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Related papers: Calorimeter R&D for the SuperNEMO Double Beta Deca…

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This paper is the first part of the manuscript written in April 2012 for my academic Accreditation to supervise research. It offers a review of the double beta experimental techniques. My purpose is to detail, for each technique, the…

Instrumentation and Detectors · Physics 2012-10-30 Xavier Sarazin

NEXT (Neutrino Experiment with a Xenon TPC) is a neutrinoless double beta decay experiment located at the Laboratorio Subterr\'aneo de Canfranc (LSC, Spain). Its aim is to demonstrate that the neutrino is a Majorana particle by detecting…

Instrumentation and Detectors · Physics 2022-09-21 Carmen Romo-Luque

The lepton number violating process of neutrinoless double-beta decay could result from the physics beyond the Standard Model needed to generate the neutrino masses. Taking different approaches, the current generation of $^{76}$Ge…

Instrumentation and Detectors · Physics 2019-08-14 Jordan Myslik

Spectroscopic studies of two beta-rays from 100Mo are shown to be of potential interest for investigating both the Majorana neutrino mass by neutrinoless double beta-decay and low energy solar neutrino's by inverse beta-decay. With a…

Nuclear Experiment · Physics 2009-10-31 H. Ejiri , J. Engel , R. Hazama , P. Krastev , N. Kudomi , R. G. H. Robertson

The NEMO collaboration is looking to measure neutrinoless double beta decay down to a lower limit of 0.1 eV for the effective neutrino mass. The NEMO 3 detector is now operating in the Frejus Underground Laboratory. The expected performance…

High Energy Physics - Experiment · Physics 2007-05-23 F. Piquemal , NEMO collaboration

The NEMO3 detector, now operating in the Frejus Underground Laboratory, is devoted to search for neutrinoless double beta decay; the expected sensitivity for the effective neutrino mass is on the order of 0.1 eV. The performances of the…

High Energy Physics - Experiment · Physics 2007-05-23 Anne-Isabelle Etienvre

The South Pole Telescope (SPT) has probed an expanded angular range of the CMB temperature power spectrum. Their recent analysis of the latest cosmological data prefers nonzero neutrino masses, mnu = 0.32+-0.11 eV. This result, if confirmed…

High Energy Physics - Phenomenology · Physics 2013-04-01 J. J. Gomez-Cadenas , J. Martin-Albo , J. Muñoz Vidal , C. Peña-Garay

Cryogenic bolometers, with their excellent energy resolution, flexibility in material, and availability in high purity, are excellent detectors for the search for neutrinoless double beta decay. Kilogram-size single crystals of TeO_2 are…

Nuclear Experiment · Physics 2019-08-13 Reina Maruyama

The CUPID-Mo experiment, located at Laboratoire Souterrain de Modane (France), was a demonstrator experiment for CUPID. It consisted of an array of 20 Li$_2^{100}$MoO$_4$ (LMO) calorimeters each equipped with a Ge light detector (LD) for…

The LUMINEU is designed to investigate the possibility to search for neutrinoless double beta decay in $^{100}$Mo by means of a large array of scintillating bolometers based on ZnMoO$_4$ crystals enriched in $^{100}$Mo. High energy…

The full data set of the NEMO-3 experiment has been used to measure the half-life of the two-neutrino double beta decay of $^{100}$Mo to the ground state of $^{100}$Ru, $T_{1/2} = \left[ 6.81 \pm 0.01\,\left(\mbox{stat}\right)…

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

The {\sc Majorana Demonstrator will search for the neutrinoless double-beta decay of the isotope Ge-76 with a mixed array of enriched and natural germanium detectors. The observation of this rare decay would indicate the neutrino is its own…

An approach to developing a feasible neutrinoless double beta decay experiment capable of probing Majorana masses in the regime of the nondegenerate normal neutrino mass hierarchy is proposed. For such an experiment, this study suggests…

Instrumentation and Detectors · Physics 2014-05-15 Steven D Biller

The NEMO-3 results for the double-$\beta$ decay of $^{150}$Nd to the 0$^+_1$ and 2$^+_1$ excited states of $^{150}$Sm are reported. The data recorded during 5.25 yr with 36.6 g of the isotope $^{150}$Nd are used in the analysis. For the…

Current bounds on neutrino Majorana mass are affected by significant uncertainties in the nuclear calculations for neutrinoless double-beta decay. A key issue for a data-driven improvement of the nuclear theory is the actual value of the…

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