English
Related papers

Related papers: A multi-isotope $0\nu2\beta$ bolometric experiment

200 papers

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

Assuming that neutrinos are Majorana particles, in a three generation framework, current and future neutrino oscillation experiments can determine six out of the nine parameters which fully describe the structure of the neutrino mass…

High Energy Physics - Phenomenology · Physics 2014-11-17 H. Nunokawa , W. J. C. Teves , R. Zukanovich Funchal

We present a framework to combine data from the latest neutrinoless double-beta decay experiments for multiple isotopes and derive a limit on the effective neutrino mass using the experimental energy distributions. The combined limits on…

High Energy Physics - Experiment · Physics 2015-06-12 Pawel Guzowski , Luke Barnes , Justin Evans , Georgia Karagiorgi , Nathan McCabe , Stefan Soldner-Rembold

After nearly 80 years since the first guess on its existence, neutrino still escapes our insight: the mass and the true nature (Majorana or Dirac) of this particle is still unknown. In the past ten years, neutrino oscillation experiments…

Instrumentation and Detectors · Physics 2013-12-17 O. Cremonesi , M. Pavan

The observation of neutrino oscillations and hence non-zero neutrino masses provided a milestone in the search for physics beyond the Standard Model. But even though we now know that neutrinos are massive, the nature of neutrino masses,…

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

The observation of neutrinoless double-beta decay (0${\nu}{\beta}{\beta}$) would show that lepton number is violated, reveal that neutrinos are Majorana particles, and provide information on neutrino mass. A discovery-capable experiment…

Instrumentation and Detectors · Physics 2018-06-15 LEGEND Collaboration , N. Abgrall , A. Abramov , N. Abrosimov , I. Abt , M. Agostini , M. Agartioglu , A. Ajjaq , S. I. Alvis , F. T. Avignone , X. Bai , M. Balata , I. Barabanov , A. S. Barabash , P. J. Barton , L. Baudis , L. Bezrukov , T. Bode , A. Bolozdynya , D. Borowicz , A. Boston , H. Boston , S. T. P. Boyd , R. Breier , V. Brudanin , R. Brugnera , M. Busch , M. Buuck , A. Caldwell , T. S. Caldwell , T. Camellato , M. Carpenter , C. Cattadori , J. Cederkäll , Y. -D. Chan , S. Chen , A. Chernogorov , C. D. Christofferson , P. -H. Chu , R. J. Cooper , C. Cuesta , E. V. Demidova , Z. Deng , M. Deniz , J. A. Detwiler , N. Di Marco , A. Domula , Q. Du , Yu. Efremenko , V. Egorov , S. R. Elliott , D. Fields , F. Fischer , A. Galindo-Uribarri , A. Gangapshev , A. Garfagnini , T. Gilliss , M. Giordano , G. K. Giovanetti , M. Gold , P. Golubev , C. Gooch , P. Grabmayr , M. P. Green , J. Gruszko , I. S. Guinn , V. E. Guiseppe , V. Gurentsov , Y. Gurov , K. Gusev , J. Hakenmüeller , L. Harkness-Brennan , Z. R. Harvey , C. R. Haufe , L. Hauertmann , D. Heglund , L. Hehn , A. Heinz , R. Hiller , J. Hinton , R. Hodak , W. Hofmann , S. Howard , M. A. Howe , M. Hult , L. V. Inzhechik , J. Janicskó Csáthy , R. Janssens , M. Ješkovský , J. Jochum , H. T. Johansson , D. Judson , M. Junker , J. Kaizer , K. Kang , V. Kazalov , Y. Kermaïdic , F. Kiessling , A. Kirsch , A. Kish , A. Klimenko , K. T. K. T. Knöpfle , O. Kochetov , S. I. Konovalov , I. Kontul , V. N. Kornoukhov , T. Kraetzschmar , K. Kröninger , A. Kumar , V. V. Kuzminov , K. Lang , M. Laubenstein , A. Lazzaro , Y. L. Li , Y. -Y. Li , H. B. Li , S. T. Lin , M. Lindner , I. Lippi , S. K. Liu , X. Liu , J. Liu , D. Loomba , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , H. Ma , B. Majorovits , F. Mamedov , R. D. Martin , R. Massarczyk , J. A. J. Matthews , N. McFadden , D. -M. Mei , H. Mei , S. J. Meijer , D. Mengoni , S. Mertens , W. Miller , M. Miloradovic , R. Mingazheva , M. Misiaszek , P. Moseev , J. Myslik , I. Nemchenok , T. Nilsson , P. Nolan , C. O'Shaughnessy , G. Othman , K. Panas , L. Pandola , L. Papp , K. Pelczar , D. Peterson , W. Pettus , A. W. P. Poon , P. P. Povinec , A. Pullia , X. C. Quintana , D. C. Radford , J. Rager , C. Ransom , F. Recchia , A. L. Reine , S. Riboldi , K. Rielage , S. Rozov , N. W. Rouf , E. Rukhadze , N. Rumyantseva , R. Saakyan , E. Sala , F. Salamida , V. Sandukovsky , G. Savard , S. Schönert , A. -K. Schütz , O. Schulz , M. Schuster , B. Schwingenheuer , O. Selivanenko , B. Sevda , B. Shanks , E. Shevchik , M. Shirchenko , F. Simkovic , L. Singh , V. Singh , M. Skorokhvatov , K. Smolek , A. Smolnikov , A. Sonay , M. Spavorova , I. Stekl , D. Stukov , D. Tedeschi , J. Thompson , T. Van Wechel , R. L. Varner , A. A. Vasenko , S. Vasilyev , A. Veresnikova , K. Vetter , K. von Sturm , K. Vorren , M. Wagner , G. -J. Wang , D. Waters , W. -Z. Wei , T. Wester , B. R. White , C. Wiesinger , J. F. Wilkerson , M. Willers , C. Wiseman , M. Wojcik , H. T. Wong , J. Wyenberg , W. Xu , E. Yakushev , G. Yang , C. -H. Yu , Q. Yue , V. Yumatov , J. Zeman , Z. Zeng , I. Zhitnikov , B. Zhu , D. Zinatulina , A. Zschocke , A. J. Zsigmond , K. Zuber , G. Zuzel

Neutrinoless double beta decay searches play a major role in determining neutrino properties, in particular the Majorana or Dirac nature of the neutrino and the absolute scale of the neutrino mass. The consequences of these searches go…

The NEMO 3 experiment is located in the Modane Underground Laboratory and has been taking data since 2003 with seven isotopes. It is searching for the double beta decay process with two or zero neutrinos emitted in the final state.…

High Energy Physics - Experiment · Physics 2019-08-14 R. L. Flack

Neutrinoless double beta decay ($0\nu\beta\beta$) is one of the most sensitive approaches to test particle physics beyond the standard model. During the last years, besides the most restrictive limit on the effective Majorana neutrino mass,…

High Energy Physics - Phenomenology · Physics 2015-06-25 H. Päs

We discuss a consistency test which makes it possible to discriminate unknown nuclear background lines from neutrinoless double beta decay with only one isotope. By considering both the transition to the ground state and to the first…

High Energy Physics - Phenomenology · Physics 2011-11-18 Michael Duerr , Manfred Lindner , Kai Zuber

Neutrinoless double beta decay is one of the most sensitive approaches in non-accelerator particle physics to take us into a regime of physics beyond the standard model. This article is a brief review of the experiments in search of…

High Energy Physics - Phenomenology · Physics 2008-03-12 Somnath Choudhury

The study of neutrinoless double-beta decay plays a fundamental role in the understanding of neutrino physics. Its observation would prove that neutrinos are Majorana particles and that lepton number is not conserved. Experimental searches…

Nuclear Experiment · Physics 2017-05-12 Sergio Di Domizio

It is well known that there exist many mechanisms that may contribute to neutrinoless double beta decay (0nbb-decay). By exploiting the fact that the associated nuclear matrix elements are target dependent we show that, given definite…

High Energy Physics - Phenomenology · Physics 2011-01-20 Fedor Simkovic , John Vergados , Amand Faessler

The {\sc Majorana} Project, a neutrinoless double-beta decay experiment is described with an emphasis on the choice of Ge-detector configuration.

Nuclear Experiment · Physics 2012-08-27 The MAJORANA collaboration

We show that, in the framework of a general model with mixing of three Majorana neutrinos and a neutrino mass hierarchy, the results of the Bugey and Krasnoyarsk reactor neutrino oscillation experiments imply strong limitations for the…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. M. Bilenky , C. Giunti , M. Monteno

The SuperNEMO project studies the feasibility of employing a technique of tracking plus calorimetry to search for neutrinoless double beta decay in 100 kg of enriched isotopes. It aims to reach an effective neutrino mass sensitivity of 50…

Instrumentation and Detectors · Physics 2019-08-13 Irina Nasteva

A discovery that neutrinos are not the usual Dirac but Majorana fermions, i.e. identical to their antiparticles, would be a manifestation of new physics with profound implications for particle physics and cosmology. Majorana neutrinos would…

High Energy Physics - Experiment · Physics 2019-10-01 GERDA collaboration , M. Agostini , A. M. Bakalyarov , M. Balata , I. Barabanov , L. Baudis , C. Bauer , E. Bellotti , S. Belogurov , A. Bettini , L. Bezrukov , D. Borowicz , V. Brudanin , R. Brugnera , A. Caldwell , C. Cattadori , A. Chernogorov , T. Comellato , V. D'Andrea , E. V. Demidova , N. Di Marco , A. Domula , E. Doroshkevich , V. Egorov , R. Falkenstein , M. Fomina , A. Gangapshev , A. Garfagnini , M. Giordano , P. Grabmayr , V. Gurentsov , K. Gusev , J. Hakenmüller , A. Hegai , M. Heisel , S. Hemmer , R. Hiller , W. Hofmann , M. Hult , L. V. Inzhechik , J. Janicskó Csáthy , J. Jochum , M. Junker , V. Kazalov , Y. Kermaïdic , T. Kihm , I. V. Kirpichnikov , A. Kirsch , A. Kish , A. Klimenko , R. Kneißl , K. T. Knöpfle , O. Kochetov , V. N. Kornoukhov , P. Krause , V. V. Kuzminov , M. Laubenstein , A. Lazzaro , M. Lindner , I. Lippi , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , C. Macolino , B. Majorovits , W. Maneschg , M. Miloradovic , R. Mingazheva , M. Misiaszek , P. Moseev , I. Nemchenok , K. Panas , L. Pandola , K. Pelczar , L. Pertoldi , P. Piseri , A. Pullia , C. Ransom , S. Riboldi , N. Rumyantseva , C. Sada , E. Sala , F. Salamida , C. Schmitt , B. Schneider , S. Schönert , A. -K. Schütz , O. Schulz , B. Schwingenheuer , M. Schwarz , O. Selivanenko , E. Shevchik , M. Shirchenko , H. Simgen , A. Smolnikov , L. Stanco , D. Stukov , L. Vanhoefer , A. A. Vasenko , A. Veresnikova , K. von Sturm , V. Wagner , A. Wegmann , T. Wester , C. Wiesinger , M. Wojcik , E. Yanovich , I. Zhitnikov , S. V. Zhukov , D. Zinatulina , A. Zschocke , A. J. Zsigmond , K. Zuber , G. Zuzel

CUPID-0 is the first pilot experiment of CUPID, a next-generation project for the measurement of neutrinoless double beta decay (0$\nu$DBD) with scintillating bolometers. The detector, consisting of 24 enriched and 2 natural ZnSe crystals,…

‹ Prev 1 4 5 6 7 8 10 Next ›