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Precision measurements in neutron beta decay serve to determine the coupling constants of beta decay and allow for several stringent tests of the standard model. This paper discusses the design and the expected performance of the Nab…

Oscillation experiments show that neutrinos have masses. They however only determine the neutrinop mass differences. Information on the absolute masses can be obtained by studying the kinematics in weak decays, or by searching for…

High Energy Physics - Experiment · Physics 2007-05-23 Jean-Luc Vuilleumier

We report on the neutrino mass measurement result from the first four-week science run of the Karlsruhe Tritium Neutrino experiment KATRIN in spring 2019. Beta-decay electrons from a high-purity gaseous molecular tritium source are energy…

High Energy Physics - Experiment · Physics 2019-12-04 M. Aker , K. Altenmüller , M. Arenz , M. Babutzka , J. Barrett , S. Bauer , M. Beck , A. Beglarian , J. Behrens , T. Bergmann , U. Besserer , K. Blaum , F. Block , S. Bobien , K. Bokeloh , J. Bonn , B. Bornschein , L. Bornschein , H. Bouquet , T. Brunst , T. S. Caldwell , L. La Cascio , S. Chilingaryan , W. Choi , T. J. Corona , K. Debowski , M. Deffert , M. Descher , P. J. Doe , O. Dragoun , G. Drexlin , J. A. Dunmore , S. Dyba , F. Edzards , L. Eisenblätter , K. Eitel , E. Ellinger , R. Engel , S. Enomoto , M. Erhard , D. Eversheim , M. Fedkevych , A. Felden , S. Fischer , B. Flatt , J. A. Formaggio , F. M. Fränkle , G. B. Franklin , H. Frankrone , F. Friedel , D. Fuchs , A. Fulst , D. Furse , K. Gauda , H. Gemmeke , W. Gil , F. Glück , S. Görhardt , S. Groh , S. Grohmann , R. Grössle , R. Gumbsheimer , M. Ha Minh , M. Hackenjos , V. Hannen , F. Harms , J. Hartmann , N. Haußmann , F. Heizmann , K. Helbing , S. Hickford , D. Hilk , B. Hillen , D. Hillesheimer , D. Hinz , T. Höhn , B. Holzapfel , S. Holzmann , T. Houdy , M. A. Howe , A. Huber , A. Jansen , A. Kaboth , C. Karl , O. Kazachenko , J. Kellerer , N. Kernert , L. Kippenbrock , M. Kleesiek , M. Klein , C. Köhler , L. Köllenberger , A. Kopmann , M. Korzeczek , A. Kosmider , A. Kovalí , B. Krasch , M. Kraus , H. Krause , L. Kuckert , B. Kuffner , N. Kunka , T. Lasserre , T. L. Le , O. Lebeda , M. Leber , B. Lehnert , J. Letnev , F. Leven , S. Lichter , V. M. Lobashev , A. Lokhov , M. Machatschek , E. Malcherek , K. Müller , M. Mark , A. Marsteller , E. L. Martin , C. Melzer , A. Menshikov , S. Mertens , L. I. Minter , S. Mirz , B. Monreal , P. I. Morales Guzman , K. Müller , U. Naumann , W. Ndeke , H. Neumann , S. Niemes , M. Noe , N. S. Oblath , H. -W. Ortjohann , A. Osipowicz , B. Ostrick , E. Otten , D. S. Parno , D. G. Phillips , P. Plischke , A. Pollithy , A. W. P. Poon , J. Pouryamout , M. Prall , F. Priester , M. Röllig , C. Röttele , P. C. -O. Ranitzsch , O. Rest , R. Rinderspacher , R. G. H. Robertson , C. Rodenbeck , P. Rohr , Ch. Roll , S. Rupp , M. Rysavy , R. Sack , A. Saenz , P. Schäfer , L. Schimpf , K. Schlösser , M. Schlösser , L. Schlüter , H. Schön , K. Schönung , M. Schrank , B. Schulz , J. Schwarz , H. Seitz-Moskaliuk , W. Seller , V. Sibille , D. Siegmann , A. Skasyrskaya , M. Slezak , A. Spalek , F. Spanier , M. Steidl , N. Steinbrink , M. Sturm , M. Suesser , M. Sun , D. Tcherniakhovski , H. H. Telle , T. Thümmler , L. A. Thorne , N. Titov , I. Tkachev , N. Trost , K. Urban , D. Venos , K. Valerius , B. A. VanDevender , R. Vianden , A. P. Vizcaya Hernandez , B. L. Wall , S. Wüstling , M. Weber , C. Weinheimer , C. Weiss , S. Welte , J. Wendel , K. J. Wierman , J. F. Wilkerson , J. Wolf , W. Xu , Y. -R. Yen , M. Zacher , S. Zadorozhny , M. Zboril , G. Zeller

The mono-energetic conversion electrons from the decay of 83mKr represent a unique tool for the energy calibration, energy scale monitoring and systematic studies of the tritium beta spectrum measurement in the neutrino mass experiment…

Instrumentation and Detectors · Physics 2009-02-03 D. Venos , J. Kaspar , M. Zboril , O. Dragoun , J. Bonn , A. Kovalik , O. Lebeda , M. Rysavy , K. Schlosser , A. Spalek , Ch. Weinheimer

The KATRIN experiment aims to measure the effective mass of the electron antineutrino from the analysis of electron spectra stemming from the beta-decay of molecular tritium with a sensitivity of 200 meV. Therefore, a daily throughput of…

Instrumentation and Detectors · Physics 2025-07-16 L. Kuckert , F. Heizmann , G. Drexlin , F. Glück , M. Hötzel , M. Kleesiek , F. Sharipov , K. Valerius

Neutrino oscillation and tritium beta decay experiments taken simultaneously into account are able to access the so far imperceptible absolute neutrino masses at the electronvolt level. The neutrino mass spectrum derived in this way is…

High Energy Physics - Phenomenology · Physics 2011-02-21 M. Czakon , J. Gluza , J. Studnik , M. Zralek

An earlier prediction of a cosmic ray neutron line right at the energy of the knee of the cosmic ray spectrum was based on the speculation that the electron neutrino is a tachyon whose mass is reciprocally related to the energy of the knee,…

High Energy Physics - Phenomenology · Physics 2009-10-31 Robert Ehrlich

We explore beta decays in a dark background field, which could be formed by dark matter, dark energy or a fifth force potential. In such scenarios, the neutrino's dispersion relation will be modified by its collective interaction with the…

High Energy Physics - Phenomenology · Physics 2023-07-25 Guo-yuan Huang , Werner Rodejohann

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 various experiments on neutrino oscillation evidenced that neutrinos have indeed non-zero masses but cannot tell us the absolute neutrino mass scale. This scale of neutrino masses is very important for understanding the evolution and…

High Energy Physics - Experiment · Physics 2013-09-05 Christian Weinheimer , Kai Zuber

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

We note that the fine structure at the endpoint region of the beta decay spectrum is now essentially known using neutrino oscillation data, if the mass of one neutrino is specified. This may help to identify the effects of nonzero neutrino…

High Energy Physics - Phenomenology · Physics 2009-11-11 S. Masood , S. Nasri , J. Schechter

We describe a beta electron spectrometer for use in an upcoming experiment that will measure the beta-antineutrino correlation coefficient (a-coefficient) in neutron beta decay. Electron energy is measured by a thick plastic scintillator…

At least one neutrino has a mass of about 50 meV or larger. However, the absolute mass scale for the neutrino remains unknown. Studies of double beta decay offer hope for determining the absolute mass scale. Furthermore, the critical…

Nuclear Experiment · Physics 2012-03-23 Steven R. Elliott

The present experimental data on neutrino oscillations, neutrinoless double beta decay and tritium beta decay are collected together and possible mass ranges for Dirac and Majorana neutrinos are found. Four future experimental situations…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Czakon , J. Studnik , M. Zralek

The discovery of neutrino mass establishes the need for physics beyond the Standard Model. I summarize the status of two- and three-neutrino oscillation parameters from current solar, atmospheric, reactor and accelerator data. Future…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. W. F. Valle

The KATRIN experiment is designed for a direct and model-independent determination of the effective electron anti-neutrino mass via a high-precision measurement of the tritium $\beta$-decay endpoint region with a sensitivity on $m_\nu$ of…

Instrumentation and Detectors · Physics 2021-07-21 M. Aker , A. Beglarian , J. Behrens , A. Berlev , U. Besserer , B. Bieringer , F. Block , B. Bornschein , L. Bornschein , M. Böttcher , T. Brunst , T. S. Caldwell , R. M. D. Carney , S. Chilingaryan , W. Choi , K. Debowski , M. Deffert , M. Descher , D. Díaz Barrero , P. J. Doe , O. Dragoun , G. Drexlin , F. Edzards , K. Eitel , E. Ellinger , A. El Miniawy , R. Engel , S. Enomoto , A. Felden , J. A. Formaggio , F. M. Fränkle , G. B. Franklin , F. Friedel , A. Fulst , K. Gauda , W. Gil , F. Glück , S. Groh , R. Grössle , R. Gumbsheimer , V. Hannen , N. Haußmann , F. Heizmann , K. Helbing , S. Hickford , R. Hiller , D. Hillesheimer , D. Hinz , T. Höhn , T. Houdy , A. Huber , A. Jansen , C. Karl , J. Kellerer , M. Kleesiek , M. Klein , C. Köhler , L. Köllenberger , A. Kopmann , M. Korzeczek , A. Kovalík , B. Krasch , H. Krause , N. Kunka , T. Lasserre , L. La Cascio , O. Lebeda , B. Lehnert , T. L. Le , A. Lokhov , M. Machatschek , E. Malcherek , M. Mark , A. Marsteller , E. L. Martin , M. Meier , C. Melzer , A. Menshikov , S. Mertens , J. Mostafa , K. Müller , S. Niemes , P. Oelpmann , D. S. Parno , A. W. P. Poon , J. M. L. Poyato , F. Priester , P. C. -O. Ranitzsch , R. G. H. Robertson , W. Rodejohann , C. Rodenbeck , M. Röllig , C. Röttele , M. Ryšavý , R. Sack , A. Saenz , P. Schäfer , A. Schaller , L. Schimpf , K. Schlösser , M. Schlösser , L. Schlüter , S. Schneidewind , M. Schrank , B. Schulz , C. Schwachtgen , M. Šefčík , H. Seitz-Moskaliuk , V. Sibille , D. Siegmann , M. Slezák , M. Steidl , M. Sturm , M. Sun , D. Tcherniakhovski , H. H. Telle , L. A. Thorne , T. Thümmler , N. Titov , I. Tkachev , N. Trost , K. Urban , K. Valerius , D. Vénos , A. P. Vizcaya Hernández , C. Weinheimer , S. Welte , J. Wendel , J. F. Wilkerson , J. Wolf , S. Wüstling , W. Xu , Y. -R. Yen , S. Zadoroghny , G. Zeller

The Karlsruhe Tritium Neutrino experiment KATRIN will allow a model independent measurement of the neutrino mass scale with an expected sensitivity of 0.2 eV/c^{2} (90% C.L.) and so will help to clarify the role of neutrinos in the early…

High Energy Physics - Experiment · Physics 2019-08-13 Michael Sturm

KATRIN is a very large scale tritium-beta-decay experiment to determine the mass of the neutrino. It is presently under construction at the Forschungszentrum Karlsruhe, and makes use of the Tritium Laboratory built there for the ITER…

Nuclear Experiment · Physics 2019-08-13 R. G. H. Robertson
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