English
Related papers

Related papers: Status report on the NEMO3 experiment

200 papers

The possibility to probe new physics scenarios of light Majorana neutrino exchange and right-handed currents at the planned next generation neutrinoless double beta decay experiment SuperNEMO is discussed. Its ability to study different…

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

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…

NEXT (Neutrino Experiment with a Xenon TPC) is a neutrinoless double beta decay experiment located at the Laboratorio Subterr\'aneo de Canfranc (LSC, Spain). Its aim is to demonstrate that the neutrino is a Majorana particle by detecting…

Instrumentation and Detectors · Physics 2022-09-21 Carmen Romo-Luque

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

Neutrinoless double beta decay ($0\nu\beta\beta$) is a rare process which could take place if neutrinos are Majorana fermions: the observation of this decay would provide unambiguous evidence for the existence of new Physics beyond the…

Nuclear Experiment · Physics 2026-01-14 Giovanna Saleh

The South Pole Telescope (SPT) has probed an expanded angular range of the CMB temperature power spectrum. Their recent analysis of the latest cosmological data prefers nonzero neutrino masses, mnu = 0.32+-0.11 eV. This result, if confirmed…

High Energy Physics - Phenomenology · Physics 2013-04-01 J. J. Gomez-Cadenas , J. Martin-Albo , J. Muñoz Vidal , C. Peña-Garay

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

Since the discovery of nuclear beta decay, nuclear physicists have studied the weak interaction and the nature of neutrinos. Many recent and current experiments have been focused on the elucidation of neutrino oscillations and neutrino…

Instrumentation and Detectors · Physics 2014-12-04 R. D. McKeown

The study of neutrinoless double beta decay is of outmost importance for neutrino physics. It is considered to be the gold plated channel to probe the fundamental character of neutrinos and to determine the neutrino mass. From the…

Nuclear Experiment · Physics 2008-11-26 K. Zuber

The Karlsruhe Tritium Neutrino (KATRIN) experiment will provide a measurement of the effective electron-neutrino mass, $m(\nu_e)$, based on a precision measurement of the tritium beta decay spectrum near its endpoint. The effective mass is…

Instrumentation and Detectors · Physics 2018-09-28 Gregg B. Franklin

The present experimental status in the search for neutrinoless double beta decay is reviewed, with emphasis on the first indication for neutrinoless double beta decay found in the Heidelberg-Moscow experiment, giving first evidence for…

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

SNO+ is a large liquid scintillator-based experiment located 2km underground at SNOLAB, Sudbury, Canada. It reuses the Sudbury Neutrino Observatory detector, consisting of a 12m diameter acrylic vessel which will be filled with about 780…

Instrumentation and Detectors · Physics 2016-08-08 SNO+ Collaboration , : , S. Andringa , E. Arushanova , S. Asahi , M. Askins , D. J. Auty , A. R. Back , Z. Barnard , N. Barros , E. W. Beier , A. Bialek , S. D. Biller , E. Blucher , R. Bonventre , D. Braid , E. Caden , E. Callaghan , J. Caravaca , J. Carvalho , L. Cavalli , D. Chauhan , M. Chen , O. Chkvorets , K. Clark , B. Cleveland , I. T. Coulter , D. Cressy , X. Dai , C. Darrach , B. Davis-Purcell , R. Deen , M. M. Depatie , F. Descamps , F. Di Lodovico , N. Duhaime , F. Duncan , J. Dunger , E. Falk , N. Fatemighomi , R. Ford , P. Gorel , C. Grant , S. Grullon , E. Guillian , A. L. Hallin , D. Hallman , S. Hans , J. Hartnell , P. Harvey , M. Hedayatipour , W. J. Heintzelman , R. L. Helmer , B. Hreljac , J. Hu , T. Iida , C. M. Jackson , N. A. Jelley , C. Jillings , C. Jones , P. G. Jones , K. Kamdin , T. Kaptanoglu , J. Kaspar , P. Keener , P. Khaghani , L. Kippenbrock , J. R. Klein , R. Knapik , J. N. Kofron , L. L. Kormos , S. Korte , C. Kraus , C. B. Krauss , K. Labe , I. Lam , C. Lan , B. J. Land , S. Langrock , A. LaTorre , I. Lawson , G. M. Lefeuvre , E. J. Leming , J. Lidgard , X. Liu , Y. Liu , V. Lozza , S. Maguire , A. Maio , K. Majumdar , S. Manecki , J. Maneira , E. Marzec , A. Mastbaum , N. McCauley , A. B. McDonald , J. E. McMillan , P. Mekarski , C. Miller , Y. Mohan , E. Mony , M. J. Mottram , V. Novikov , H. M. O'Keeffe , E. O'Sullivan , G. D. Orebi Gann , M. J. Parnell , S. J. M. Peeters , T. Pershing , Z. Petriw , G. Prior , J. C. Prouty , S. Quirk , A. Reichold , A. Robertson , J. Rose , R. Rosero , P. M. Rost , J. Rumleskie , M. A. Schumaker , M. H. Schwendener , D. Scislowski , J. Secrest , M. Seddighin , L. Segui , S. Seibert , T. Shantz , T. M. Shokair , L. Sibley , J. R. Sinclair , K. Singh , P. Skensved , A. Soerensen , T. Sonley , R. Stainforth , M. Strait , M. I. Stringer , R. Svoboda , J. Tatar , L. Tian , N. Tolich , J. Tseng , H. W. C. Tseung , R. Van Berg , E. Vázquez-Jáuregui , C. Virtue , B. von Krosigk , J. M. G. Walker , M. Walker , O. Wasalski , J. Waterfield , R. F. White , J. R. Wilson , T. J. Winchester , A. Wright , M. Yeh , T. Zhao , K. Zuber

Neutrinoless double beta decay (0nbb) is a direct probe of physics beyond the Standard Model. Its discovery would demonstrate that the lepton number is not a symmetry of nature and would provide us with unique information on the nature and…

High Energy Physics - Experiment · Physics 2019-01-09 Chiara Brofferio , Stefano Dell'Oro

The GEM project is designed for the next generation 2 beta decay experiments with 76-Ge. One ton of ''naked'' HP Ge detectors (natural at the first GEM-I phase and enriched in 76-Ge to 86% at the second GEM-II stage) are operating in…

Nuclear Experiment · Physics 2008-11-26 Yu. G. Zdesenko , O. A. Ponkratenko , V. I. Tretyak

Searches for neutrinoless double-beta decay continue to expand our understanding of the lepton sector, with experiments now pursuing ton-scale target masses with sensitivity to $m_{\beta\beta}$ covering the allowed parameter space for the…

High Energy Physics - Experiment · Physics 2023-04-10 A. Mastbaum , F. Psihas , J. Zennamo

The investigation of the endpoint region of the tritium beta decay spectrum is still the most sensitive direct method to determine the neutrino mass scale. In the nineties and the beginning of this century the tritium beta decay experiments…

High Energy Physics - Experiment · Physics 2009-12-10 C. Weinheimer

The predictions for the effective Majorana mass |<m>| in neutrinoless double-beta decay in the case of 3-neutrino mixing and massive Majorana neutrinos are reviewed. The physics potential of the experiments, searching for neutrinoless…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Pascoli , S. T. Petcov
‹ Prev 1 8 9 10 Next ›