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Start Over Author "Guandalini, C." Topic physics - instrumentation and detectors
13 results on '"Guandalini, C."'

1. Design and Implementation of the Cosmic Ray Tagger System for the ICARUS detector at FNAL

Author

Aduszkiewicz, A., Bagby, L., Behera, B., Bernardini, P., Bertolucci, S., Betancourt, M., Budd, H., Boone, T., Campos, A., Casazza, D., Cicero, V., Cherdack, D., Coan, T. E., Esposti, L. Degli, Di Ferdinando, D., Di Noto, L., Guandalini, C., Guerzoni, M., Heggestuen, A., Hilgenberg, C., Howell, R., Iliescu, M., Ingratta, G., Kim, T., Kose, U., Laurenti, G., Mariani, C., Mauri, N., McFarland, K. S., Montagna, E., Montanari, A., Moggi, N., Murphy, M., Pasqualini, L., Paolone, V., Patrizii, L., Pellegrini, G., Pia, V., Poppi, F., Pozzato, M., Ruggeri, A., Sala, P., Sapienza, P., Schukraft, A., Sirri, G., Stanco, L., Surdo, A., Tenti, M., Togo, V., Tosi, N., Vicenzi, M., Wilson, R. J., and Zucchelli, S.

Subjects
High Energy Physics - Experiment, Physics - Instrumentation and Detectors
Abstract

The ICARUS-T600 Liquid Argon Time Projection Chamber is operating at Fermilab at shallow depth and thus exposed to a high flux of cosmic rays that can fake neutrino interactions. A cosmic ray tagging (CRT) system ($\sim$1100 m$^2$), surrounding the cryostat with two layers of fiber embedded plastic scintillators, was developed to mitigate the cosmic ray induced background. Using nanosecond-level timing information, the CRT can distinguish incoming cosmic rays from outgoing particles from neutrino interactions in the TPC. In this paper an overview of the CRT system, its installation and commissioning at Fermilab, and its performance are discussed.

Published
2025

2. The Analytical Method algorithm for trigger primitives generation at the LHC Drift Tubes detector

Author

Abbiendi, G., Maestre, J. Alcaraz, Fernández, A. Álvarez, González, B. Álvarez, Amapane, N., Bachiller, I., Barcellan, L., Baldanza, C., Battilana, C., Bellato, M., Bencze, G., Benettoni, M., Beni, N., Benvenuti, A., Bergnoli, A., Ramos, L. C. Blanco, Borgonovi, L., Bragagnolo, A., Cafaro, V., Calderon, A., Calvo, E., Carlin, R., Montoya, C. A. Carrillo, Cavallo, F. R., Ruiz, J. M. Cela, Cepeda, M., Cerrada, M., Checchia, P., Ciano, L., Colino, N., Corti, D., Cotto, G., Crupano, A., Calzada, S. Cuadrado, Cuevas, J., Cuffiani, M., Dallavalle, G. M., Dattola, D., De La Cruz, B., Rodríguez, C. I. de Lara, De Remigis, P., Cid, C. Erice, Eliseev, D., Fabbri, F., Fanfani, A., Fasanella, D., Bedoya, C. F., de Trocóniz, J. F., del Val, D. Fernández, Menéndez, J. Fernández, Ramos, J. P. Fernández, Folgueras, S., Fouz, M. C., Ferrero, D. Francia, Romero, J. García, Gasparini, F., Gasparini, U., Giordano, V., Gonella, F., Caballero, I. González, Fernández, J. R. González, López, O. González, López, S. Goy, Gozzelino, A., Griggio, A., Grosso, G., Guandalini, C., Guiducci, L., Gulmini, M., Hebbeker, T., Hoepfner, K., Isocrate, R., Josa, M. I., Kiani, B., Holgado, J. León, Meo, S. Lo, Lusiani, E., Lunerti, L., Marcellini, S., Margoni, M., Mariotti, C., Martín, I. Martín, Morales, J. J. Martínez, Maselli, S., Masetti, G., Meneguzzo, A. T., Merschmeyer, M., Migliorini, M., Modenese, L., Molnar, J., Montecassiano, F., Martínez, J. Mora, Moran, D., Mukherjee, S., Navarrete, J. J., Navarria, F., Tobar, A. Navarro, Nowotny, F., Cortezón, E. Palencia, Passaseo, M., Pazzini, J., Pelliccioni, M., Perrotta, A., Philipps, B., Gomez, J. Piedra, Primavera, F., Pelayo, J. Puerta, Sánchez, J. C. Puras, Álvarez, C. Ramón, Redondo, I., Ferrero, D. D. Redondo, Reithler, H., Reyes-Almanza, R., Bouza, V. Rodríguez, Ronchese, P., Rossi, A. M., Rossin, R., Rotondo, F., Rovelli, T., Cruz, S. Sánchez, Navas, S. Sánchez, Sastre, J., Sharma, A., Simonetto, F., Rodríguez, A. Soto, Staiano, A., Szillasi, Z., Teyssier, D. F., Toniolo, N., Torromeo, G., Trapote, A., Trevisani, N., Triossi, A., Trocino, D., Ujvari, B., Umoret, G., Gómez, L. Urda, Uwe, B., Ventura, S., Villalba, C. Vico, Wiedenbeck, S., Zanetti, M., Zantis, F. P., Zilizi, G., Zotto, P., and Zucchetta, A.

Subjects
High Energy Physics - Experiment, Physics - Instrumentation and Detectors
Abstract

The Compact Muon Solenoid (CMS) experiment prepares its Phase-2 upgrade for the high-luminosity era of the LHC operation (HL-LHC). Due to the increase of occupancy, trigger latency and rates, the full electronics of the CMS Drift Tube (DT) chambers will need to be replaced. In the new design, the time bin for the digitisation of the chamber signals will be of around 1~ns, and the totality of the signals will be forwarded asynchronously to the service cavern at full resolution. The new backend system will be in charge of building the trigger primitives of each chamber. These trigger primitives contain the information at chamber level about the muon candidates position, direction, and collision time, and are used as input in the L1 CMS trigger. The added functionalities will improve the robustness of the system against ageing. An algorithm based on analytical solutions for reconstructing the DT trigger primitives, called Analytical Method, has been implemented both as a software C++ emulator and in firmware. Its performance has been estimated using the software emulator with simulated and real data samples, and through hardware implementation tests. Measured efficiencies are 96 to 98\% for all qualities and time and spatial resolutions are close to the ultimate performance of the DT chambers. A prototype chain of the HL-LHC electronics using the Analytical Method for trigger primitive generation has been installed during Long Shutdown 2 of the LHC and operated in CMS cosmic data taking campaigns in 2020 and 2021. Results from this validation step, the so-called Slice Test, are presented., Comment: 16 pages, 11 figures

Published
2023
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3. CUORE Opens the Door to Tonne-scale Cryogenics Experiments

Author

CUORE Collaboration, Adams, D. Q., Alduino, C., Alessandria, F., Alfonso, K., Andreotti, E., Avignone III, 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., Dompè, 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, Yu. 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. Martinez, 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., and Zucchelli, S.

Subjects
Physics - Instrumentation and Detectors, Nuclear Experiment
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
2021
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4. Further studies on the physics potential of an experiment using LHC neutrinos

Author

Beni, N., Brucoli, M., Cafaro, V., Cerutti, F., Dallavalle, G. M., Danzeca, S., DeRoeck, A., De Rujula, A., Fasanella, D., Giordano, V., Guandalini, C., Ioannisyan, A., Lazic, D., Margotti, A., Meo, S. Lo, Navarria, F. L., Patrizii, L., Rovelli, T., Sabate-Gilarte, M., Galan, F. Sanchez, Diaz, P. Santos, Sirri, G., Szillasi, Z., and Wulz, C. -E.

Subjects
High Energy Physics - Experiment, High Energy Physics - Phenomenology, Physics - Instrumentation and Detectors
Abstract

We discuss an experiment to investigate neutrino physics at the LHC in Run 3, with emphasis on tau flavour. As described in our previous paper [arXiv:1903.06564v1], the detector can be installed in the decommissioned TI18 tunnel, about 480 m downstream the ATLAS cavern, after the first bending dipoles of the LHC arc. In that location, the prolongation of the beam Line-of-Sight from Interaction Point IP1 to TI18 traverses about 100 m of rock. The detector intercepts the intense neutrino flux, generated by the LHC beams colliding in IP1, at large pseudorapidity eta, where neutrino energies can exceed a TeV. This paper focuses on optimizing global features of the experiment, like detector mass and acceptance. Since the neutrino-nucleon interaction cross section grows almost linearly with energy, the detector can be light and still collect a considerable sample of neutrino events; in the present study it weighs less than 3 tons. The detector is positioned off the beam axis, slightly above the ideal prolongation of the LHC beam from the straight section, covering 7.4 < eta < 9.2. In this configuration, the flux at high energies (0.5-1.5 TeV and beyond) is found to be dominated by neutrinos originating directly from IP1, mostly from charm decays, of which about 50% are electron neutrinos and about 5% are tau neutrinos. The contribution of pion and kaon decays to the muon neutrino flux is studied by means of simulations that embed the LHC optics and found small at high energies. The above studies indicate that with 150 /fb of delivered LHC luminosity in Run 3 the experiment can record a few thousand very high energy neutrino charged current interactions and over 50 tau neutrino charged current events., Comment: 2+20 pages, 15 figures. It is a follow-up of paper arXiv:1903.06564v1 (2019/03/05). arXiv admin note: substantial text overlap with arXiv:1910.11340

Published
2020
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5. Study of the effects of radiation on the CMS Drift Tubes Muon Detector for the HL-LHC

Author

Abbiendi, G., Maestre, J. Alcaraz, Fernández, A. Álvarez, González, B. Álvarez, Amapane, N., Bachiller, I., Barcala, J. M., Barcellan, L., Battilana, C., Bellato, M., Bencze, G., Benettoni, M., Beni, N., Benvenuti, A., Ramos, L. C. Blanco, Boletti, A., Bragagnolo, A., Cifuentes, J. A. Brochero, Cafaro, V., Calderon, A., Calvo, E., Cappati, A., Carlin, R., Montoya, C. A. Carrillo, Cavallo, F. R., Ruiz, J. M. Cela, Cepeda, M., Cerrada, M., Quero, B. Chazin, Checchia, P., Ciano, L., Colino, N., Corti, D., Cotto, G., Cuevas, J., Cuffiani, M., Dallavalle, G. M., Dattola, D., De La Cruz, B., DeRemigis, P., Cid, C. Erice, Fabbri, F., Fanfani, A., Fasanella, D., Bedoya, C. F., de Trocóniz, J. F., Manteca, P. Fernandez, Menéndez, J. Fernández, Ramos, J. P. Fernández, Folgueras, S., Fouz, M. C., Ferrero, D. Francia, Romero, J. García, Gasparini, F., Gasparini, U., Ghosh, S., Giordano, V., Casademunt, F. Gomez, Gonella, F., Caballero, I. González, Fernández, J. R. González, López, O. González, López, S. Goy, Gozzelino, A., Griggio, A., Grosso, G., Guandalini, C., Guiducci, L., Gulmini, M., Hebbeker, T., Heidemann, C., Hernández, J. M., Hoepfner, K., Iemmi, F., Isocrate, R., Josa, M. I., Kiani, B., Lacaprara, S., Meo, S. Lo, Marcellini, S., Margoni, M., Marín, J., Mariotti, C., Martín, I. Martín, Morales, J. J. Martínez, Rivero, C. Martínez, Maselli, S., Masetti, G., Meneguzzo, A. T., Merschmeyer, M., Mocellin, G., Modenese, L., Molinero, A., Molnar, J., Montecassiano, F., Moran, D., Navarrete, J. J., Navarria, F., Tobar, Á. Navarro, Oller, J. C., Passaseo, M., Pazzini, J., Pegoraro, M., Pelayo, J. Puerta, Pelliccioni, M., Philipps, B., Gomez, J. Piedra, Angioni, G. L. Pinna, Pozzobon, N., Presilla, M., Prieels, C., Primavera, F., Sánchez, J. C. Puras, Redondo, I., Ferrero, D. D. Redondo, Reithler, H., Rodrigo, T., Bouza, V. Rodríguez, Roemer, J., Ronchese, P., Rossin, R., Rotondo, F., Rovelli, T., Cruz, S. Sánchez, Navas, S. Sánchez, Sastre, J., Scodellaro, L., Simonetto, F., Soares, M. S., Staiano, A., Szillasi, Z., Teyssier, D. F., Toniolo, N., Torassa, E., Trocino, D., Ujvari, B., Ventura, S., Cortabitarte, R. Vilar, Garcia, J. Vizan, Zanetti, M., Zantis, F. P., Zilizi, G., and Zotto, P.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

The CMS drift tubes (DT) muon detector, built for withstanding the LHC expected integrated and instantaneous luminosities, will be used also in the High Luminosity LHC (HL-LHC) at a 5 times larger instantaneous luminosity and, consequently, much higher levels of radiation, reaching about 10 times the LHC integrated luminosity. Initial irradiation tests of a spare DT chamber at the CERN gamma irradiation facility (GIF++), at large ($\sim$O(100)) acceleration factor, showed ageing effects resulting in a degradation of the DT cell performance. However, full CMS simulations have shown almost no impact in the muon reconstruction efficiency over the full barrel acceptance and for the full integrated luminosity. A second spare DT chamber was moved inside the GIF++ bunker in October 2017. The chamber was being irradiated at lower acceleration factors, and only 2 out of the 12 layers of the chamber were switched at working voltage when the radioactive source was active, being the other layers in standby. In this way the other non-aged layers are used as reference and as a precise and unbiased telescope of muon tracks for the efficiency computation of the aged layers of the chamber, when set at working voltage for measurements. An integrated dose equivalent to two times the expected integrated luminosity of the HL-LHC run has been absorbed by this second spare DT chamber and the final impact on the muon reconstruction efficiency is under study. Direct inspection of some extracted aged anode wires presented a melted resistive deposition of materials. Investigation on the outgassing of cell materials and of the gas components used at the GIF++ are underway. Strategies to mitigate the ageing effects are also being developed. From the long irradiation measurements of the second spare DT chamber, the effects of radiation in the performance of the DTs expected during the HL-LHC run will be presented., Comment: 10 pages, 7 figures, to be published in JINST, editor I. Gonz\'alez Caballero

Published
2019
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6. Physics Potential of an Experiment using LHC Neutrinos

Author

Beni, N., Brucoli, M., Buontempo, S., Cafaro, V., Dallavalle, G . M., Danzeca, S., De Lellis, G., Di Crescenzo, A., Giordano, V., Guandalini, C., Lazic, D., Meo, S. Lo, Navarria, F. L., and Szillasi, Z.

Subjects
High Energy Physics - Experiment, Physics - Instrumentation and Detectors
Abstract

Production of neutrinos is abundant at LHC. Flavour composition and energy reach of the neutrino flux from proton-proton collisions depend on the pseudorapidity $\eta$. At large $\eta$, energies can exceed the TeV, with a sizeable contribution of the $\tau$ flavour. A dedicated detector could intercept this intense neutrino flux in the forward direction, and measure the interaction cross section on nucleons in the unexplored energy range from a few hundred GeV to a few TeV. The high energies of neutrinos result in a larger $\nu$N interaction cross section, and the detector size can be relatively small. Machine backgrounds vary rapidly while moving along and away from the beam line. Four locations were considered as hosts for a neutrino detector: the CMS quadruplet region (~25 m from CMS Interaction Point (IP)), UJ53 and UJ57 (90 and 120 m from CMS IP), RR53 and RR57 (240 m from CMS IP), TI18 (480 m from ATLAS IP). The potential sites are studied on the basis of (a) expectations for neutrino interaction rates, flavour composition and energy spectrum, (b) predicted backgrounds and in-situ measurements, performed with a nuclear emulsion detector and radiation monitors. TI18 emerges as the most favourable location. A small detector in TI18 could measure, for the first time, the high-energy $\nu$N cross section, and separately for $\tau$ neutrinos, with good precision, already with 300 fb$^{-1}$ in the LHC Run3.

Published
2019
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7. First Results from CUORE: A Search for Lepton Number Violation via $0\nu\beta\beta$ Decay of $^{130}$Te

Author

CUORE Collaboration, Alduino, C., Alfonso, K., Andreotti, E., Arnaboldi, C., Avignone III, F. T., Azzolini, O., Bandac, I., Banks, T. I., Bari, G., Barucci, M., Beeman, J. W., Bellini, F., Benato, G., Bersani, A., Biare, D., Biassoni, M., Branca, A., Brofferio, C., Bryant, A., Buccheri, A., Bucci, C., Bulfon, C., Camacho, A., Caminata, A., Canonica, L., Cao, X. G., Capelli, S., Capodiferro, M., Cappelli, L., Cardani, L., Carniti, P., Carrettoni, M., Casali, N., Cassina, L., Ceruti, G., Chiarini, A., Chiesa, D., Chott, N., Clemenza, M., Copello, S., Cosmelli, C., Cremonesi, O., Crescentini, C., Creswick, R. J., Cushman, J. S., D'Addabbo, A., D'Aguanno, D., Dafinei, I., Davis, C. J., Del Corso, F., Dell'Oro, S., Deninno, M. M., Di Domizio, S., Di Vacri, M. L., Di Paolo, L., Drobizhev, A., Ejzak, L., Faccini, R., Fang, D. Q., Faverzani, M., Ferri, E., Ferroni, F., Fiorini, E., Franceschi, M. A., Freedman, S. J., Fujikawa, B. K., Giachero, A., Gironi, L., Giuliani, A., Gladstone, L., Goett, J., Gorla, P., Gotti, C., Guandalini, C., Guerzoni, M., Gutierrez, T. D., Haller, E. E., Han, K., Hansen, E. V., Heeger, K. M., Hennings-Yeomans, R., Hickerson, K. P., Huang, H. Z., Iannone, M., Kadel, R., Keppel, G., Kogler, L., Kolomensky, Yu. G., Leder, A., Ligi, C., Lim, K. E., Ma, Y. G., Maiano, C., Marini, L., Martinez, M., Amaya, C. Martinez, Maruyama, R. H., Mei, Y., Moggi, N., Morganti, S., Mosteiro, P. J., Nagorny, S. S., Napolitano, T., Nastasi, M., Nones, C., Norman, E. B., Novati, V., Nucciotti, A., Nutini, I., O'Donnell, T., Olivieri, E., Orio, F., Ouellet, J. L., Pagliarone, C. E., Pallavicini, M., Palmieri, V., Pattavina, L., Pavan, M., Pedretti, M., Pelosi, A., Pessina, G., Pettinacci, V., Piperno, G., Pira, C., Pirro, S., Pozzi, S., Previtali, E., Reindl, F., Rimondi, F., Risegari, L., Rosenfeld, C., Rusconi, C., Sakai, M., Sala, E., Salvioni, C., Sangiorgio, S., Santone, D., Schaeffer, D., Schmidt, B., Schmidt, J., Scielzo, N. D., Singh, V., Sisti, M., Smith, A. R., Stivanello, F., Taffarello, L., Tenconi, M., Terranova, F., Tomei, C., Ventura, G., Vignati, M., Wagaarachchi, S. L., Wang, B. S., Wang, H. W., Welliver, B., Wilson, J., Wilson, K., Winslow, L. A., Wise, T., Zanotti, L., Zhang, G. Q., Zhu, B. X., Zimmermann, S., and Zucchelli, S.

Subjects
Nuclear Experiment, High Energy Physics - Experiment, Physics - Instrumentation and Detectors
Abstract

The CUORE experiment, a ton-scale cryogenic bolometer array, recently began operation at the Laboratori Nazionali del Gran Sasso in Italy. The array represents a significant advancement in this technology, and in this work we apply it for the first time to a high-sensitivity search for a lepton-number--violating process: $^{130}$Te neutrinoless double-beta decay. Examining a total TeO$_2$ exposure of 86.3 kg$\cdot$yr, characterized by an effective energy resolution of (7.7 $\pm$ 0.5) keV FWHM and a background in the region of interest of (0.014 $\pm$ 0.002) counts/(keV$\cdot$kg$\cdot$yr), we find no evidence for neutrinoless double-beta decay. The median statistical sensitivity of this search is $7.0\times10^{24}$ yr. Including systematic uncertainties, we place a lower limit on the decay half-life of $T^{0\nu}_{1/2}$($^{130}$Te) > $1.3\times 10^{25}$ yr (90% C.L.). Combining this result with those of two earlier experiments, Cuoricino and CUORE-0, we find $T^{0\nu}_{1/2}$($^{130}$Te) > $1.5\times 10^{25}$ yr (90% C.L.), which is the most stringent limit to date on this decay. Interpreting this result as a limit on the effective Majorana neutrino mass, we find $m_{\beta\beta}<(110 - 520)$ meV, where the range reflects the nuclear matrix element estimates employed., Comment: Published in PRL, reference and DOI added

Published
2017
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8. Search for anomalies in the neutrino sector with muon spectrometers and large LArTPC imaging detectors at CERN

Author

Antonello, M., Bagliani, D., Baibussinov, B., Bilokon, H., Boffelli, F., Bonesini, M., Calligarich, E., Canci, N., Centro, S., Cesana, A., Cieslik, K., Cline, D. B., Cocco, A. G., Dequal, D., Dermenev, A., Dolfini, R., De Gerone, M., Dussoni, S., Farnese, C., Fava, A., Ferrari, A., Fiorillo, G., Garvey, G. T., Gatti, F., Gibin, D., Gninenko, S., Guber, F., Guglielmi, A., Haranczyk, M., Holeczek, J., Ivashkin, A., Kirsanov, M., Kisiel, J., Kochanek, I., Kurepin, A., Lagoda, J., Lucchini, G., Louis, W. C., Mania, S., Mannocchi, G., Marchini, S., Matveev, V., Menegolli, A., Meng, G., Mills, G. B., Montanari, C., Nicoletto, M., Otwinowski, S., Palczewki, T. J., Passardi, G., Perfetto, F., Picchi, P., Pietropaolo, F., Plonski, P., Rappoldi, A., Raselli, G. L., Rossella, M., Rubbia, C., Sala, P., Scaramelli, A., Segreto, E., Stefan, D., Stepaniak, J., Sulej, R., Suvorova, O., Terrani, M., Tlisov, D., Van de Water, R. G., Trinchero, G., Turcato, M., Varanini, F., Ventura, S., Vignoli, C., Wang, H. G., Yang, X., Zani, A., Zaremba, K, Benettoni, M., Bernardini, P., Bertolin, A., Brugnera, R., Calabrese, M., Cecchetti, A., Cecchini, S., Collazuol, G., Creti, P., Corso, F. Dal, Del Prete, A., De Mitri, I., De Robertis, G., De Serio, M., Esposti, L. Degli, Di Ferdinando, D., Dore, U., Dusini, S., Fabbricatore, P., Fanin, C., Fini, R. A., Fiore, G., Garfagnini, A., Giacomelli, G., Giacomelli, R., Guandalini, C., Guerzoni, M., Kose, U., Laurenti, G., Laveder, M., Lippi, I., Loddo, F., Longhin, A., Loverre, P., Mancarella, G., Mandrioli, G., Margiotta, A., Marsella, G., Mauri, N., Medinaceli, E., Mengucci, A., Mezzetto, M., Michinelli, R., Muciaccia, M. T., Orecchini, D., Paoloni, A., Papadia, G., Pastore, A., Patrizii, L., Pozzato, M., Rosa, G., Sahnounm, Z., Simone, S., Sioli, M., Sirri, G., Spurio, M., Stanco, L., Surdo, A., Tenti, M., Togo, V., Ventura, M., and Zago, M.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment, High Energy Physics - Phenomenology
Abstract

A new experiment with an intense ~2 GeV neutrino beam at CERN SPS is proposed in order to definitely clarify the possible existence of additional neutrino states, as pointed out by neutrino calibration source experiments, reactor and accelerator experiments and measure the corresponding oscillation parameters. The experiment is based on two identical LAr-TPCs complemented by magnetized spectrometers detecting electron and muon neutrino events at Far and Near positions, 1600 m and 300 m from the proton target, respectively. The ICARUS T600 detector, the largest LAr-TPC ever built with a size of about 600 ton of imaging mass, now running in the LNGS underground laboratory, will be moved at the CERN Far position. An additional 1/4 of the T600 detector (T150) will be constructed and located in the Near position. Two large area spectrometers will be placed downstream of the two LAr-TPC detectors to perform charge identification and muon momentum measurements from sub-GeV to several GeV energy range, greatly complementing the physics capabilities. This experiment will offer remarkable discovery potentialities, collecting a very large number of unbiased events both in the neutrino and antineutrino channels, largely adequate to definitely settle the origin of the observed neutrino-related anomalies., Comment: Contribution to the European Strategy for Particle Physics - Open Symposium Preparatory Group, Kracow 10-12 September 2012

Published
2012

9. Search for 'anomalies' from neutrino and anti-neutrino oscillations at Delta_m^2 ~ 1eV^2 with muon spectrometers and large LAr-TPC imaging detectors

Author

Antonello, M., Bagliani, D., Baibussinov, B., Bilokon, H., Boffelli, F., Bonesini, M., Calligarich, E., Canci, N., Centro, S., Cesana, A., Cieslik, K., Cline, D. B., Cocco, A. G., Dequal, D., Dermenev, A., Dolfini, R., De Gerone, M., Dussoni, S., Farnese, C., Fava, A., Ferrari, A., Fiorillo, G., Garvey, G. T., Gatti, F., Gibin, D., Gninenko, S., Guber, F., Guglielmi, A., Haranczyk, M., Holeczek, J., Ivashkin, A., Kirsanov, M., Kisiel, J., Kochanek, I., Kurepin, A., Łagoda, J., Lucchini, G., Louis, W. C., Mania, S., Mannocchi, G., Marchini, S., Matveev, V., Menegolli, A., Meng, G., Mills, G. B., Montanari, C., Nicoletto, M., Otwinowski, S., Palczewski, T. J., Passardi, G., Perfetto, F., Picchi, P., Pietropaolo, F., Płoński, P., Rappoldi, A., Raselli, G. L., Rossella, M., Rubbia, C., Sala, P., Scaramelli, A., Segreto, E., Stefan, D., Stepaniak, J., Sulej, R., Suvorova, O., Terrani, M., Tlisov, D., Van de Water, R. G., Trinchero, G., Turcato, M., Varanini, F., Ventura, S., Vignoli, C., Wang, H. G., Yang, X., Zani, A., Zaremba, K., Benettoni, M., Bernardini, P., Bertolin, A., Bozza, C., Brugnera, R., Cecchetti, A., Cecchini, S., Collazuol, G., Creti, P., Corso, F. Dal, De Mitri, I., De Robertis, G., De Serio, M., Esposti, L. Degli, Di Ferdinando, D., Dore, U., Dusini, S., Fabbricatore, P., Fanin, C., Fini, R. A., Fiore, G., Garfagnini, A., Giacomelli, G., Giacomelli, R., Grelli, G., Guandalini, C., Guerzoni, M., Kose, U., Laurenti, G., Laveder, M., Lippi, I., Loddo, F., Longhin, A., Loverre, P., Mancarella, G., Mandrioli, G., Margiotta, A., Marsella, G., Mauri, N., Medinaceli, E., Mengucci, A., Mezzetto, M., Michinelli, R., Muciaccia, M. T., Orecchini, D., Paoloni, A., Pastore, A., Patrizii, L., Pozzato, M., Rescigno, R., Rosa, G., Simone, S., Sioli, M., Sirri, G., Spurio, M., Stanco, L., Stellacci, S., Surdo, A., Tenti, M., Togo, V., Ventura, M., and Zago, M.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

This proposal describes an experimental search for sterile neutrinos beyond the Standard Model with a new CERN-SPS neutrino beam. The experiment is based on two identical LAr-TPC's followed by magnetized spectrometers, observing the electron and muon neutrino events at 1600 and 300 m from the proton target. This project will exploit the ICARUS T600, moved from LNGS to the CERN "Far" position. An additional 1/4 of the T600 detector will be constructed and located in the "Near" position. Two spectrometers will be placed downstream of the two LAr-TPC detectors to greatly complement the physics capabilities. Spectrometers will exploit a classical dipole magnetic field with iron slabs, and a new concept air-magnet, to perform charge identification and muon momentum measurements in a wide energy range over a large transverse area. In the two positions, the radial and energy spectra of the nu_e beam are practically identical. Comparing the two detectors, in absence of oscillations, all cross sections and experimental biases cancel out, and the two experimentally observed event distributions must be identical. Any difference of the event distributions at the locations of the two detectors might be attributed to the possible existence of {\nu}-oscillations, presumably due to additional neutrinos with a mixing angle sin^2(2theta_new) and a larger mass difference Delta_m^2_new. The superior quality of the LAr imaging TPC, in particular its unique electron-pi_zero discrimination allows full rejection of backgrounds and offers a lossless nu_e detection capability. The determination of the muon charge with the spectrometers allows the full separation of nu_mu from anti-nu_mu and therefore controlling systematics from muon mis-identification largely at high momenta., Comment: Experiment proposal

Published
2012

10. First Results from CUORE: A Search for Lepton Number Violation via $0\nu\beta\beta$ Decay of $^{130}$Te

Author

CUORE Collaboration, Alduino, C., Alfonso, K., Andreotti, E., Arnaboldi, C., Avignone III, F. T., Azzolini, O., Bandac, I., Banks, T. I., Bari, G., Barucci, M., Beeman, J. W., Bellini, F., Benato, G., Bersani, A., Biare, D., Biassoni, M., Branca, A., Brofferio, C., Bryant, A., Buccheri, A., Bucci, C., Bulfon, C., Camacho, A., Caminata, A., Canonica, L., Cao, X. G., Capelli, S., Capodiferro, M., Cappelli, L., Cardani, L., Carniti, P., Carrettoni, M., Casali, N., Cassina, L., Ceruti, G., Chiarini, A., Chiesa, D., Chott, N., Clemenza, M., Copello, S., Cosmelli, C., Cremonesi, O., Crescentini, C., Creswick, R. J., Cushman, J. S., D'Addabbo, A., D'Aguanno, D., Dafinei, I., Davis, C. J., Del Corso, F., Dell'Oro, S., Deninno, M. M., Di Domizio, S., Di Vacri, M. L., Di Paolo, L., Drobizhev, A., Ejzak, L., Faccini, R., Fang, D. Q., Faverzani, M., Ferri, E., Ferroni, F., Fiorini, E., Franceschi, M. A., Freedman, S. J., Fujikawa, B. K., Giachero, A., Gironi, L., Giuliani, A., Gladstone, L., Goett, J., Gorla, P., Gotti, C., Guandalini, C., Guerzoni, M., Gutierrez, T. D., Haller, E. E., Han, K., Hansen, E. V., Heeger, K. M., Hennings-Yeomans, R., Hickerson, K. P., Huang, H. Z., Iannone, M., Kadel, R., Keppel, G., Kogler, L., Kolomensky, Yu. G., Leder, A., Ligi, C., Lim, K. E., Ma, Y. G., Maiano, C., Marini, L., Martinez, M., Amaya, C. Martinez, Maruyama, R. H., Mei, Y., Moggi, N., Morganti, S., Mosteiro, P. J., Nagorny, S. S., Napolitano, T., Nastasi, M., Nones, C., Norman, E. B., Novati, V., Nucciotti, A., Nutini, I., O'Donnell, T., Olivieri, E., Orio, F., Ouellet, J. L., Pagliarone, C. E., Pallavicini, M., Palmieri, V., Pattavina, L., Pavan, M., Pedretti, M., Pelosi, A., Pessina, G., Pettinacci, V., Piperno, G., Pira, C., Pirro, S., Pozzi, S., Previtali, E., Reindl, F., Rimondi, F., Risegari, L., Rosenfeld, C., Rusconi, C., Sakai, M., Sala, E., Salvioni, C., Sangiorgio, S., Santone, D., Schaeffer, D., Schmidt, B., Schmidt, J., Scielzo, N. D., Singh, V., Sisti, M., Smith, A. R., Stivanello, F., Taffarello, L., Tenconi, M., Terranova, F., Tomei, C., Ventura, G., Vignati, M., Wagaarachchi, S. L., Wang, B. S., Wang, H. W., Welliver, B., Wilson, J., Wilson, K., Winslow, L. A., Wise, T., Zanotti, L., Zhang, G. Q., Zhu, B. X., 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) (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, Département de Physique des Particules (ex SPP) (DPhP), 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) ( DPP ), 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-Commissariat à l'énergie atomique et aux énergies alternatives ( CEA ) -Université Paris-Saclay

Subjects
double-beta decay: neutrinoless, Physics - Instrumentation and Detectors, energy resolution, [PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex], High Energy Physics - Experiment, background: low, double-beta decay: (0neutrino), bolometer, [ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex], [PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex], [PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], [ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex], Nuclear Experiment, [ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det], lepton number: violation, S076H0N, CUORE, background, nucleus, neutrino: Majorana: mass, sensitivity, Gran Sasso, Automatic Keywords, cryogenics, S076MW, statistical, experimental results
Abstract

The CUORE experiment, a ton-scale cryogenic bolometer array, recently began operation at the Laboratori Nazionali del Gran Sasso in Italy. The array represents a significant advancement in this technology, and in this work we apply it for the first time to a high-sensitivity search for a lepton-number--violating process: $^{130}$Te neutrinoless double-beta decay. Examining a total TeO$_2$ exposure of 86.3 kg$\cdot$yr, characterized by an effective energy resolution of (7.7 $\pm$ 0.5) keV FWHM and a background in the region of interest of (0.014 $\pm$ 0.002) counts/(keV$\cdot$kg$\cdot$yr), we find no evidence for neutrinoless double-beta decay. The median statistical sensitivity of this search is $7.0\times10^{24}$ yr. Including systematic uncertainties, we place a lower limit on the decay half-life of $T^{0\nu}_{1/2}$($^{130}$Te) > $1.3\times 10^{25}$ yr (90% C.L.). Combining this result with those of two earlier experiments, Cuoricino and CUORE-0, we find $T^{0\nu}_{1/2}$($^{130}$Te) > $1.5\times 10^{25}$ yr (90% C.L.), which is the most stringent limit to date on this decay. Interpreting this result as a limit on the effective Majorana neutrino mass, we find $m_{\beta\beta}, Comment: Published in PRL, reference and DOI added

Published
2018
Full Text
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11. Search for anomalies in the neutrino sector with muon spectrometers and large LArTPC imaging detectors at CERN

Author

Antonello, A., Bagliani, D., Baibussinov, B., Bilokon, H., Boffelli, F., Bonesini, M., Calligarich, E., Canci, N., Centro, Sandro, Cesana, A., Cieslik, K., Cline, D. B., Cocco, A. G., Dequal, D., Dermenev, A., Dolfini, R., Gerone, M. D., Dussoni, S., Farnese, C., Fava, Angela, Ferrari, A., Fiorillo, G., Garvey, G. T., Gatti, F., Daniele Gibin, Gninenko, S., Guber, F., Guglielmi, A., Haranczyk, M., Holeczek, J., Ivashkin, A., Kirsanov, M., Kisiel, J., Kochanek, I., Kurepin, A., Lagoda, J., Lucchini, G., Louis, W. C., Mania, S., Mannocchi, G., Marchini, S., Matveev, V., Menegolli, A., Meng, G., Mills, G. B., Montanari, C., Nicoletto, M., Otwinowski, S., Palczewki, T. J., Passardi, G., Perfetto, F., Picchi, P., Pietropaolo, F., Plonski, P., Rappoldi, A., Raselli, G. L., Rossella, M., Rubbia, C., Sala, P., Scaramelli, A., Segreto, E., Stefan, D., Stepaniak, J., Sulej, R., Suvorova, O., Terrani, M., Tlisov, D., Van, R. G., Trinchero, G., Turcato, M., Varanini, F., Ventura, Sandro, Vignoli, C., Wang, H. G., Yang, X., Zani, A., Zaremba, K., Benettoni, M., Bernardini, P., Bertolin, A., Riccardo Brugnera, Calabrese, M., Cecchetti, A., Cecchini, S., Gianmaria Collazuol, Creti, P., Corso, F. D., Prete, A. D., Mitri, I. D., Robertis, G. D., Serio, M. D., Esposti, L. D., Ferdinando, D. D., Dore, U., Dusini, S., Fabbricatore, P., Fanin, C., Fini, R. A., Fiore, G., Alberto Garfagnini, Giacomelli, G., Giacomelli, R., Guandalini, C., Guerzoni, M., Kose, U., Laurenti, G., Marco Laveder, Lippi, I., Loddo, F., Longhin, A., Loverre, P., Mancarella, G., Mandrioli, G., Margiotta, A., Marsella, G., Mauri, N., Eduardo Medinaceli, Mengucci, A., Mezzetto, M., Michinelli, R., Muciaccia, M. T., Orecchini, D., Paoloni, A., Papadia, G., Pastore, A., Patrizii, L., Pozzato, M., Rosa, G., Sahnounm, Z., Simone, S., Sioli, M., Sirri, G., Spurio, M., Stanco, L., Surdo, A., Tenti, M., Togo, V., Ventura, M., and Zago, M.

Subjects
High Energy Physics - Experiment (hep-ex), High Energy Physics - Phenomenology, High Energy Physics - Phenomenology (hep-ph), Physics - Instrumentation and Detectors, Physics::Instrumentation and Detectors, FOS: Physical sciences, High Energy Physics::Experiment, Instrumentation and Detectors (physics.ins-det), Nuclear Experiment, High Energy Physics - Experiment, Particle Physics - Phenomenology
Abstract

A new experiment with an intense ~2 GeV neutrino beam at CERN SPS is proposed in order to definitely clarify the possible existence of additional neutrino states, as pointed out by neutrino calibration source experiments, reactor and accelerator experiments and measure the corresponding oscillation parameters. The experiment is based on two identical LAr-TPCs complemented by magnetized spectrometers detecting electron and muon neutrino events at Far and Near positions, 1600 m and 300 m from the proton target, respectively. The ICARUS T600 detector, the largest LAr-TPC ever built with a size of about 600 ton of imaging mass, now running in the LNGS underground laboratory, will be moved at the CERN Far position. An additional 1/4 of the T600 detector (T150) will be constructed and located in the Near position. Two large area spectrometers will be placed downstream of the two LAr-TPC detectors to perform charge identification and muon momentum measurements from sub-GeV to several GeV energy range, greatly complementing the physics capabilities. This experiment will offer remarkable discovery potentialities, collecting a very large number of unbiased events both in the neutrino and antineutrino channels, largely adequate to definitely settle the origin of the observed neutrino-related anomalies., Contribution to the European Strategy for Particle Physics - Open Symposium Preparatory Group, Kracow 10-12 September 2012

12. 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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13. Physics Potential of an Experiment using LHC Neutrinos

Author

Gaetano-Marco Dallavalle, V. Cafaro, Noemi Beni, S. Buontempo, C. Guandalini, Francesco Navarria, D. Lazic, S. Lo Meo, S. Danzeca, A. Di Crescenzo, G. De Lellis, V. Giordano, M. Brucoli, Z. Szillasi, Beni, N, Brucoli, M, Buontempo, S, Cafaro, V, Dallavalle, G M, Danzeca, S, Lellis, G De, Crescenzo, A Di, Giordano, V, Guandalini, C, Lazic, D, Meo, S Lo, Navarria, F L, and Szillasi, Z

Subjects
Nuclear and High Energy Physics, Particle physics, Physics - Instrumentation and Detectors, Physics::Instrumentation and Detectors, Astrophysics::High Energy Astrophysical Phenomena, FOS: Physical sciences, 01 natural sciences, High Energy Physics - Experiment, High Energy Physics - Experiment (hep-ex), 0103 physical sciences, Nuclear emulsion, Detectors and Experimental Techniques, 010306 general physics, physics.ins-det, Physics, Large Hadron Collider, Interaction point, 010308 nuclear & particles physics, hep-ex, Computer Science::Information Retrieval, Detector, High Energy Physics::Phenomenology, Instrumentation and Detectors (physics.ins-det), Neutrino detector, Pseudorapidity, High Energy Physics::Experiment, Neutrino, Nucleon, Particle Physics - Experiment
Abstract

Production of neutrinos is abundant at LHC. Flavour composition and energy reach of the neutrino flux from proton-proton collisions depend on the pseudorapidity $\eta$. At large $\eta$, energies can exceed the TeV, with a sizeable contribution of the $\tau$ flavour. A dedicated detector could intercept this intense neutrino flux in the forward direction, and measure the interaction cross section on nucleons in the unexplored energy range from a few hundred GeV to a few TeV. The high energies of neutrinos result in a larger $\nu$N interaction cross section, and the detector size can be relatively small. Machine backgrounds vary rapidly while moving along and away from the beam line. Four locations were considered as hosts for a neutrino detector: the CMS quadruplet region (~25 m from CMS Interaction Point (IP)), UJ53 and UJ57 (90 and 120 m from CMS IP), RR53 and RR57 (240 m from CMS IP), TI18 (480 m from ATLAS IP). The potential sites are studied on the basis of (a) expectations for neutrino interaction rates, flavour composition and energy spectrum, (b) predicted backgrounds and in-situ measurements, performed with a nuclear emulsion detector and radiation monitors. TI18 emerges as the most favourable location. A small detector in TI18 could measure, for the first time, the high-energy $\nu$N cross section, and separately for $\tau$ neutrinos, with good precision, already with 300 fb$^{-1}$ in the LHC Run3. Neutrinos are abundantly produced in the LHC. Flavour composition and energy reach of the neutrino flux from proton–proton collisions depend on the pseudorapidity η. At large η, energies can exceed the TeV, with a sizeable contribution of the τ flavour. A dedicated detector could intercept this intense neutrino flux in the forward direction, and measure the interaction cross section on nucleons in the unexplored energy range from a few hundred GeV to a few TeV. The high energies of neutrinos result in a larger νN interaction cross section, and the detector size can be relatively small. Machine backgrounds vary rapidly while moving along and away from the beam line. Four locations were considered as hosts for a neutrino detector: the CMS quadrupole region (25 m from CMS Interaction Point (IP)), UJ53 and UJ57 (90 and 120 m from CMS IP), RR53 and RR57 (240 m from CMS IP), TI18 (480 m from ATLAS IP). The potential sites are studied on the basis of (a) expectations for neutrino interaction rates, flavour composition and energy spectrum, (b) predicted backgrounds and in situ measurements, performed with a nuclear emulsion detector and radiation monitors. TI18 emerges as the most favourable location. Already with 150 fb−1 expected in LHC Run3, a small detector in TI18 could measure, for the first time and with good precision, the high-energy νN cross section for all neutrino flavours. Production of neutrinos is abundant at LHC. Flavour composition and energy reach of the neutrino flux from proton-proton collisions depend on the pseudorapidity $\eta$. At large $\eta$, energies can exceed the TeV, with a sizeable contribution of the $\tau$ flavour. A dedicated detector could intercept this intense neutrino flux in the forward direction, and measure the interaction cross section on nucleons in the unexplored energy range from a few hundred GeV to a few TeV. The high energies of neutrinos result in a larger $\nu$N interaction cross section, and the detector size can be relatively small. Machine backgrounds vary rapidly while moving along and away from the beam line. Four locations were considered as hosts for a neutrino detector: the CMS quadruplet region (~25 m from CMS Interaction Point (IP)), UJ53 and UJ57 (90 and 120 m from CMS IP), RR53 and RR57 (240 m from CMS IP), TI18 (480 m from ATLAS IP). The potential sites are studied on the basis of (a) expectations for neutrino interaction rates, flavour composition and energy spectrum, (b) predicted backgrounds and in-situ measurements, performed with a nuclear emulsion detector and radiation monitors. TI18 emerges as the most favourable location. A small detector in TI18 could measure, for the first time, the high-energy $\nu$N cross section, and separately for $\tau$ neutrinos, with good precision, already with 300 fb$^{-1}$ in the LHC Run3.

Published
2019

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