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Related papers: Experiments for the absolute neutrino mass measure…

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The \underline{KA}rlsruhe \underline{TRI}tium \underline{N}eutrino Mass Experiment is a next generation tritium beta decay experiment designed to reach a sensitivity of $0.2~ \mathrm{eV}/\mathrm{c}^2$. KATRIN will allow to investigate the…

High Energy Physics - Experiment · Physics 2019-08-14 Lutz Bornschein

Various ways of determining the absolute neutrino masses are briefly reviewed and their sensitivities compared. The apparent tension between the announced but unconfirmed observation of the $0\nu\beta\beta$ decay and the neutrino mass upper…

High Energy Physics - Phenomenology · Physics 2008-11-26 Petr Vogel

We present a concise formula to relate the effective mass term of the neutrinoless double beta decay to a single neutrino mass, two Majorana CP-violating phases and four observables of neutrino oscillations for a generic neutrino mass…

High Energy Physics - Phenomenology · Physics 2009-11-07 Zhi-zhong Xing

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

Within the standard three-neutrino framework, the absolute neutrino masses and their ordering (either normal, NO, or inverted, IO) are currently unknown. However, the combination of current data coming from oscillation experiments,…

High Energy Physics - Phenomenology · Physics 2017-06-07 Francesco Capozzi , Eleonora Di Valentino , Eligio Lisi , Antonio Marrone , Alessandro Melchiorri , Antonio Palazzo

The fact that neutrinos carry a non-vanishing rest mass is evidence of physics beyond the Standard Model of elementary particles. Their absolute mass bears important relevance from particle physics to cosmology. In this work, we report on…

Nuclear Experiment · Physics 2025-09-19 M. Aker , D. Batzler , A. Beglarian , J. Behrens , J. Beisenkötter , M. Biassoni , B. Bieringer , Y. Biondi , F. Block , S. Bobien , M. Böttcher , B. Bornschein , L. Bornschein , T. S. Caldwell , M. Carminati , A. Chatrabhuti , S. Chilingaryan , B. A. Daniel , K. Debowski , M. Descher , D. Díaz Barrero , P. J. Doe , O. Dragoun , G. Drexlin , F. Edzards , K. Eitel , E. Ellinger , R. Engel , S. Enomoto , A. Felden , C. Fengler , C. Fiorini , J. A. Formaggio , C. Forstner , F. M. Fränkle , K. Gauda , A. S. Gavin , W. Gil , F. Glück , S. Grohmann , R. Grössle , R. Gumbsheimer , N. Gutknecht , V. Hannen , L. Hasselmann , N. Haußmann , K. Helbing , H. Henke , S. Heyns , S. Hickford , R. Hiller , D. Hillesheimer , D. Hinz , T. Höhn , A. Huber , A. Jansen , C. Karl , J. Kellerer , K. Khosonthongkee , M. Kleifges , M. Klein , J. Kohpeiß , C. Köhler , L. Köllenberger , A. Kopmann , N. Kovač , A. Kovalík , H. Krause , L. La Cascio , T. Lasserre , J. Lauer , T. Le , O. Lebeda , B. Lehnert , G. Li , A. Lokhov , M. Machatschek , M. Mark , A. Marsteller , E. L. Martin , C. Melzer , S. Mertens , S. Mohanty , J. Mostafa , K. Müller , A. Nava , H. Neumann , S. Niemes , A. Onillon , D. S. Parno , M. Pavan , U. Pinsook , A. W. P. Poon , J. M. Lopez Poyato , S. Pozzi , F. Priester , J. Ráliš , S. Ramachandran , R. G. H. Robertson , C. Rodenbeck , M. Röllig , C. Röttele , M. Ryšavý , R. Sack , A. Saenz , R. Salomon , P. Schäfer , M. Schlösser , K. Schlösser , L. Schlüter , S. Schneidewind , U. Schnurr , M. Schrank , J. Schürmann , A. Schütz , A. Schwemmer , A. Schwenck , M. Šefčík , D. Siegmann , F. Simon , F. Spanier , D. Spreng , W. Sreethawong , M. Steidl , J. Štorek , X. Stribl , M. Sturm , N. Suwonjandee , N. Tan Jerome , H. H. Telle , L. A. Thorne , T. Thümmler , S. Tirolf , N. Titov , I. Tkachev , K. Urban , K. Valerius , D. Vénos , C. Weinheimer , S. Welte , J. Wendel , C. Wiesinger , J. F. Wilkerson , J. Wolf , S. Wüstling , J. Wydra , W. Xu , S. Zadorozhny , G. Zeller

While the mass differences between neutrino mass states are known, their absolute masses and mass hierarchy have not yet been determined. Determining the mass of neutrinos provides access to physics beyond the Standard Model and the…

The KArlsruhe TRItium Neutrino experiment (KATRIN) aims to measure the mass of electron neutrinos from beta-decay of tritium with an unprecedented sensitivity of 0.2 eV/c^2 improving present limits by one order of magnitude. The decay…

Instrumentation and Detectors · Physics 2019-08-13 J. Wolf

Neutrinoless double beta decay is the only process known so far able to test the neutrino intrinsic nature: its experimental observation would imply that the lepton number is violated by two units and prove that neutrinos have a Majorana…

High Energy Physics - Experiment · Physics 2015-06-22 Alberto Garfagnini

The present status of double beta decay experiments are reviewed. The results of the most sensitive experiments, NEMO-3 and CUORICINO, are discussed. Proposals for future double beta decay experiments are considered. In these experiments…

High Energy Physics - Experiment · Physics 2015-06-25 A. S. Barabash

The KATRIN experiment is designed to measure the absolute neutrino mass scale with a sensitivity of 200 meV at 90% C.L. by high resolution tritium beta-spectroscopy. A low background level of 10 mHz at the beta-decay endpoint is required in…

Instrumentation and Detectors · Physics 2015-06-04 S. Mertens , G. Drexlin , F. M. Fraenkle , D. Furse , F. Glueck , S. Goerhardt , M. Hoetzel , W. Kaefer , B. Leiber , T. Thuemmler , N. Wandkowsky , J. Wolf

The next generation of double-beta decay experiments have an excellent chance of providing data on the neutrino mass pattern. This presentation is a summary of what is currently known about the mass pattern and expectations from experiment.…

Nuclear Experiment · Physics 2015-06-26 Steven R. Elliott

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

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

The observation of neutrinoless double beta decay will have important consequences. First it will signal that lepton number is not conserved and the neutrinos are Majorana particles. Second, it represents our best hope for determining the…

High Energy Physics - Phenomenology · Physics 2016-12-12 J. D. Vergados , H. Ejiri , F Šimkovic

In this followup to Phys. Rev. D 75, 053001 (2007) [arXiv:hep-ph/0608060] we report updated constraints on neutrino mass-mixing parameters, in light of recent neutrino oscillation data (KamLAND, SNO, and MINOS) and cosmological observations…

High Energy Physics - Phenomenology · Physics 2010-05-12 G. L. Fogli , E. Lisi , A. Marrone , A. Melchiorri , A. Palazzo , A. M. Rotunno , P. Serra , J. Silk , A. Slosar

The phenomenology of absolute neutrino masses is reviewed, focusing on tritium beta decay, cosmological measurements and neutrinoless double-beta decay.

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

Measuring the absolute scale of the neutrino masses is one of the most exciting opportunities available with near-term cosmological datasets. Two quantities that are sensitive to neutrino mass, scale-dependent halo bias $b(k)$ and the…

Cosmology and Nongalactic Astrophysics · Physics 2016-06-01 Marilena LoVerde

The most stringent constraint on the so-called effective electron neutrino mass from the present neutrinoless double beta decay experiments is |M_{ee}| < 0.2 eV, while the planned next generation experiment GENIUS is anticipated to reach a…

High Energy Physics - Phenomenology · Physics 2009-10-31 Anna Kalliomaki , Jukka Maalampi

The KArlsruhe TRItium Neutrino experiment (KATRIN) aims to measure the absolute neutrino mass scale with an unprecedented sensitivity of 0.2 eV/c2 (90% C.L.), using beta decay electrons from tritium decay. The kinetic energy of the decay…

Instrumentation and Detectors · Physics 2018-09-26 J. Letnev , W. Hazenbiller , A. Osipowicz , A. Beglarian , H. Bouquet , G. Drexlin , F. Glück , J. Garbe , H. Hillmer , P. Marte , T. Thümmler , Ch. Weinheimer