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Related papers: Extra Dimensions and Neutrinoless Double Beta Deca…

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We have examined the importance of momentum dependent induced nucleon currents such as weak-magnetism and pseudoscalar couplings to the amplitude of neutrinoless double beta decay in the mechanisms of light and heavy Majorana neutrino as…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. Simkovic , G. Pantis , J. D. Vergados , A. Faessler

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

Many extensions of the Standard Model of particle physics suggest that neutrinos should be Majorana-type fermions, but this assumption is difficult to confirm. Observation of neutrinoless double-beta decay ($0\nu \beta \beta$), a…

Of the many extensions to the standard model that could possibly generate neutrino mass, most necessitate the neutrino being a Majorana fermion. If this is the case, the rare process of neutrinoless double beta decay is predicted with half…

Instrumentation and Detectors · Physics 2019-10-30 Ethan Brown , Kelly Odgers , Adam Tidball

We consider the possibility that neutrinoless double beta decay may occur in models with unbroken lepton number via the emission of a massive gauge boson with electron lepton number $-2$. We determine the shape of the $\beta\,\beta$ sum…

High Energy Physics - Phenomenology · Physics 2009-10-22 Christopher D. Carone

Recent results of the Heidelberg-Moscow double beta decay experiment are presented. After 8.6 kg$\cdot$a of measuring time no signal is seen for the neutrinoless decay mode. A half-life limit of $T_{1/2}^{0\nu\beta\beta} > 5.1\cdot…

High Energy Physics - Experiment · Physics 2016-08-31 Heidelberg-Moscow-Collaboration

In this brief review we discuss the generation of Majorana neutrino masses through the see-saw mechanism, the theory of neutrinoless double-beta decay, the implications of neutrino oscillation data for the effective Majorana mass, taking…

High Energy Physics - Phenomenology · Physics 2015-06-04 S. M. Bilenky , C. Giunti

The discovery of neutrinoless double-beta decay could soon be within reach. This hypothetical ultra-rare nuclear decay offers a privileged portal to physics beyond the Standard Model of particle physics. Its observation would constitute the…

High Energy Physics - Experiment · Physics 2023-06-01 Matteo Agostini , Giovanni Benato , Jason A. Detwiler , Javier Menéndez , Francesco Vissani

Since 2003 the NEMO~3 experiment has been searching for neutrinoless double beta decay using about 10 kg of enriched isotopes. A limit of T_(1/2)(0nu) > 5.8 10**23 years at 90 % CL has been obtained for 100-Mo from the first two years of…

High Energy Physics - Experiment · Physics 2008-11-26 Stefan Soldner-Rembold

Neutrinoless double beta decay (\( 0 \nu \beta \beta \)) is a hypothetical nuclear decay mode with important implications. In particular, observation of this decay would demonstrate that the neutrino is a Majorana particle and that lepton…

High Energy Physics - Lattice · Physics 2020-04-17 W. Detmold , D. J. Murphy

The LEGEND experiment is looking for the extremely rare neutrinoless double beta ($0\nu\beta\beta$) decay of $^{76}$Ge using isotopically-enriched high-purity germanium (HPGe) detectors. The detection of this process would imply that the…

High Energy Physics - Experiment · Physics 2025-08-27 Carmen Romo-Luque

The Standard Model of particle physics cannot explain the dominance of matter over anti-matter in our Universe. In many model extensions this is a very natural consequence of neutrinos being their own anti-particles (Majorana particles)…

Nuclear Experiment · Physics 2017-04-07 M. Agostini , M. Allardt , A. M. Bakalyarov , M. Balata , I. Barabanov , L. Baudis , C. Bauer , E. Bellotti , S. Belogurov , S. T. Belyaev , G. Benato , A. Bettini , L. Bezrukov , T. Bode , D. Borowicz , V. Brudanin , R. Brugnera , A. Caldwell , C. Cattadori , A. Chernogorov , V. D'Andrea , E. V. Demidova , N. DiMarco , A. diVacri , A. Domula , E. Doroshkevich , V. Egorov , R. Falkenstein , O. Fedorova , K. Freund , N. Frodyma , A. Gangapshev , A. Garfagnini , C. Gooch , P. Grabmayr , V. Gurentsov , K. Gusev , J. Hakenmüller , A. Hegai , M. Heisel , S. Hemmer , W. Hofmann , M. Hult , L. V. Inzhechik , J. Janicskó Csáthy , J. Jochum , M. Junker , V. Kazalov , T. Kihm , I. V. Kirpichnikov , A. Kirsch , A. Kish , A. Klimenko , R. Kneißl , K. T. Knöpfle , O. Kochetov , V. N. Kornoukhov , V. V. Kuzminov , M. Laubenstein , A. Lazzaro , V. I. Lebedev , B. Lehnert , H. Y. Liao , M. Lindner , I. Lippi , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , C. Macolino , B. Majorovits , W. Maneschg , E. Medinaceli , M. Miloradovic , R. Mingazheva , M. Misiaszek , P. Moseev , I. Nemchenok , D. Palioselitis , K. Panas , L. Pandola , K. Pelczar , A. Pullia , S. Riboldi , N. Rumyantseva , C. Sada , F. Salamida , M. Salathe , C. Schmitt , B. Schneider , S. Schönert , J. Schreiner , O. Schulz , A. -K. Schütz , B. Schwingenheuer , O. Selivanenko , E. Shevchik , M. Shirchenko , H. Simgen , A. Smolnikov , L. Stanco , L. Vanhoefer , A. A. Vasenko , A. Veresnikova , K. von Sturm , V. Wagner , M. Walter , A. Wegmann , T. Wester , C. Wiesinger , M. Wojcik , E. Yanovich , I. Zhitnikov , S. V. Zhukov , D. Zinatulina , K. Zuber , G. Zuzel

A new generation of neutrinoless double beta decay experiments with improved sensitivity is currently under design and construction. They will probe inverted hierarchy region of the neutrino mass pattern. There is also a revived interest to…

Nuclear Theory · Physics 2015-06-05 Amand Faessler , Vadim Rodin , Fedor Simkovic

The LEGEND collaboration is searching for neutrinoless double beta ($0\nu\beta\beta$) decay by operating high-purity germanium detectors enriched in $^{76}$Ge in a low-background liquid argon environment. Building on key technological…

High Energy Physics - Experiment · Physics 2025-10-01 H. Acharya , N. Ackermann , M. Agostini , A. Alexander , C. Andreoiu , G. R. Araujo , F. T. Avignone , M. Babicz , W. Bae , A. Bakalyarov , M. Balata , A. S. Barabash , P. S. Barbeau , C. J. Barton , L. Baudis , C. Bauer , E. Bernieri , L. Bezrukov , K. H. Bhimani , V. Biancacci , E. Blalock , S. J. Borden , G. Borghi , F. Borra , B. Bos , A. Boston , V. Bothe , R. Bouabid , R. Brugnera , N. Burlac , M. Busch , S. Calgaro , L. Canonica , S. Capra , M. Carminati , R. M. D. Carney , C. Cattadori , R. Cesarano , Y. -D. Chan , J. R. Chapman , A. Chernogorov , P. -J. Chiu , C. D. Christofferson , M. L. Clark , A. I. Colon-Rivera , T. Comellato , V. D'Andrea , R. Deckert , J. A. Detwiler , A. Di Giacinto , N. Di Marco , T. Dixon , K. -M. Dong , A. Drobizhev , G. Duran , Yu. Efremenko , S. R. Elliott , C. H. J. Emmanuel , E. Engelhardt , E. Esch , M. T. Febbraro , F. Ferella , D. E. Fields , C. Fiorini , M. Fomina , N. Fuad , R. Gala , A. Galindo-Uribarri , A. Gangapshev , A. Garfagnini , S. Gazzana , A. Geraci , L. Gessler , C. Ghiano , A. Gieb , S. Giri , M. Gold , C. Gooch , G. Grünauer , M. P. Green , J. Gruszko , I. Guinn , V. E. Guiseppe , V. Gurentsov , Y. Gurov , K. Gusev , B. Hackett , F. Hagemann , M. Haranczyk , F. Henkes , R. Henning , J. Herrera , D. Hervas Aguilar , J. Hinton , R. Hodák , H. F. R. Hoffmann , M. A. Howe , M. Huber , M. Hult , A. Ianni , K. Jędrzejczak , J. Jochum , R. W. L. Jones , D. S. Judson , M. Junker , J. Kaizer , V. Kazalov , M. F. Kidd , T. Kihm , K. Kilgus , A. Klimenko , K. T. Knöpfle , I. Kochanek , O. Kochetov , I. Kontul , L. L. Kormos , V. N. Kornoukhov , P. Krause , H. Krishnamoorthy , V. V. Kuzminov , K. Lang , M. Laubenstein , N. N. P. N. Lay , E. León , A. Leder , B. Lehnert , A. Leonhardt , N. Levashko , L. Y. Li , A. Li , Y. -R. Lin , M. Lindner , I. Lippi , A. Love , A. Lubashevskiy , B. Lubsandorzhiev , N. Lusardi , C. Macolino , B. Majorovits , F. Mamedov , L. Manzanillas , G. G. Marshall , R. D. Martin , E. L. Martin , R. Massarczyk , A. Mazumdar , G. McDowell , D. -M. Mei , S. P. Meireles , M. Menzel , S. Mertens , E. Miller , I. Mirza , M. Misiaszek , M. Morella , B. Morgan , T. Mroz , D. Muenstermann , C. J. Nave , I. Nemchenok , M. Neuberger , N. O'Briant , F. Paissan , L. Papp , L. S. Paudel , K. Pelczar , L. Pertoldi , W. Pettus , F. Piastra , M. Pichotta , P. Piseri , A. W. P. Poon , P. P. Povinec , M. Pruckner , A. Pullia , W. S. Quinn , D. C. Radford , Y. A. Ramachers , A. Razeto , M. Redchuk , A. L. Reine , S. Riboldi , K. Rielage , C. Romo-Luque , N. Rossi , S. Rozov , T. J. Ruland , N. Rumyantseva , J. Runge , R. Saakyan , S. Sailer , G. Salamanna , F. Salamida , G. Saleh , V. Sandukovsky , C. Savarese , S. Schönert , A. -K. Schütz , D. C. Schaper , L. Schlüter , S. J. Schleich , O. Schulz , M. Schwarz , B. Schwingenheuer , C. Seibt , O. Selivanenko , G. Senatore , A. Serafini , K. Shakhov , E. Shevchik , M. Shirchenko , Y. Shitov , H. Simgen , F. Šimkovic , S. Simonaitis-Boyd , M. Skorokhvatov , M. Slavíčková , A. Smolnikov , J. A. Solomon , G. Song , A. C. Sousa , A. R. Sreekala , L. Steinhart , I. Štekl , T. Sterr , M. Stommel , S. A. Sullivan , R. R. Sumathi , K. Szczepaniec , L. Taffarello , D. Tagnani , D. J. Tedeschi , T. N. Thorpe , V. Tretyak , M. Turqueti , E. E. Van Nieuwenhuizen , L. J. Varriano , S. Vasilyev , A. Veresnikova , C. Vignoli , C. Vogl , K. von Sturm , A. Warren , D. Waters , S. L. Watkins , C. Wiesinger , J. F. Wilkerson , M. Willers , C. Wiseman , M. Wojcik , D. Xu , W. Xu , E. Yakushev , T. Ye , C. -H. Yu , V. Yumatov , D. Zinatulina , K. Zuber , G. Zuzel

The neutrinoless double beta decay is analyzed using a general Lorentz invariant effective Lagrangian for various decaying nuclei of current experimental interest: $^{76}$Ge, $^{82}$Se, $^{100}$Mo, $^{130}$Te, and $^{136}$Xe. We work out…

High Energy Physics - Phenomenology · Physics 2015-06-03 A. Ali , A. V. Borisov , D. V. Zhuridov

Study of the neutrinoless $\beta\beta$ decay allows us to put a stringent limit on the effective neutrino Majorana mass, a quantity of fundamental importance. To test our ability to evaluate the nuclear matrix elements that govern the decay…

Nuclear Theory · Physics 2007-05-23 Petr Vogel

The Majorana nature of neutrinos will be the confirmed by the observation of the rare process called as neutrinoless double beta decay process, i.e. the simultaneous decay of two neutrons in the nucleus of an isotope (A, Z) into two protons…

High Energy Physics - Phenomenology · Physics 2022-04-27 Pritam Kumar Bishee , Purushottam Sahu , Sudhanwa Patra

We construct two new classes of models for double beta decay, each of which leads to an electron spectrum which differs from the decays which are usually considered. One of the classes has a spectrum which has not been considered to date,…

High Energy Physics - Phenomenology · Physics 2009-10-28 P. Bamert , C. P. Burgess , R. N. Mohapatra

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

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