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A Neutrino Factory producing an intense beam composed of nu_e(nubar_e) and nubar_mu(nu_mu) from muon decays has been shown to have the greatest sensitivity to the two currently unmeasured neutrino mixing parameters, theta_13 and delta_CP .…

High Energy Physics - Experiment · Physics 2015-03-13 A. Cervera , A. Laing , J. Martin-Albo , F. J. P. Soler

We report the in-situ 3D reconstruction of through-going muons in the CUORE experiment, a cryogenic calorimeter array searching for neutrinoless double beta ($0\nu\beta\beta$) decay, leveraging the segmentation of the detector. Due to the…

Instrumentation and Detectors · Physics 2025-09-09 CUORE Collaboration , D. Q. Adams , C. Alduino , K. Alfonso , A. Armatol , F. T. Avignone , O. Azzolini , G. Bari , F. Bellini , G. Benato , M. Beretta , M. Biassoni , A. Branca , D. Brandani , C. Brofferio , C. Bucci , J. Camilleri , A. Caminata , A. Campani , J. Cao , S. Capelli , L. Cappelli , L. Cardani , P. Carniti , N. Casali , D. Chiesa , Y. Chu , M. Clemenza , S. Copello , O. Cremonesi , R. J. Creswick , A. D'Addabbo , I. Dafinei , S. Dell'Oro , S. Di Domizio , S. Di Lorenzo , T. Dixon , D. Q. Fang , M. Faverzani , E. Ferri , F. Ferroni , E. Fiorini , M. A. Franceschi , S. J. Freedman , S. H. Fu , B. K. Fujikawa , S. Ghislandi , A. Giachero , M. Girola , L. Gironi , A. Giuliani , P. Gorla , C. Gotti , P. V. Guillaumon , T. D. Gutierrez , K. Han , E. V. Hansen , K. M. Heeger , D. L. Helis , H. Z. Huang , M. T. Hurst , G. Keppel , Yu. G. Kolomensky , R. Kowalski , R. Liu , L. Ma , Y. G. Ma , L. Marini , R. H. Maruyama , D. Mayer , M. N. Moore , T. Napolitano , M. Nastasi , C. Nones , E. B. Norman , A. Nucciotti , I. Nutini , T. O'Donnell , M. Olmi , S. Pagan , C. E. Pagliarone , L. Pagnanini , M. Pallavicini , L. Pattavina , M. Pavan , G. Pessina , V. Pettinacci , C. Pira , S. Pirro , E. G. Pottebaum , S. Pozzi , E. Previtali , A. Puiu , S. Puranam , S. Quitadamo , A. Ressa , C. Rosenfeld , B. Schmidt , R. Serino , A. Shaikina , V. Sharma , V. Singh , M. Sisti , D. Speller , P. T. Surukuchi , L. Taffarello , C. Tomei , A. Torres , J. A. Torres , K. J. Vetter , M. Vignati , S. L. Wagaarachchi , R. Wang , B. Welliver , J. Wilson , K. Wilson , L. A. Winslow , F. Xie , T. Zhu , S. Zimmermann , S. Zucchelli

The NO$\nu$A collaboration has constructed a 14,000 ton, fine-grained, low-Z, total absorption tracking calorimeter at an off-axis angle to an upgraded NuMI neutrino beam. This detector, with its excellent granularity and energy resolution…

Instrumentation and Detectors · Physics 2016-01-20 R. Mina , M. J. Frank , E. Fries , R. C. Group , A. Norman , I. Oksuzian

Random coincidences of events could be one of the main sources of background in the search for neutrino-less double-beta decay of $^{100}$Mo with macro-bolometers, due to their modest time resolution. Scintillating bolometers as those based…

The observation of neutrinoless double-beta decay would resolve the Majorana nature of the neutrino and could provide information on the absolute scale of the neutrino mass. The initial phase of the Majorana experiment, known as the…

A radiopure cadmium tungstate crystal scintillator, enriched in $^{106}$Cd to 66%, with mass of 216 g ($^{106}$CdWO$_4$), was used to search for double beta decay processes in $^{106}$Cd in coincidence with four ultra-low background high…

The status and plans of a research program on the development of ultra-low-energy germanium detectors with sub-keV sensitivities are reported. We survey the scientific goals which include the observation of neutrino-nucleus coherent…

High Energy Physics - Experiment · Physics 2008-11-26 Henry T. Wong

The Mu2e experiment at Fermilab will search for the charged lepton flavor violating process of neutrino-less $\mu \to e$ coherent conversion in the field of an aluminum nucleus. Mu2e will reach a single event sensitivity of about $2.5\cdot…

Thermal detectors have recently achieved a leading position in the fields of neutrinoless double beta decay and dark matter searches thanks to excellent energy resolution and numerous absorber material choices. These detectors operate at…

Instrumentation and Detectors · Physics 2011-03-29 Carlo Bucci , Paolo Gorla , Wolfgang Seidel

The correct identification of charged hadrons plays a crucial role in flavor-physics measurements. The final detector configurations at the proposed Future Circular Collider are yet to be determined and this study aims to contribute to this…

High Energy Physics - Experiment · Physics 2026-05-18 Anja Beck , Eluned Smith

SuperNEMO is a double-$\beta$ decay experiment, which will employ the successful tracker-calorimeter technique used in the recently completed NEMO-3 experiment. SuperNEMO will implement 100 kg of double-$\beta$ decay isotope, reaching a…

Composite-fermion models predict excited quarks and leptons with mass scales which can potentially be observed at high-energy colliders like the LHC; the most recent exclusion limits from the CMS and ATLAS Collaborations corner…

High Energy Physics - Phenomenology · Physics 2021-11-02 S. Biondini , S. Dell'Oro , R. Leonardi , S. Marcocci , O. Panella , M. Presilla , F. Vissani

The baseline energy-resolution performance for the current generation of large-mass, low-temperature calorimeters (utilizing TES and NTD sensor technologies) is $>2$ orders of magnitude worse than theoretical predictions. A detailed study…

Instrumentation and Methods for Astrophysics · Physics 2015-03-13 Matt Pyle , Enectali Figueroa-Feliciano , Bernard Sadoulet

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…

Nuclear Experiment · Physics 2018-04-03 CUORE Collaboration , C. Alduino , K. Alfonso , E. Andreotti , C. Arnaboldi , F. T. Avignone , O. Azzolini , I. Bandac , T. I. Banks , G. Bari , M. Barucci , J. W. Beeman , F. Bellini , G. Benato , A. Bersani , D. Biare , M. Biassoni , A. Branca , C. Brofferio , A. Bryant , A. Buccheri , C. Bucci , C. Bulfon , A. Camacho , A. Caminata , L. Canonica , X. G. Cao , S. Capelli , M. Capodiferro , L. Cappelli , L. Cardani , P. Carniti , M. Carrettoni , N. Casali , L. Cassina , G. Ceruti , A. Chiarini , D. Chiesa , N. Chott , M. Clemenza , S. Copello , C. Cosmelli , O. Cremonesi , C. Crescentini , R. J. Creswick , J. S. Cushman , A. D'Addabbo , D. D'Aguanno , I. Dafinei , C. J. Davis , F. Del Corso , S. Dell'Oro , M. M. Deninno , S. Di Domizio , M. L. Di Vacri , L. Di Paolo , A. Drobizhev , L. Ejzak , R. Faccini , 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 , J. Goett , P. Gorla , C. Gotti , C. Guandalini , M. Guerzoni , T. D. Gutierrez , E. E. Haller , K. Han , E. V. Hansen , K. M. Heeger , R. Hennings-Yeomans , K. P. Hickerson , H. Z. Huang , M. Iannone , R. Kadel , G. Keppel , L. Kogler , Yu. G. Kolomensky , A. Leder , C. Ligi , K. E. Lim , Y. G. Ma , C. Maiano , L. Marini , M. Martinez , C. Martinez Amaya , R. H. Maruyama , Y. Mei , N. Moggi , S. Morganti , P. J. Mosteiro , S. S. Nagorny , T. Napolitano , M. Nastasi , C. Nones , E. B. Norman , V. Novati , A. Nucciotti , I. Nutini , T. O'Donnell , E. Olivieri , F. Orio , J. L. Ouellet , C. E. Pagliarone , M. Pallavicini , V. Palmieri , L. Pattavina , M. Pavan , M. Pedretti , A. Pelosi , G. Pessina , V. Pettinacci , G. Piperno , C. Pira , S. Pirro , S. Pozzi , E. Previtali , F. Reindl , F. Rimondi , L. Risegari , C. Rosenfeld , C. Rusconi , M. Sakai , E. Sala , C. Salvioni , S. Sangiorgio , D. Santone , D. Schaeffer , B. Schmidt , J. Schmidt , N. D. Scielzo , V. Singh , M. Sisti , A. R. Smith , F. Stivanello , L. Taffarello , M. Tenconi , F. Terranova , C. Tomei , G. Ventura , M. Vignati , S. L. Wagaarachchi , B. S. Wang , H. W. Wang , B. Welliver , J. Wilson , K. Wilson , L. A. Winslow , T. Wise , L. Zanotti , G. Q. Zhang , B. X. Zhu , S. Zimmermann , S. Zucchelli

Neutrinoless double-beta decay is practically the only way to establish the Majorana nature of the neutrino mass and its decay rate provides a probe of an effective neutrino mass. Double beta experiments are long-running underground…

Nuclear Experiment · Physics 2008-12-08 Oleg Chkvorets

The MAJORANA Collaboration has completed construction and is now operating an array of high purity Ge detectors searching for neutrinoless double-beta decay ($0\nu\beta\beta$) in $^{76}$Ge. The array, known as the MAJORANA DEMONSTRATOR, is…

The NA64 experiment at CERN H4 beamline recently started a high-energy positron-beam program to search for light dark matter particles through a thick-target, missing-energy measurement. To fulfil the energy resolution requirement of the…

Instrumentation and Detectors · Physics 2026-03-24 Andrei Antonov , Pietro Bisio , Mariangela Bondì , Andrea Celentano , Anna Marini , Luca Marsicano

Rare-event search experiments located on-surface, such as short-baseline reactor neutrino experiments, are often limited by muon-induced background events. Highly efficient muon vetos are essential to reduce the detector background and to…

BINGO is a project aiming to set the grounds for large-scale bolometric neutrinoless double-beta-decay experiments capable of investigating the effective Majorana neutrino mass at a few meV level. It focuses on developing innovative…