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Related papers: A multi-isotope $0\nu2\beta$ bolometric experiment

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We consider the scheme with mixing of three neutrinos and a mass hierarchy. We shown that, under the natural assumptions that massive neutrinos are Majorana particles and there are no unlikely fine-tuned cancellations among the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Carlo Giunti

The neutrinoless double beta ($0\nu\beta\beta$) decay process could provide crucial information to determine the absolute scale of the neutrino masses, and it is the only one that can establish whether neutrino is a Dirac or a Majorana…

Nuclear Theory · Physics 2010-05-12 Mihai Horoi , Sabin Stoica

The recent neutrino oscillation experimental results indicate that at least one neutrino has a mass greater than 50 meV. The next generation of double-beta decay experiments will very likely have a sensitivity to an effective Majorana…

Nuclear Experiment · Physics 2011-07-19 Steven R. Elliott

We have studied the constraints imposed by the results of neutrino oscillation experiments on the effective Majorana mass |<m>| that characterizes the contribution of Majorana neutrino masses to the matrix element of neutrinoless…

High Energy Physics - Phenomenology · Physics 2016-08-25 S. M. Bilenky , C. Giunti , C. W. Kim , M. Monteno

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…

We describe in detail the methods used to obtain the lower bound on the lifetime of neutrinoless double-beta ($0\nu\beta\beta$) decay in $^{130}$Te and the associated limit on the effective Majorana mass of the neutrino using the CUORE-0…

Nuclear Experiment · Physics 2016-04-28 CUORE Collaboration , C. Alduino , K. Alfonso , D. R. Artusa , F. T. Avignone , O. Azzolini , T. I. Banks , G. Bari , J. W. Beeman , F. Bellini , A. Bersani , M. Biassoni , C. Brofferio , C. Bucci , 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 , I. Dafinei , A. Dally , 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 , 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 , 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 , 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 , S. Pirro , S. Pozzi , E. Previtali , C. Rosenfeld , C. Rusconi , E. Sala , S. Sangiorgio , D. Santone , N. D. Scielzo , V. Singh , M. Sisti , A. R. Smith , L. Taffarello , M. Tenconi , F. Terranova , C. Tomei , S. Trentalange , G. Ventura , 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 , S. Zucchelli

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…

The observation of neutrinoless double-beta ($0\nu\beta\beta$) decay would offer proof of lepton number violation, demonstrating that neutrinos are Majorana particles, while also helping us understand why there is more matter than…

The $(\beta ^{+}\beta ^{+})_{0\nu}$ and $(\varepsilon \beta ^{+})_{0\nu}$ modes of $^{96}$Ru, $^{102}$Pd, $^{106}$Cd, $^{124}$Xe, $^{130}$Ba and $^{156}$Dy isotopes are studied in the Projected Hartree-Fock-Bogoliubov framework for the…

Nuclear Theory · Physics 2009-11-06 P. K. Rath , R. Chandra , K. Chaturvedi , P. K. Raina , J. G. Hirsch

A new generation of neutrinoless double beta decay experiments with improved sensitivity is currently under design and construction. They will probe inverted hierarchy region of the neutrino mass pattern. There is also a revived interest to…

Nuclear Theory · Physics 2015-06-05 Amand Faessler , Vadim Rodin , Fedor Simkovic

Study of the neutrinoless $\beta\beta$ decay allows us to put a stringent limit on the effective neutrino Majorana mass, a quantity of fundamental importance. To test our ability to evaluate the nuclear matrix elements that govern the decay…

Nuclear Theory · Physics 2007-05-23 Petr Vogel

The aim of the NEMO 3 experiment is the search for neutrinoless double beta decay and precise measurement of two-neutrino double beta decay of several isotopes. The experiment has been taking data since 2003. Since no evidence for…

High Energy Physics - Experiment · Physics 2019-08-13 Ladislav Vala

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…

The study of neutrinoless double beta decay is of outmost importance for neutrino physics. It is considered to be the gold plated channel to probe the fundamental character of neutrinos and to determine the neutrino mass. From the…

Nuclear Experiment · Physics 2008-11-26 K. Zuber

The NEMO-3 experiment is searching for neutrinoless double beta decay for 2 main isotopes (100Mo and 82Se) and is studying the two-neutrino double beta decay of seven isotopes. The experiment has been taking data since 2003 and, up to the…

High Energy Physics - Experiment · Physics 2019-08-14 Mathieu BONGRAND

The Majorana Collaboration is assembling an array of HPGe detectors to search for neutrinoless double-beta decay in Ge-76. Initially, Majorana aims to construct a prototype module to demonstrate the potential of a future 1-tonne experiment.…

Nuclear Experiment · Physics 2019-08-13 V. E. Guiseppe

Neutrinoless double beta decay is a promising test for lepton number violating physics beyond the standard model of particle physics. There is a deep connection between this decay and the phenomenon of neutrino masses. In particular, we…

High Energy Physics - Phenomenology · Physics 2012-07-30 Michael Duerr

The search for neutrinoless double beta decay probes lepton number conservation with high sensitivity and investigates the neutrino nature and mass scale. Experiments presently in preparation will cover the quasi-degeneracy region of the…

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…

CUPID-0, an array of Zn$^{82}$Se cryogenic calorimeters, was the first medium-scale demonstrator of the scintillating bolometers technology. The first project phase (March 2017 - December 2018) allowed the most stringent limit on the…

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