physical sciences, General Materials Science, Neutrinoless double beta decay, 010306 general physics, Axion, Physics, 010308 nuclear & particles physics, Scattering, Bolometer, Astrophysics::Instrumentation and Methods for Astrophysics, Trigger algorithms, Condensed Matter Physics, Digital signal processing, Atomic and Molecular Physics, and Optics, Energy (signal processing)
Abstract

CUORE is a tonne-scale cryogenic experiment located at the Laboratori Nazionali del Gran Sasso that exploits bolometric technique to search for neutrinoless double beta decay of 130Te. Thanks to its very low background and large mass, CUORE is also a powerful tool to study a broad class of phenomena, such as solar axions and WIMP scattering. The ability to conduct such sensitive searches crucially depends on the energy threshold, which has to be kept as low as possible. In this contribution, we show how the trigger algorithm affects the sensitivity to low-energy phenomena and the interpretation of the energy spectrum. In particular, we focus on the impact that the trigger algorithm has on the identification of the coincidence events among different crystals and, consequently, on the reconstruction of the background.

Published
2020

48. Status and results from the CUORE experiment

Author

C. Bucci, T. D. Gutierrez, Silvia Capelli, Massimiliano Nastasi, C. Pira, L. Gironi, F. T. Avignone, X. G. Cao, S. Di Domizio, V. Dompè, L. Taffarello, Danielle Speller, L. Cappelli, Laura Cardani, H. Z. Huang, M. Pavan, M. A. Franceschi, B. K. Fujikawa, Stefano Pozzi, Carlo Ligi, C. Pagliarone, Y. Mei, Massimiliano Clemenza, Carlo Cosmelli, Stefano Dell'Oro, A. D’Addabbo, M. Vignati, Lindley Winslow, A. Campani, S. Zucchelli, G. Keppel, K. Wilson, Davide Chiesa, Claudio Gotti, R. G. Huang, M. Faverzani, Jonathan Ouellet, G. Bari, A. Branca, C. Brofferio, L. Ma, Deqing Fang, S. Pirro, C. Rusconi, N. Casali, A. Caminata, Ezio Previtali, S. Zimmermann, S. L. Wagaarachchi, S. Morganti, T. O'Donnell, B. Welliver, K. M. Heeger, G. Fantini, C. Nones, A. Puiu, V. Pettinacci, V. Sharma, D. D'Aguanno, J. Nikkel, N. Chott, Oliviero Cremonesi, Marco Pallavicini, G. Pessina, A. Giuliani, Yu. G. Kolomensky, Ke Han, Reina H. Maruyama, C. Rosenfeld, Stuart J. Freedman, P. Gorla, F. Ferroni, C. Tomei, C. J. Davis, L. Zanotti, Irene Nutini, Evelyn Ferri, Yu-Gang Ma, F. Terranova, N. Moggi, Samuele Sangiorgio, P. T. Surukuchi, A. Nucciotti, L. Pagnanini, C. Alduino, S. Copello, Paolo Carniti, Ettore Fiorini, V. Novati, Andrea Giachero, D. Q. Adams, K. Alfonso, L. Pattavina, N. D. Scielzo, L. Canonica, L. Marini, Vasundhara Singh, J. Johnston, B. Schmidt, B. S. Wang, O. Azzolini, I. Dafinei, M. Sakai, James R. Wilson, F. Bellini, Monica Sisti, R. J. Creswick, Giovanni Benato, Eric B. Norman, T. Napolitano, M. Biassoni, Campani, A, Adams, D, Alduino, C, Alfonso, K, Avignone, F, Azzolini, O, Bari, G, Bellini, F, Benato, G, Biassoni, M, Branca, A, Brofferio, C, Bucci, C, Caminata, A, Canonica, L, Cao, X, Capelli, S, Cappelli, L, Cardani, L, Carniti, P, Casali, N, Chiesa, D, Chott, N, Clemenza, M, Copello, S, Cosmelli, C, Cremonesi, O, Creswick, R, D'Addabbo, A, D'Aguanno, D, Dafinei, I, Davis, C, Dell'Oro, S, Di Domizio, S, Dompe, V, Fang, D, Fantini, G, Faverzani, M, Ferri, E, Ferroni, F, Fiorini, E, Franceschi, M, Freedman, S, Fujikawa, B, Giachero, A, Gironi, L, Giuliani, A, Gorla, P, Gotti, C, Gutierrez, T, Han, K, Heeger, K, Huang, R, Huang, H, Johnston, J, Keppel, G, Kolomensky, Y, Ligi, C, Ma, Y, Ma, L, Marini, L, Maruyama, R, Mei, Y, Moggi, N, Morganti, S, Napolitano, T, Nastasi, M, Nikkel, J, Nones, C, Norman, E, Novati, V, Nucciotti, A, Nutini, I, O'Donnell, T, Ouellet, J, Pagliarone, C, Pagnanini, L, Pallavicini, M, Pattavina, L, Pavan, M, Pessina, G, Pettinacci, V, Pira, C, Pirro, S, Pozzi, S, Previtali, E, Puiu, A, Rosenfeld, C, Rusconi, C, Sakai, M, Sangiorgio, S, Schmidt, B, Scielzo, N, Sharma, V, Singh, V, Sisti, M, Speller, D, Surukuchi, P, Taffarello, L, Terranova, F, Tomei, C, Vignati, M, Wagaarachchi, S, Wang, B, Welliver, B, Wilson, J, Wilson, K, Winslow, L, Zanotti, L, Zimmermann, S, Zucchelli, S, Centre de Sciences Nucléaires et de Sciences de la Matière (CSNSM), Université Paris-Sud - Paris 11 (UP11)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Département de Physique des Particules (ex SPP) (DPhP), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, CUORE, and Département de Physique des Particules (ex SPP) (DPP)

Subjects
Nuclear and High Energy Physics, data analysis method, background: model, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], 01 natural sciences, Combinatorics, CUORE, double-beta decay: (0neutrino), bolometer, 0103 physical sciences, [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], Neutrinoless double beta decay, 010306 general physics, activity report, Physics, 010308 nuclear & particles physics, 29.90.+r, Astronomy and Astrophysics, Background model, Atomic and Molecular Physics, and Optics, tellurium: nuclide, data management, Two-neutrino double beta decay, background model, two-neutrino double beta decay, experimental results
Abstract

Author(s): Campani, A; Adams, DQ; Alduino, C; Alfonso, K; Avignone, FT; Azzolini, O; Bari, G; Bellini, F; Benato, G; Biassoni, M; Branca, A; Brofferio, C; Bucci, C; Caminata, A; Canonica, L; Cao, XG; Capelli, S; Cappelli, L; Cardani, L; Carniti, P; Casali, N; Chiesa, D; Chott, N; Clemenza, M; Copello, S; Cosmelli, C; Cremonesi, O; Creswick, RJ; D'Addabbo, A; D'Aguanno, D; Dafinei, I; Davis, CJ; Dell'oro, S; Di Domizio, S; Dompe, V; Fang, DQ; Fantini, G; Faverzani, M; Ferri, E; Ferroni, F; Fiorini, E; Franceschi, MA; Freedman, SJ; Fujikawa, BK; Giachero, A; Gironi, L; Giuliani, A; Gorla, P; Gotti, C; Gutierrez, TD; Han, K; Heeger, KM; Huang, RG; Huang, HZ; Johnston, J; Keppel, G; Kolomensky, YG; Ligi, C; Ma, YG; Ma, L; Marini, L; Maruyama, RH; Mei, Y; Moggi, N; Morganti, S; Napolitano, T; Nastasi, M; Nikkel, J; Nones, C; Norman, EB; Novati, V; Nucciotti, A; Nutini, I; O'Donnell, T; Ouellet, JL; Pagliarone, CE; Pagnanini, L; Pallavicini, M; Pattavina, L; Pavan, M; Pessina, G; Pettinacci, V; Pira, C; Pirro, S; Pozzi, S | Abstract: The Cryogenic Underground Observatory for Rare Events (CUORE) is a tonne-scale cryogenic experiment located at the Laboratori Nazionali del Gran Sasso that exploits bolometric technique to search for neutrinoless double beta decay (0νββ) of 130Te. The detector consists of a segmented array of 988 natural TeO2 cubic crystals arranged in a cylindrical compact structure of 19 towers. The detector construction was completed in August 2016 and data taking started in Spring 2017. In this work, we present a brief description of the bolometric technique for rare events search and the CUORE detector, then we concentrate on the data analysis results. In this respect, we focus on the procedure for data processing and on the first 0νββ results we obtained from a total TeO2 exposure of 86.3kg yr. Next, we illustrate the main background sources and the CUORE background model, from which we obtain the most precise measurement of 130Te 2νββ half-life to date. Finally, we discuss the improvements achieved with 2018 and 2019 detector optimization campaigns and the current perspectives of our experiment.

Published
2020
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49. Characterization of the low temperature behavior of thin Titanium/Titanium Nitride multilayer films

Author

Renato Mezzena, Benno Margesin, C Giordano, Andrea Giachero, A. Puiu, M. Faverzani, Evelyn Ferri, A. Nucciotti, Faverzani, M, Ferri, E, Giachero, A, Giordano, C, Margesin, B, Mezzena, R, Nucciotti, A, and Puiu, A

Subjects
010302 applied physics, Materials science, Silicon, Transition temperature, Metals and Alloys, chemistry.chemical_element, Nitride, Condensed Matter Physics, 01 natural sciences, Titanium nitride, titanium nitride, multilayers Ti/TiNfilms, resistivity, superconducting transition temperature, proximity effect, chemistry.chemical_compound, chemistry, Electrical resistance and conductance, Electrical resistivity and conductivity, 0103 physical sciences, Materials Chemistry, Ceramics and Composites, Electrical and Electronic Engineering, Composite material, 010306 general physics, Tin, Titanium
Abstract

Titanium and titanium nitride layers were alternately sputtered on a high resistivity silicon wafer to obtain a multilayer film structure, for a total thickness ranging between 34 and 180 nm. The electrical resistance of the Ti/TiN film was characterized from room temperature down to the superconducting transition. Both the resistivity just above the transition and the critical temperature were investigated as a function of the total film thickness and the single TiN layer thickness, respectively. The obtained resistivity range is 67–312 μΩ cm. Exploiting the proximity effect, we were able to tune the critical temperature in the 0.29–4.5 K range. A comparison between experimental data and theoretical models is proposed in order to facilitate the a priori design of superconducting detectors.

Published
2020

50. $$^{163}$$ 163 Ho Distillation and Implantation for HOLMES Experiment

Author

Andrea Giachero, V. Ceriale, Michele Biasotti, A. Nucciotti, Flavio Gatti, Emanuele Ferri, A. Puiu, Angelo Orlando, M. Faverzani, Alessia Provino, Pietro Manfrinetti, M. De Gerone, and G. Gallucci

Subjects
Physics, Q value, Resonance, chemistry.chemical_element, Condensed Matter Physics, 01 natural sciences, Heat capacity, Atomic and Molecular Physics, and Optics, 010305 fluids & plasmas, Section (fiber bundle), Ion implantation, chemistry, Excited state, 0103 physical sciences, General Materials Science, Production (computer science), Atomic physics, 010306 general physics, Holmium
Abstract

HOLMES is an experiment to directly measure the neutrino mass with a calorimetric approach. The calorimetric technique eliminates several systematic uncertainties usually present in spectrometers where the external source and decays to excited states affect the measurement. $$^{163}\hbox {Ho}$$ is chosen as source for its very low Q value (2.8 keV), the proximity of the end-point to resonance M1 and its half life (4570 year). These features are optimal to reach simultaneously a reasonable activity to have sufficient statistics in the end-point and a small quantity of $$^{163}\hbox {Ho}$$ embedded in the detector not to alter significantly its heat capacity. $$^{163}\hbox {Ho}$$ will be produced via neutron irradiation of enriched $$^{162}\hbox {Er}_{2}\hbox {O}_{3}$$ at the Institute Laue–Langevin (Grenoble, France), and chemically separated at Paul Scherrer Institut (Villigen, Switzerland). It will arrive at INFN laboratory of Genova in oxide form ( $$\hbox {Ho}_{2}\hbox {O}_{3}$$ ) with traces of others Ho isotopes and contaminants not removable using chemical methods. In particular, the metastable $$^{166\hbox {m}}\hbox {Ho}$$ undergoes beta decay with a half life of about 1200 year, if present $$^{166\hbox {m}}\hbox {Ho}$$ induces background below 5 keV. The removal of these contaminants is critical for HOLMES so a dedicated system is being set up. The system is designed to achieve an optimal mass separation for $$^{163}\hbox {Ho}$$ and consists of two main components: an evaporation chamber and an ion implanter. In the evaporation chamber, holmium will be reduced in metallic form, using the reaction $$\hbox {2Y+Ho}_{2}\hbox {O}_{3}\rightarrow $$ $$\hbox {Y}_{2}\hbox {O}_{3}\hbox {+2Ho}$$ and used to produce a metallic target for the ion implanter source. The ion implanter consists of five main components: a Penning sputter ion source, an acceleration section, a magnetic/electrostatic mass analyser, a magnetic scanning stage and a focusing electrostatic triplet. In this contribution, we describe the procedures, under continuous refinement, for the holmium evaporation process, the ion-implanted metallic target production and the status of the ion implanter.

Published
2018
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