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Related papers: Neutrino-less Double Beta Decay and Particle Physi…

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From the standard seesaw mechanism of neutrino mass generation, which is based on the assumption that the lepton number is violated at a large (~10exp(+15) GeV) scale, follows that the neutrinoless double-beta decay is ruled by the Majorana…

High Energy Physics - Phenomenology · Physics 2015-05-27 Samoil M. Bilenky , Amand Faessler , Walter Potzel , Fedor Simkovic

Neutrinoless double-beta decay is proposed as an important low energy phenomenon that could test beyond the Standard Model physics. There are several potentially competing beyond the Standard Model mechanisms that can induce the process. It…

High Energy Physics - Phenomenology · Physics 2019-12-09 Fahim Ahmed , Andrei Neacsu , Mihai Horoi

Neutrinoless double beta ($0\nu\beta\beta$) decays of spin-1/2 hyperons are investigated in a covariant baryon chiral perturbation theory framework, extended by a $\Delta L=2$ operator proportional to the Majorana neutrino mass, where $L$…

High Energy Physics - Phenomenology · Physics 2026-02-10 Zi-Ying Zhao , Ze-Rui Liang , Feng-Kun Guo , Li-Ping He , De-Liang Yao

Recently the evidence of the neutrinoless double $\beta$ ($0\nu \beta\beta$) decay has been announced. This means that neutrinos are Majorana particles and their mass hierarchy is forced to inverted mass hierarchy (Type B) or degenerate…

High Energy Physics - Phenomenology · Physics 2007-05-23 Naoyuki Haba , Noboru Nakamura , Tomoharu Suzuki

We review current experimental efforts to search for neutrinoless double beta decay (0$\nu\beta\beta$). A description of the selected leading experiments is given and the strongest recent results are compared in terms of achieved background…

High Energy Physics - Experiment · Physics 2016-06-29 Igor Ostrovskiy , Kevin O'Sullivan

We study the effective operators of the standard model fields which would yield an observable rate of neutrinoless double beta decay. We particularly focus on the possibility that neutrinoless double beta decay is dominantly induced by…

High Energy Physics - Phenomenology · Physics 2009-11-07 Kiwoon Choi , Kwang Sik Jeong , Wan Young Song

If the electron neutrino has an effective nonzero Majorana mass, then neutrinoless double beta decay will occur. However, the latter is possible also with a negligible neutrino mass. We show how this may happen in a simple model of scalar…

High Energy Physics - Phenomenology · Physics 2009-11-07 Biswajoy Brahmachari , Ernest Ma

This White Paper, prepared for the Fundamental Symmetries, Neutrons, and Neutrinos Town Meeting related to the 2023 Nuclear Physics Long Range Plan, makes the case for double beta decay as a critical component of the future nuclear physics…

Nuclear Experiment · Physics 2022-12-22 C. Adams , K. Alfonso , C. Andreoiu , E. Angelico , I. J. Arnquist , J. A. A. Asaadi , F. T. Avignone , S. N. Axani , A. S. Barabash , P. S. Barbeau , L. Baudis , F. Bellini , M. Beretta , T. Bhatta , V. Biancacci , M. Biassoni , E. Bossio , P. A. Breur , J. P. Brodsky , C. Brofferio , E. Brown , R. Brugnera , T. Brunner , N. Burlac , E. Caden , S. Calgaro , G. F. Cao , L. Cao , C. Capelli , L. Cardani , R. Castillo Fernandez , C. M. Cattadori , B. Chana , D. Chernyak , C. D. Christofferson , P. -H. Chu , E. Church , V. Cirigliano , R. Collister , T. Comellato , J. Dalmasson , V. D'Andrea , T. Daniels , L. Darroch , M. P. Decowski , M. Demarteau , S. De Meireles Peixoto , J. A. Detwiler , R. G. DeVoe , S. Di Domizio , N. Di Marco , M. L. di Vacri , M. J. Dolinski , Yu. Efremenko , M. Elbeltagi , S. R. Elliott , J. Engel , L. Fabris , W. M. Fairbank , J. Farine , M. Febbraro , E. Figueroa-Feliciano , D. E. Fields , J. A. Formaggio , B. T. Foust , B. Franke , Y. Fu , B. K. Fujikawa , D. Gallacher , G. Gallina , A. Garfagnini , C. Gingras , L. Gironi , A. Giuliani , M. Gold , R. Gornea , C. Grant , G. Gratta , M. P. Green , G. F. Grinyer , J. Gruszko , Y. Guan , I. S. Guinn , V. E. Guiseppe , T. D. Gutierrez , E. V. Hansen , C. A. Hardy , J. Hauptman , M. Heffner , K. M. Heeger , R. Henning , H. Hergert , D. Hervas Aguilar , R. Hodak , J. D. Holt , E. W. Hoppe , M. Horoi , H. Z. Huang , K. Inoue , A. Jamil , J. Jochum , B. J. P. Jones , J. Kaizer , G. Karapetrov , S. Al Kharusi , M. F. Kidd , Y. Kishimoto , J. R. Klein , Yu. G. Kolomensky , I. Kontul , V. N. Kornoukhov , P. Krause , R. Krucken , K. S. Kumar , K. Lang , K. G. Leach , B. G. Lenardo , A. Leonhardt , A. Li , G. Li , Z. Li , C. Licciardi , R. Lindsay , I. Lippi , J. Liu , M. Macko , R. MacLellan , C. Macolino , S. Majidi , F. Mamedov , J. Masbou , R. Massarczyk , A. T. Mastbaum , D. Mayer , A. Mazumdar , D. M. Mei , Y. Mei , S. J. Meijer , E. Mereghetti , S. Mertens , K. Mistry , T. Mitsui , D. C. Moore , M. Morella , J. T. Nattress , M. Neuberger , X. E. Ngwadla , C. Nones , V. Novosad , D. R. Nygren , J. C. Nzobadila Ondze , T. O'Donnell , G. D. Orebi Gann , J. L. Orrell , G. S. Ortega , J. L. Ouellet , C. Overman , L. Pagani , V. Palusova , A. Para , M. Pavan , A. Perna , L. Pertoldi , W. Pettus , A. Piepke , P. Piseri , A. Pocar , P. Povinec , F. Psihas , A. Pullia , D. C. Radford , G. J Ramonnye , H. Rasiwala , M. Redchuk , S. Riboldi , G. Richardson , K. Rielage , L. Rogers , P. C. Rowson , E. Rukhadze , R. Saakyan , C. Sada , G. Salamanna , F. Salamida , R. Saldanha , D. J. Salvat , S. Sangiorgio , D. C. Schaper , S. Schoenert , M. Schwarz , S. E. Schwartz , Y. Shitov , F. Simkovic , V. Singh , M. Slavickova , A. C. Sousa , F. L. Spadoni , D. H. Speller , I. Stekl , R. R. Sumathi , P. T. Surukuchi , R. Tayloe , W. Tornow , J. A. Torres , T. I. Totev , S. Triambak , O. A. Tyuka , S. I. Vasilyev , M. Velazquez , S. Viel , C. Vogl , K. von Strum , Q. Wang , D. Waters , S. L. Watkins , M. Watts , W. -Z. Wei , B. Welliver , Liangjian Wen , U. Wichoski , S. Wilde , J. F. Wilkerson , L. Winslow , C. Wiseman , X. Wu , W. Xu , H. Yang , L. Yang , C. H. Yu , J. Zeman , J. Zennamo , G. Zuzel

We present a new channel of the neutrinoless double beta decay. In this scenario neutrinos not only oscillate inside the nucleus but also interact with an external non-uniform magnetic field. We assume that the field rotates about the…

High Energy Physics - Phenomenology · Physics 2016-05-11 Marek Góźdź , Wiesław A. Kamiński

Neutrinoless double beta decay experiments constrain one combination of neutrino parameters, while cosmic surveys constrain another. This complementarity opens up an exciting range of possibilities. If neutrinos are Majorana particles, and…

Cosmology and Nongalactic Astrophysics · Physics 2014-03-21 Scott Dodelson , Joseph Lykken

While neutrino oscillation experiments have demonstrated that neutrinos have small, nonzero masses, much remains unknown about their properties and decay modes. One potential decay mode --- neutrinoless double beta decay ($0 \nu \beta…

High Energy Physics - Lattice · Physics 2018-11-15 W. Detmold , D. J. Murphy

The relation between neutrino oscillation parameters and neutrinoless double beta decay is studied, assuming normal and inverse hierarchies for Majorana neutrino masses. For normal hierarchy the crucial dependence on U_{e3} is explored. The…

High Energy Physics - Phenomenology · Physics 2009-11-07 D. Falcone , F. Tramontano

Study of the neutrinoless double beta decay and searches for the manifestation of the neutrino mass in ordinary beta decay are the main sources of information about the absolute neutrino mass scale, and the only practical source of…

We perform a comprehensive study of the $3+3$ Type-I seesaw model for a broad range of right-handed mass scales (from keV to 10 TeV). We take into account and, in some cases, update the constraints from a large number of high- and…

High Energy Physics - Phenomenology · Physics 2025-05-16 Vincenzo Cirigliano , Wouter Dekens , Sebastián Urrutia Quiroga

Neutrinoless double beta decay ($0\nu\beta\beta$) is a crucial test for lepton number violation. Observation of this process would have fundamental implications for neutrino physics, theories beyond the Standard Model and cosmology.…

High Energy Physics - Phenomenology · Physics 2020-12-01 Frank F. Deppisch , Lukas Graf , Francesco Iachello , Jenni Kotila

In the event of an observation of neutrinoless double beta decay, a relevant question would be: what lepton number violating physics is responsible for the decay? The exchange of Majorana neutrinos and/or supersymmetric particles may…

High Energy Physics - Phenomenology · Physics 2010-07-20 B. C. Allanach , C. H. Kom , H. Päs

Neutrinoless double beta decay allows to constrain lepton number violating extensions of the standard model. If neutrinos are Majorana particles, the mass mechanism will always contribute to the decay rate, however, it is not a priori…

High Energy Physics - Phenomenology · Physics 2015-05-22 J. C. Helo , M. Hirsch , T. Ota , F. A. Pereira dos Santos

A discovery that neutrinos are not the usual Dirac but Majorana fermions, i.e. identical to their antiparticles, would be a manifestation of new physics with profound implications for particle physics and cosmology. Majorana neutrinos would…

High Energy Physics - Experiment · Physics 2019-10-01 GERDA collaboration , M. Agostini , A. M. Bakalyarov , M. Balata , I. Barabanov , L. Baudis , C. Bauer , E. Bellotti , S. Belogurov , A. Bettini , L. Bezrukov , D. Borowicz , V. Brudanin , R. Brugnera , A. Caldwell , C. Cattadori , A. Chernogorov , T. Comellato , V. D'Andrea , E. V. Demidova , N. Di Marco , A. Domula , E. Doroshkevich , V. Egorov , R. Falkenstein , M. Fomina , A. Gangapshev , A. Garfagnini , M. Giordano , P. Grabmayr , V. Gurentsov , K. Gusev , J. Hakenmüller , A. Hegai , M. Heisel , S. Hemmer , R. Hiller , W. Hofmann , M. Hult , L. V. Inzhechik , J. Janicskó Csáthy , J. Jochum , M. Junker , V. Kazalov , Y. Kermaïdic , T. Kihm , I. V. Kirpichnikov , A. Kirsch , A. Kish , A. Klimenko , R. Kneißl , K. T. Knöpfle , O. Kochetov , V. N. Kornoukhov , P. Krause , V. V. Kuzminov , M. Laubenstein , A. Lazzaro , M. Lindner , I. Lippi , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , C. Macolino , B. Majorovits , W. Maneschg , M. Miloradovic , R. Mingazheva , M. Misiaszek , P. Moseev , I. Nemchenok , K. Panas , L. Pandola , K. Pelczar , L. Pertoldi , P. Piseri , A. Pullia , C. Ransom , S. Riboldi , N. Rumyantseva , C. Sada , E. Sala , F. Salamida , C. Schmitt , B. Schneider , S. Schönert , A. -K. Schütz , O. Schulz , B. Schwingenheuer , M. Schwarz , O. Selivanenko , E. Shevchik , M. Shirchenko , H. Simgen , A. Smolnikov , L. Stanco , D. Stukov , L. Vanhoefer , A. A. Vasenko , A. Veresnikova , K. von Sturm , V. Wagner , A. Wegmann , T. Wester , C. Wiesinger , M. Wojcik , E. Yanovich , I. Zhitnikov , S. V. Zhukov , D. Zinatulina , A. Zschocke , A. J. Zsigmond , K. Zuber , G. Zuzel

We study the decay of heavy sterile Majorana neutrinos according to the interactions obtained from an effective general theory. We describe the two and three-body decays for a wide range of neutrino masses. The results obtained and…

High Energy Physics - Phenomenology · Physics 2016-09-21 Lucía Duarte , Ismael Romero , Javier Peressutti , Oscar A. Sampayo

The study of the neutrinoless double beta ($0 \beta\beta$) decay mode can provide us with important information on the neutrino properties, particularly on the electron neutrino absolute mass. In this work we revise the present constraints…

Nuclear Theory · Physics 2016-11-25 Sabin Stoica , Andrei Neacsu
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