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Related papers: Neutrinoless Double $\beta$-Decay: Status and Futu…

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We study the range of the elements of the neutrino mass matrix m_nu in the charged lepton basis. Neutrino-less double beta decay is sensitive to the ee element of m_nu. We then analyze the phenomenological implications of single texture…

High Energy Physics - Phenomenology · Physics 2011-06-24 A. Merle , W. Rodejohann

We consider the minimal seesaw model, the Standard Model extended by two right-handed neutrinos, for explaining the neutrino masses and mixing angles measured in oscillation experiments. When one of right-handed neutrinos is lighter than…

High Energy Physics - Phenomenology · Physics 2023-07-26 Takehiko Asaka , Hiroyuki Ishida , Kazuki Tanaka

The possibility to probe new physics scenarios of light Majorana neutrino exchange and right-handed currents at the planned next generation neutrinoless double beta decay experiment SuperNEMO is discussed. Its ability to study different…

We examine the constraints from the recent HEIDELBERG-MOSCOW double beta decay experiment. It leads us to the almost degenerate or inverse hierarchy neutrino mass scenario. In this scenario, we obtain possible upper bounds for the Majorana…

High Energy Physics - Phenomenology · Physics 2014-11-17 K. Matsuda , T. Kikuchi , T. Fukuyama , H. Nishiura

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

As experimental searches for neutrinoless double-beta ($0\nu\beta\beta$) decay are entering a new generation, with hopes to completely probe the inverted mass hierarchy, the need for reliable nuclear matrix elements, which govern the rate…

Nuclear Theory · Physics 2025-05-08 A. Belley , T. Miyagi , S. R. Stroberg , J. D. Holt

Neutrinoless Double Beta Decay is a hypothesised nuclear process in which two neutrons simultaneously decay into protons with no neutrino emission. The prized observation of this decay would point to the existence of a process that violates…

Nuclear Experiment · Physics 2018-12-19 L. Cardani

We review and remark on models of radiatively induced neutrino Majorana masses and oscillations. It is pointed out that while the models are capable of accounting for the observed solar and atmospheric neutrino oscillation, some of them can…

High Energy Physics - Phenomenology · Physics 2009-12-30 Darwin Chang , A. Zee

The $\nu_M{\rm SM}$ is defined as the SM extended to include dimension-5 operators. In this model neutrino masses violate lepton number, and two parameters of the lepton mixing matrix, the Majorana phases, are yet to be constrained. One…

High Energy Physics - Phenomenology · Physics 2024-10-16 Avital Dery , Stefania Gori , Yuval Grossman , Zoltan Ligeti

At least one neutrino has a mass of about 50 meV or larger. However, the absolute mass scale for the neutrino remains unknown. Furthermore, the critical question: Is the neutrino its own antiparticle? is unanswered. Studies of double beta…

Nuclear Experiment · Physics 2012-04-20 Steven R. Elliott

Present limits on neutrino masses are briefly reviewed, along with cosmological and astrophysical hints from dark matter, solar and atmospheric neutrino observations that suggest neutrino masses. These would imply many possible new…

High Energy Physics - Phenomenology · Physics 2009-09-25 JosÉ W. F. Valle

In this paper we analyze the neutrinoless double beta decay predictions in some scenarios with admixture of pseudo-Dirac and Majorana neutrinos in the 3 and 3+1 neutrino frameworks. We found that some of the cases can be falsifiable in…

High Energy Physics - Phenomenology · Physics 2015-06-22 A. Meroni , E. Peinado

We assess how well next generation neutrinoless double beta decay and normal neutrino beta decay experiments can answer four fundamental questions. 1) If neutrinoless double beta decay searches do not detect a signal, and if the spectrum is…

High Energy Physics - Phenomenology · Physics 2009-09-29 John N. Bahcall , Hitoshi Murayama , Carlos Pena-Garay

We review the current status of the neutrino mass and mixing parameters needed to reconstruct the neutrino mass matrix. A comparative study of the precision in the measurement of oscillation parameters expected from the next generation…

High Energy Physics - Phenomenology · Physics 2016-09-06 Sandhya Choubey

Status of the problem of neutrino masses, mixing and oscillations is discussed. Future perspectives are briefly considered.

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Bilenky

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

Neutrino mass sum rules relate the three neutrino masses within generic classes of flavour models, leading to restrictions on the effective mass parameter measured in experiments on neutrinoless double beta decay as a function of the…

High Energy Physics - Phenomenology · Physics 2015-06-16 Stephen F. King , Alexander Merle , Alexander J. Stuart

Taking as input the best fit solar neutrino anomaly description, MSW LMA, and the tritium beta decay results we estimate the allowed range of neutrino masses independently of their nature. Adding the present bound on the effective neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Czakon , J. Gluza , J. Studnik , M. Zralek

Double beta decay is indispensable to solve the question of the neutrino mass matrix together with $\nu$ oscillation experiments. Recent analysis of the most sensitive experiment since nine years - the HEIDELBERG-MOSCOW experiment in…

High Energy Physics - Phenomenology · Physics 2009-11-10 H. V. Klapdor-Kleingrothaus

If the present or upcoming searches for neutrinoless double beta decay give a positive result, the Majorana nature of massive neutrinos will be established. From the determination of the value of the effective Majorana mass parameter |<m>|,…

High Energy Physics - Phenomenology · Physics 2015-06-25 S. Pascoli , S. T. Petcov
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