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Neutrinoless double-beta decay (0$\nu\beta\beta$) decay is a hypothetical process that violates lepton number, and whose observation would unambiguously indicate that neutrinos are Majorana fermions. In the standard inverted-ordering…

Nuclear Experiment · Physics 2019-12-10 J. M. López-Castaño , I. Guinn

The next generation of double-beta decay experiments have an excellent chance of providing data on the neutrino mass pattern. This presentation is a summary of what is currently known about the mass pattern and expectations from experiment.…

Nuclear Experiment · Physics 2015-06-26 Steven R. Elliott

The most stringent constraint on the so-called effective electron neutrino mass from the present neutrinoless double beta decay experiments is |M_{ee}| < 0.2 eV, while the planned next generation experiment GENIUS is anticipated to reach a…

High Energy Physics - Phenomenology · Physics 2009-10-31 Anna Kalliomaki , Jukka Maalampi

We present accurate predictions of the effective Majorana mass $|m_{\beta\beta}|$ in neutrinoless double-$\beta$ decay in the standard case of $3\nu$ mixing and in the case of 3+1 neutrino mixing indicated by the reactor, Gallium and LSND…

High Energy Physics - Phenomenology · Physics 2015-09-02 C. Giunti , E. M. Zavanin

All existing data on neutrino oscillations (including those from the LSND experiment) imply a four neutrino scheme with six different allowed mass patterns. Some of the latter are shown to be disfavored by using a conservative upper bound…

High Energy Physics - Phenomenology · Physics 2009-11-07 Sandip Pakvasa , Probir Roy

Assuming mixing of three massive Majorana neutrinos, we study the implications of the neutrino oscillation solutions of the solar and atmospheric neutrino problems and of the results of the CHOOZ experiment for the predictions of the…

High Energy Physics - Phenomenology · Physics 2014-11-17 S. M. Bilenky , S. Pascoli , S. T. Petcov

In short-baseline experiments such as LSND and MiniBooNE, an excess of electron neutrinos has been observed, originating from a muon neutrino beam. To address this anomaly, in the line of many works, we investigate various neutrino mixing…

High Energy Physics - Phenomenology · Physics 2026-03-06 Priya , Simran Arora , B. C. Chauhan

With 741 kg of TeO2 crystals and an excellent energy resolution of 5 keV (0.2%) at the region of interest, the CUORE (Cryogenic Underground Observatory for Rare Events) experiment aims at searching for neutrinoless double beta decay of…

Instrumentation and Detectors · Physics 2015-02-10 CUORE Collaboration , 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 , A. Caminata , L. Canonica , X. Cao , S. Capelli , L. Cappelli , L. Carbone , L. Cardani , 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 , V. Datskov , S. Dell'Oro , M. Deninno , S. Di Domizio , M. L. di Vacri , A. Drobizhev , 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 , P. Gorla , C. Gotti , T. D. Gutierrez , E. E. Haller , K. Han , K. M. Heeger , R. Hennings-Yeomans , K. P. Hickerson , H. Z. Huang , R. Kadel , K. Kazkaz , G. Keppel , Yu. G. Kolomensky , Y. L. Li , C. Ligi , K. E. Lim , X. Liu , Y. G. Ma , C. Maiano , M. Maino , M. Martinez , R. H. Maruyama , Y. Mei , N. Moggi , S. Morganti , T. Napolitano , M. Nastasi , S. Nisi , C. Nones , E. B. Norman , A. Nucciotti , T. O'Donnell , F. Orio , D. Orlandi , J. L. Ouellet , C. E. Pagliarone , M. Pallavicini , V. Palmieri , L. Pattavina , M. Pavan , M. Pedretti , G. Pessina , V. Pettinacci , G. Piperno , C. Pira , S. Pirro , S. Pozzi , 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 , G. Q. Zhang , B. X. Zhu , S. Zucchelli

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…

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 determination of experimental sensitivity is a key step in the search for neutrinoless double beta decay ($0\nu\beta\beta$), providing a quantitative benchmark for detector design. Two commonly used statistical approaches are the…

Instrumentation and Detectors · Physics 2025-11-05 Haoyang Fu , Wentai Luo , Xiangpan Ji , Shaomin Chen

The HEIDELBERG-MOSCOW experiment, which is the most sensitive double beta decay experiment since ten years has been regularly continued until end of November 2003. An analysis of the data has been performed already until May 20, 2003. The…

High Energy Physics - Phenomenology · Physics 2009-09-29 H. V. Klapdor-Kleingrothaus , I. V. Krivosheina , A. Dietz , C. Tomei , O. Chkvoretz , H. Strecker

The observation of neutrino oscillations and hence non-zero neutrino masses provided a milestone in the search for physics beyond the Standard Model. But even though we now know that neutrinos are massive, the nature of neutrino masses,…

Neutrinoless double-beta decay is a predicted beyond Standard Model process that could clarify some of the not yet known neutrino properties, such as the mass scale, the mass hierarchy, and its nature as a Dirac or Majorana fermion. Should…

Nuclear Theory · Physics 2016-07-06 Andrei Neacsu , Mihai Horoi

We study the discovery potential of future beta decay experiments on searches for the neutrino mass in the sub-eV range, and, in particular, KATRIN experiment with sensitivity $m > 0.3$ eV. Effects of neutrino mass and mixing on the beta…

High Energy Physics - Phenomenology · Physics 2014-11-17 Y. Farzan , O. L. G. Peres , A. Yu. Smirnov

The nuclear matrix elements $M^{0\nu}$ of the neutrinoless double beta decay ($0\nu\beta\beta$) are evaluated for $^{76}$Ge,$^{100}$Mo, $^{130}$Te, and $^{136}$Xe within the Renormalized Quasiparticle Random Phase Approximation (RQRPA) and…

Nuclear Theory · Physics 2011-05-05 V. A. Rodin , Amand Faessler , F. Šimkovic , Petr Vogel

The compelling experimental evidences for oscillations of solar and atmospheric neutrinos imply the existence of 3-neutrino mixing in vacuum. We briefly review the phenomenology of 3-neutrino mixing, and the current data on the 3-neutrino…

High Energy Physics - Phenomenology · Physics 2009-11-11 S. T. Petcov

The Cryogenic Underground Observatory for Rare Events (CUORE) is designed to search for neutrinoless double beta decay of 130Te with an array of 988 TeO2 bolometers operating at temperatures around 10 mK. The experiment is currently being…

Instrumentation and Detectors · Physics 2017-09-01 CUORE Collaboration , 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 , M. Laubenstein