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Related papers: The Majorana Neutrinoless Double-Beta Decay Experi…

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Spectroscopic studies of two beta-rays from 100Mo are shown to be of potential interest for investigating both the Majorana neutrino mass by neutrinoless double beta-decay and low energy solar neutrino's by inverse beta-decay. With a…

Nuclear Experiment · Physics 2009-10-31 H. Ejiri , J. Engel , R. Hazama , P. Krastev , N. Kudomi , R. G. H. Robertson

The occurrence of the neutrinoless decay 0n-bb mode has fundamental consequences: first total lepton number is not conserved, and second, the neutrino is a Majorana particle. Further the effective mass measured allows to put an absolute…

High Energy Physics - Phenomenology · Physics 2007-05-23 Hans Volker Klapdor-Kleingrothaus

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

We propose the construction of LEGEND-1000, the ton-scale Large Enriched Germanium Experiment for Neutrinoless $\beta \beta$ Decay. This international experiment is designed to answer one of the highest priority questions in fundamental…

Instrumentation and Detectors · Physics 2024-09-10 LEGEND Collaboration , N. Abgrall , I. Abt , M. Agostini , A. Alexander , C. Andreoiu , G. R. Araujo , F. T. Avignone , W. Bae , A. Bakalyarov , M. Balata , M. Bantel , I. Barabanov , A. S. Barabash , P. S. Barbeau , C. J. Barton , P. J. Barton , L. Baudis , C. Bauer , E. Bernieri , L. Bezrukov , K. H. Bhimani , V. Biancacci , E. Blalock , A. Bolozdynya , S. Borden , B. Bos , E. Bossio , A. Boston , V. Bothe , R. Bouabid , S. Boyd , R. Brugnera , N. Burlac , M. Busch , A. Caldwell , T. S. Caldwell , R. Carney , C. Cattadori , Y. -D. Chan , A. Chernogorov , C. D. Christofferson , P. -H. Chu , M. Clark , T. Cohen , D. Combs , T. Comellato , R. J. Cooper , I. A. Costa , V. D'Andrea , J. A. Detwiler , A. Di Giacinto , N. Di Marco , J. Dobson , A. Drobizhev , M. R. Durand , F. Edzards , Yu. Efremenko , S. R. Elliott , A. Engelhardt , L. Fajt , N. Faud , M. T. Febbraro , F. Ferella , D. E. Fields , F. Fischer , M. Fomina , H. Fox , J. Franchi , R. Gala , A. Galindo-Uribarri , A. Gangapshev , A. Garfagnini , A. Geraci , C. Gilbert , M. Gold , C. Gooch , K. P. Gradwohl , M. P. Green , G. F. Grinyer , A. Grobov , J. Gruszko , I. Guinn , V. E. Guiseppe , V. Gurentsov , Y. Gurov , K. Gusev , B. Hacket , F. Hagemann , J. Hakenmüeller , M. Haranczyk , L. Hauertmann , C. R. Haufe , C. Hayward , B. Heffron , F. Henkes , R. Henning , D. Hervas Aguilar , J. Hinton , R. Hodak , H. Hoffmann , W. Hofmann , A. Hostiuc , J. Huang , M. Hult , M. Ibrahim Mirza , J. Jochum , R. Jones , D. Judson , M. Junker , J. Kaizer , V. Kazalov , Y. Kermaïdic , H. Khushbakht , M. Kidd , T. Kihm , K. Kilgus , I. Kim , A. Klimenko , K. T. Knöpfle , O. Kochetov , S. I. Konovalov , I. Kontul , K. Kool , L. L. Kormos , V. N. Kornoukhov , M. Korosec , P. Krause , V. V. Kuzminov , J. M. López-Castaño , K. Lang , M. Laubenstein , E. León , B. Lehnert , A. Leonhardt , A. Li , M. Lindner , I. Lippi , X. Liu , J. Liu , D. Loomba , A. Lubashevskiy , B. Lubsandorzhiev , N. Lusardi , Y. Müller , M. Macko , C. Macolino , B. Majorovits , F. Mamedov , W. Maneschg , L. Manzanillas , G. Marshall , R. D. Martin , E. L. Martin , R. Massarczyk , D. Mei , S. J. Meijer , S. Mertens , M. Misiaszek , E. Mondragon , M. Morella , B. Morgan , T. Mroz , D. Muenstermann , C. J. Nave , I. Nemchenok , M. Neuberger , T. K. Oli , G. Orebi Gann , G. Othman , V. Palušova , R. Panth , L. Papp , L. S. Paudel , K. Pelczar , J. Perez Perez , L. Pertoldi , W. Pettus , P. Piseri , A. W. P. Poon , P. Povinec , A. Pullia , D. C. Radford , Y. A. Ramachers , C. Ransom , L. Rauscher , M. Redchuk , A. L. Reine , S. Riboldi , K. Rielage , S. Rozov , E. Rukhadze , N. Rumyantseva , J. Runge , N. W. Ruof , R. Saakyan , S. Sailer , G. Salamanna , F. Salamida , D. J. Salvat , V. Sandukovsky , S. Schönert , A. Schültz , M. Schütt , D. C. Schaper , J. Schreiner , O. Schulz , M. Schuster , M. Schwarz , B. Schwingenheuer , O. Selivanenko , M. Shafiee , E. Shevchik , M. Shirchenko , Y. Shitov , H. Simgen , F. Simkovic , M. Skorokhvatov , M. Slavickova , K. Smolek , A. Smolnikov , J. A. Solomon , G. Song , K. Starosta , I. Stekl , M. Stommel , D. Stukov , R. R. Sumathi , D. A. Sweigart , K. Szczepaniec , L. Taffarello , D. Tagnani , R. Tayloe , D. Tedeschi , M. Turqueti , R. L. Varner , S. Vasilyev , A. Veresnikova , K. Vetter , C. Vignoli , C. Vogl , K. von Sturm , D. Waters , J. C. Waters , W. Wei , C. Wiesinger , J. F. Wilkerson , M. Willers , C. Wiseman , M. Wojcik , V. H. -S. Wu , W. Xu , E. Yakushev , T. Ye , C. -H. Yu , V. Yumatov , N. Zaretski , J. Zeman , I. Zhitnikov , D. Zinatulina , A. -K. Zschocke , A. J. Zsigmond , K. Zuber , G. Zuzel

Neutrinoless double beta decay has been the subject of intensive theoretical work as it represents the only practical approach to discovering whether neutrinos are Majorana particles or not, and whether lepton number is a conserved quantum…

Nuclear Theory · Physics 2013-03-04 R. G. H. Robertson

In this paper a microscopic state-of-the-art approach to calculation of the nuclear matrix element $M^{0\nu}$ for neutrinoless double beta decay with an account for nuclear deformation is presented in length and applied for $^{76}$Ge,…

Nuclear Theory · Physics 2015-03-17 Dong-Liang Fang , Amand Faessler , Vadim Rodin , Fedor Simkovic

We present a search for neutrinoless double-beta ($0\nu\beta\beta$) decay of $^{136}$Xe using the full \mbox{KamLAND-Zen 800} dataset with 745\,kg of enriched xenon, corresponding to an exposure of $2.1$\,ton\,yr of $^{136}$Xe. This updated…

The primary goal of the GERmanium Detector Array (Gerda) experiment at the Laboratori Nazionali del Gran Sasso of INFN is the search for the neutrinoless double beta decay of Ge-76. High-purity germanium detectors made from material…

Nuclear Experiment · Physics 2013-02-14 GERDA Collaboration , M. Agostini , M. Allardt , E. Andreotti , A. M. Bakalyarov , M. Balata , I. Barabanov , M. Barnabe Heider , N. Barros , L. Baudis , C. Bauer , N. Becerici-Schmidt , E. Bellotti , S. Belogurov , S. T. Belyaev , G. Benato , A. Bettini , L. Bezrukov , T. Bode , V. Brudanin , R. Brugnera , D. Budjas , A. Caldwell , C. Cattadori , A. Chernogorov , F. Cossavella , E. V. Demidova , A. Denisov , A. Domula , V. Egorov , R. Falkenstein , A. D. Ferella , K. Freund , F. Froborg , N. Frodyma , A. Gangapshev , A. Garfagnini , S. Gazzana , P. Grambayr , V. Gurentsov , K. Gusev , K. K. Guthikonda , W. Hampel , A. Hegai , M. Heisel , S. Hemmer , G. Heusser , W. Hofmann , M. Hult , L. V. Inzhechik , L. Ioannucci , J. Janicsko Csathy , J. Jochum , M. Junker , S. Kianovsky , I. V. Kirpichnikov , A. Kirsch , A. Klimenko , K. T. Knoepfle , O. Kochetov , V. N. Kornoukhov , V. Kusminov , M. Laubenstein , A. Lazzaro , V. I. Lebedev , B. Lehnert , H. Y. Liao , M. Lindner , I. Lippi , X. Liu , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , A. A. Machado , B. Majorovits , W. Maneschg , I. Nemchenok , S. Nisi , C. O'Shaughnessy , L. Pandola , K. Pelczar , L. Peraro , A. Pullia , S. Riboldi , F. Ritter , C. Sada , M. Salathe , C. Schmitt , S. Schoenert , J. Schreiner , O. Schulz , B. Schwingenheuer , E. Shevchik , M. Shirchenko , H. Simgen , A. Smolnikov , L. Stanco , H. Strecker , M. Tarka , C. A. Ur , A. A. Vasenko , O. Volynets , K. von Sturm , M. Walter , A. Wegmann , M. Wojcik , E. Yanovich , P. Zavarise , I. Zhitnikov , S. V. Zhukov , D. Zinatulina , K. Zuber , G. Zuzel

A generalisation of the neutrinoless double beta decay process is presented. Neutrinoless double beta decay measures only one out of nine possible effective Majorana neutrino masses in case of three flavours. Limits obtained for all the…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. Zuber

Background of germanium and xenon detectors due to the elastic scattering of $^{8}B$ solar neutrinos on electrons have been calculated. The background is 4.6 \times $10^{-4}$ counts/(keV$\cdot t\cdot$y) that defines the sensitivity of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alexander A. Klimenko

The SuperNEMO project aims to search for neutrinoless double beta decay ($0\nu\beta\beta$) up to a sensitivity of 10$^{26}$ years for the $0\nu\beta\beta$ half-life (down to 50 meV in the effective Majorana neutrino mass), using $\sim$100…

Nuclear Experiment · Physics 2008-07-22 Yu. Shitov

Neutrinoless double-beta decay($0\nu\beta\beta$) decay is a hypothetical process that violates lepton number, and whose observation would unambiguously indicate that neutrinos are Majorana fermions. In the standard inverted-ordering…

Nuclear Experiment · Physics 2019-12-10 I. S. Guinn , J. M. López-Castaño

Virtual Majorana neutrinos are indispensable for neutrinoless double-beta (0$\nu\beta\beta$) decay. In this study, we demonstrate that the overlap of the virtual Majorana neutrino wavefunction, predominantly composed of a right-handed…

High Energy Physics - Phenomenology · Physics 2025-03-24 Dongming Mei , Kunming Dong , Austin Warren , Sanjay Bhattarai

Neutrinoless double-beta decay ($0\nu\beta\beta$) is a rare hypothesised process that, if discovered, would establish that the neutrino is Majorana, that is, it is its own antiparticle. Interpretation of experimental results relies on…

High Energy Physics - Lattice · Physics 2025-04-29 Anthony V. Grebe

The observation of neutrino oscillations has proven that neutrinos have mass. This is direct evidence of physics beyond the Standard Model. This discovery has renewed interest in neutrinoless double beta decay ($0\nu\beta\beta$) experiments…

High Energy Physics - Experiment · Physics 2008-10-20 R. Benton Pahlka

The results of the HEIDELBERG-MOSCOW experiment which searches with 11 kg of enriched 76Ge for double beta decay in the GRAN Sasso underground laboratory are presented for the full running period August 1990 - May 2003. The duty cycle of…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. V. Klapdor-Kleingrothaus , I. V. Krivosheina , A. Dietz , O. Chkvorets

The Neutrinoless double beta Decay allows to determine the effectice Majorana electron neutrino mass. For this the following conditions have to be satisfied: (i) The neutrino must be a Majorana particle, i. e. identical to the antiparticle.…

High Energy Physics - Phenomenology · Physics 2012-03-19 Amand Faessler

The MAJORANA DEMONSTRATOR will search for the neutrinoless double-beta decay of the 76Ge isotope with a mixed array of enriched and natural germanium detectors. The observation of this rare decay would indicate the neutrino is its own…

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