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Related papers: Gauge vectors and double beta decay

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We study possible contribution of the Majorana neutrino mass eigenstate $\nu_h$ dominated by a sterile neutrino component to neutrinoless double beta ($0\nu\beta\beta$) decay. From the current experimental lower bound on the…

High Energy Physics - Phenomenology · Physics 2009-11-11 P. Benes , Amand Faessler , S. Kovalenko , F. Simkovic

Proton decay via d=5 operators is excluded by now not only in the framework of SUSY SU(5) but also its extensions like SUSY SO(10) are on the verge of being inconsistent with d=5 decays. It is reasonable therefore to suppress, e.g. by a…

High Energy Physics - Phenomenology · Physics 2009-11-07 Yoav Achiman , Marcus Richter

We investigate neutrinoless double beta decay ($0\nu\beta\beta$) in the presence of sterile neutrinos with Majorana mass terms. These gauge-singlet fields are allowed to interact with Standard-Model (SM) fields via renormalizable Yukawa…

High Energy Physics - Phenomenology · Physics 2020-07-15 Wouter Dekens , Jordy de Vries , Kaori Fuyuto , Emanuele Mereghetti , Guanghui Zhou

We revisit the impact of heavy neutrinos with masses in the MeV-GeV range on neutrinoless double beta decay ($0\nu\beta\beta$) in view of updated results for the lifetime of this process. Working in a minimal realistic extension of the…

High Energy Physics - Phenomenology · Physics 2025-05-21 J. de Vries , M. Drewes , Y. Georis , J. Klarić , V. Plakkot

Neutrinoless double beta ($0\nu\beta\beta$) decay can in general produce electrons of either chirality, in contrast with the minimal Standard Model (SM) extension with only the addition of the Weinberg operator, which predicts two…

High Energy Physics - Phenomenology · Physics 2015-06-04 Francisco del Aguila , Alberto Aparici , Subhaditya Bhattacharya , Arcadi Santamaria , Jose Wudka

Motivated by the observation of non-zero neutrino masses and the potential for discovering physics beyond the Standard Model, numerous experiments are actively searching for neutrinoless double beta $(0\nu\beta\beta)$ decay. In all of these…

High Energy Physics - Phenomenology · Physics 2026-05-05 Noor-Ines Boudjema , Frank F. Deppisch , Antonio Herrero-Brocal , Chayan Majumdar , Supriya Senapati

We present an alternative formulation of the left-right symmetric theory where the scalar sector consists of two Higgs doublets which differs from the standard version of the left-right model that makes use of $L-$ and $R-$ Higgs triplets…

High Energy Physics - Phenomenology · Physics 2013-02-01 Sudhanwa Patra

After a short review of the current status of three-neutrino mixing, the implications for the values of neutrino masses are discussed. The bounds on the absolute scale of neutrino masses from Tritium beta-decay and cosmological data are…

High Energy Physics - Phenomenology · Physics 2009-11-10 Carlo Giunti

Neutrinoless double beta ($0\nu\beta\beta$) decay, an important low-energy process, serves not only as a potential test of the Majorana nature of neutrinos, but also as a sensitive probe for new physics beyond the Standard Model. In this…

High Energy Physics - Phenomenology · Physics 2025-10-10 Vivek Banerjee , Sasmita Mishra

We explore the phenomenology of virtual spin-1 contributions to the h to gamma gamma and h to Z gamma decay rates in gauge extensions of the standard model. We consider generic lorentz and gauge invariant vector self-interactions, which can…

High Energy Physics - Phenomenology · Physics 2014-03-05 Don Bunk , Jay Hubisz , Bithika Jain

We consider tritium beta decay with additional emission of light pseudoscalar or vector bosons coupling to electrons or neutrinos. The electron energy spectrum for all cases is evaluated and shown to be well estimated by approximated…

The angular distribution of the final electrons in the so-called long range mechanism of the neutrinoless double beta decay ($0\nu2\beta$) is derived for the general Lorentz invariant effective Lagrangian. Possible theories beyond the SM…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Ali , A. V. Borisov , D. V. Zhuridov

When three Majorana neutrinos describe the solar and atmospheric neutrino data via oscillations, a nonzero measurement of neutrinoless double beta ($0\nu\beta\beta$) decay can determine the sum of neutrino masses $\sum m_\nu$ if the solar…

High Energy Physics - Phenomenology · Physics 2009-09-15 V. Barger , K. Whisnant

We discuss the use of massive vectors for the interpretation of some recent experimental anomalies, with special attention to the muon $g-2$. We restrict our discussion to the case where the massive vector is embedded into a spontaneously…

High Energy Physics - Phenomenology · Physics 2016-11-03 Carla Biggio , Marzia Bordone , Luca Di Luzio , Giovanni Ridolfi

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

Solar neutrinos interact within double-beta decay (\BB) detectors and contribute to backgrounds for \BB\ experiments. Background contributions due to charge-current solar neutrino interactions with \BB\ nuclei of $^{76}$Ge, $^{82}$Se,…

Nuclear Experiment · Physics 2017-10-25 S. R. Elliott , H. Ejiri

Gauge bosons associated with unbroken gauge symmetries, under which all standard model fields are singlets, may interact with ordinary matter via higher-dimensional operators. A complete set of dimension-six operators involving a massless…

High Energy Physics - Phenomenology · Physics 2008-11-26 Bogdan A. Dobrescu

The experimental determination of V_{ud} from neutron beta decay requires accurate values of the neutron lifetime and the ratio of the weak axial-vector to vector coupling constants of the nucleon. The latter is derived from measurements of…

Nuclear Experiment · Physics 2013-02-19 Oliver Zimmer

Ruling out the inverted neutrino hierarchy with neutrinoless double beta decay experiments is possible if a limit on the effective mass below the minimal theoretically possible value is reached. We stress that this lower limit depends…

High Energy Physics - Phenomenology · Physics 2011-07-05 Alexander Dueck , Werner Rodejohann , Kai Zuber

The solar and atmospheric data and possibly large value for the effective neutrino mass in neutrinoless double beta decay experiment together indicate that all the three neutrinos are nearly degenerate. A verifiable texture for the neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 Anjan S. Joshipura , Saurabh D. Rindani