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Related papers: Neutrinoless double beta decay: 2015 review

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We decompose the neutrinoless double-beta decay matrix elements into sums of products over the intermediate nucleus with two less nucleons. We find that the sum is dominated by the J^pi=0^+ ground state of this intermediate nucleus for both…

Nuclear Theory · Physics 2015-06-23 B. A. Brown , M. Horoi , R. A. Sen'kov

The discovery of neutrino masses has raised the importance of studies in the context of neutrinoless double beta decay, which constitutes a landmark for lepton number violation. The standard interpretation is that the light massive…

High Energy Physics - Phenomenology · Physics 2018-05-25 A. C. O. Santos , P. Vasconcelos

The extension of the Standard Model by right handed neutrinos with masses in the GeV range can simultaneously explain the observed neutrino masses via the seesaw mechanism and the baryon asymmetry of the universe via leptogenesis. It has…

High Energy Physics - Phenomenology · Physics 2017-01-18 Marco Drewes , Shintaro Eijima

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

Nearly 70 years since the neutrino was discovered, and 25 years since discovery of neutrino oscillations established its non-zero mass, the absolute neutrino-mass scale remains unknown. Due to its unique characteristics, determining this…

Nuclear Experiment · Physics 2024-11-14 Larisa A. Thorne

We revisit the "interpolating formula" proposed in our previous publication. It allows one to calculate the neutrinoless double beta decay ($0\nu\beta\beta$-decay) half-life for arbitrary neutrino mass without involvement of the complicated…

High Energy Physics - Phenomenology · Physics 2018-07-11 A. Babič , S. Kovalenko , M. I. Krivoruchenko , F. Šimkovic

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

A large experimental program is being mounted to search for neutrinoless double-beta decay over the next decade. Multiple experiments using different target isotopes are being prepared to explore the whole parameter space allowed for…

High Energy Physics - Phenomenology · Physics 2023-03-22 Matteo Agostini , Frank F. Deppisch , Graham Van Goffrier

The main aspects of the phenomenology of absolute neutrino masses are reviewed, focusing on the limits on neutrino masses obtained in tritium beta decay experiments, cosmological observations and neutrinoless double-beta decay experiments.

High Energy Physics - Phenomenology · Physics 2007-05-23 Carlo Giunti

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 propose a model where neutrino masses are generated at three loop order but neutrinoless double beta decay occurs at one loop. Thus we can have large neutrinoless double beta decay observable in the future experiments even when the…

High Energy Physics - Phenomenology · Physics 2018-06-21 Julien Alcaide , Dipankar Das , Arcadi Santamaria

The effective Majorana neutrino mass is evaluated by using the latest results of neutrino oscillation experiments. The problems of the neutrino mass spectrum,absolute mass scale of neutrinos and the effect of CP phases are addressed. A…

High Energy Physics - Phenomenology · Physics 2014-11-17 S. M. Bilenky , Amand Faessler , F. Simkovic

Neutrinoless double-beta decay, if observed, would signal physics beyond the Standard Model that could be discovered at energies significantly lower than those at which the relevant degrees of freedom could be excited. Therefore, it could…

High Energy Physics - Phenomenology · Physics 2016-07-13 Mihai Horoi , Andrei Neacsu

We make a comparative study of the neutrinoless double beta decay constraints on heavy sterile neutrinos versus other direct and indirect constraints from both lepton number conserving and violating processes, as a sensitive probe of the…

High Energy Physics - Phenomenology · Physics 2020-04-02 Patrick D. Bolton , Frank F. Deppisch , P. S. Bhupal Dev

Neutrino masses are yet unknown. We discuss the present state of effective electron anti-neutrino mass from $\beta$ decay experiments; effective Majorana neutrino mass from neutrinoless double-beta decay experiments; neutrino mass squared…

High Energy Physics - Experiment · Physics 2023-10-31 Jyotsna Singh , M. Ibrahim Mirza

We investigate the predictions for neutrinoless double beta ($(\beta \beta)_{0 \nu}$-) decay effective Majorana mass $\left| \langle \, m \, \rangle \right|$ in the 3+1 and 3+2 schemes with one and two additional sterile neutrinos with…

High Energy Physics - Phenomenology · Physics 2014-06-10 Ivan Girardi , Aurora Meroni , S. T. Petcov

A significant signal of neutrinoless double beta decay can be consistent with the existence of light quasi-Dirac neutrinos. To demonstrate this possibility, we consider a realistic model where the neutrino masses and the neutrinoless double…

High Energy Physics - Phenomenology · Physics 2013-05-30 Pei-Hong Gu

We study the general phenomenology of neutrinoless double beta decay in seesaw models. In particular, we focus on the dependence of the neutrinoless double beta decay rate on the mass of the extra states introduced to account for the…

High Energy Physics - Phenomenology · Physics 2015-03-17 Mattias Blennow , Enrique Fernandez-Martinez , Jacobo Lopez-Pavon , Javier Menendez

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

Neutrino masses can be generated radiatively. In such scenarios their masses are calculated by evaluating a self-energy diagram with vanishing external momentum, i.e. taking only the leading order term in a momentum expansion. The…

High Energy Physics - Phenomenology · Physics 2020-01-08 Werner Rodejohann , Xun-Jie Xu