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The KATRIN neutrino experiment is a next-generation tritium beta decay experiment aimed at measuring the mass of the electron neutrino to better than 200 meV at 90% C.L. Due to its intense tritium source, KATRIN can also serve as a possible…

High Energy Physics - Experiment · Physics 2014-11-21 A. Kaboth , J. A. Formaggio , B. Monreal

The KArlsruhe TRItium Neutrino experiment (KATRIN) combines an ultra-luminous molecular tritium source with an integrating high-resolution spectrometer to gain sensitivity to the absolute mass scale of neutrinos. The projected sensitivity…

Nuclear Experiment · Physics 2015-05-28 J. A. Formaggio , J. Barrett

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

The KArlsruhe TRItium Neutrino (KATRIN) experiment is a next generation, model independent, large scale experiment to determine the neutrino mass by investigating the kinematics of tritium beta-decay with a sensitivity of 200 meV/c2. The…

Instrumentation and Detectors · Physics 2011-10-04 F. M. Fraenkle

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

With the compelling evidence for massive neutrinos from recent neutrino-oscillation experiments, one of the most fundamental tasks of particle physics over the next years will be the determination of the absolute mass scale of neutrinos.…

High Energy Physics - Experiment · Physics 2012-08-27 KATRIN collaboration

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

KATRIN is a very large scale tritium-beta-decay experiment to determine the mass of the neutrino. It is presently under construction at the Karlsruhe Institute of Technology north campus, and makes use of the Karlsruhe Tritium Laboratory…

Instrumentation and Detectors · Physics 2013-07-23 R. G. Hamish Robertson

The KArlsruhe TRItium Neutrino (KATRIN) experiment is designed to measure tritium $\beta$-decay spectrum with enough precision to be sensitive to neutrino mass down to 0.2eV at 90$\%$ Confidence Level. After an initial first tritium run in…

Nuclear Experiment · Physics 2019-07-10 Yung-Ruey Yen

One of the most important tasks in neutrino physics is to determine the neutrino mass scale to distinguish between hierarchical and degenerate neutrino mass models and to clarify the role of neutrinos as dark matter particles in the…

High Energy Physics - Experiment · Physics 2007-05-23 Christian Weinheimer

The Karlsruhe Tritium Neutrino (KATRIN) experiment is designed to measure a high-precision integral spectrum of the endpoint region of T2 beta decay, with the primary goal of probing the absolute mass scale of the neutrino. After a first…

Nuclear Experiment · Physics 2023-06-21 M. Aker , M. Balzer , D. Batzler , A. Beglarian , J. Behrens , A. Berlev , U. Besserer , M. Biassoni , B. Bieringer , F. Block , S. Bobien , L. Bombelli , D. Bormann , B. Bornschein , L. Bornschein , M. Böttcher , C. Brofferio , C. Bruch , T. Brunst , T. S. Caldwell , M. Carminati , R. M. D. Carney , S. Chilingaryan , W. Choi , O. Cremonesi , 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 , D. Fink , C. Fiorini , J. A. Formaggio , C. Forstner , F. M. Fränkle , G. B. Franklin , F. Friedel , A. Fulst , K. Gauda , A. S. Gavin , W. Gil , F. Glück , A. Grande , R. Grössle , M. Gugiatti , R. Gumbsheimer , V. Hannen , J. Hartmann , N. Haußmann , K. Helbing , S. Hickford , R. Hiller , D. Hillesheimer , D. Hinz , T. Höhn , T. Houdy , A. Huber , A. Jansen , C. Karl , J. Kellerer , P. King , M. Kleifges , M. Klein , C. Köhler , L. Köllenberger , A. Kopmann , M. Korzeczek , A. Kovalík , B. Krasch , H. Krause , T. Lasserre , L. La Cascio , O. Lebeda , P. Lechner , B. Lehnert , T. L. Le , A. Lokhov , M. Machatschek , E. Malcherek , D. Manfrin , M. Mark , A. Marsteller , E. L. Martin , E. Mazzola , C. Melzer , S. Mertens , J. Mostafa , K. Müller , A. Nava , H. Neumann , S. Niemes , P. Oelpmann , A. Onillon , D. S. Parno , M. Pavan , A. Pigliafreddo , A. W. P. Poon , J. M. L. Poyato , S. Pozzi , F. Priester , M. Puritscher , D. C. Radford , J. Ráliš , S. Ramachandran , R. G. H. Robertson , W. Rodejohann , C. Rodenbeck , M. Röllig , C. Röttele , M. Ryšavý , R. Sack , A. Saenz , R. W. J. Salomon , P. Schäfer , L. Schimpf , K. Schlösser , M. Schlösser , L. Schlüter , S. Schneidewind , M. Schrank , A. K. Schütz , A. Schwemmer , A. Sedlak , M. Šefčík , V. Sibille , D. Siegmann , M. Slezák , F. Spanier , D. Spreng , M. Steidl , M. Sturm , H. H. Telle , L. A. Thorne , T. Thümmler , N. Titov , I. Tkachev , P. Trigilio , K. Urban , K. Valerius , D. Vénos , A. P. Vizcaya Hernández , P. Voigt , C. Weinheimer , E. Weiss , S. Welte , J. Wendel , C. Wiesinger , J. F. Wilkerson , J. Wolf , L. Wunderl , S. Wüstling , J. Wydra , W. Xu , S. Zadoroghny , G. Zeller

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

We investigate the sensitivity of tritium $\beta$-decay experiments for keV-scale sterile neutrinos. Relic sterile neutrinos in the keV mass range can contribute both to the cold and warm dark matter content of the universe. This work shows…

Instrumentation and Detectors · Physics 2015-06-22 S. Mertens , T. Lasserre , S. Groh , F. Glueck , A. Huber , A. W. P. Poon , M. Steidl , N. Steinbrink , C. Weinheimer

The presence of light sterile neutrinos would strongly modify the energy spectrum of the Tritium \beta-electrons. We perform an analysis of the KATRIN experiment's sensitivity by scanning almost all the allowed region of neutrino…

High Energy Physics - Phenomenology · Physics 2012-07-02 Arman Esmaili , Orlando L. G. Peres

The KArlsruhe TRitium Neutrino mass experiment, KATRIN, aims to search for the mass of the electron neutrino with a sensitivity of 0.2 eV/c^2 (90% C.L.) and a detection limit of 0.35 eV/c^2 (5 sigma). Both a positive or a negative result…

Nuclear Experiment · Physics 2010-11-22 Marcus Beck

The KATRIN experiment aims to determine the absolute neutrino mass by measuring the endpoint region of the tritium $\beta$ spectrum. As a large-scale experiment with a sharp energy resolution, high source luminosity and low background it…

The aim of the KArlsruhe TRItium Neutrino experiment KATRIN is the determination of the absolute neutrino mass scale down to 0.2 eV, with essentially smaller model dependence than from cosmology and neutrinoless double beta decay. For this…

High Energy Physics - Phenomenology · Physics 2011-09-07 J. Bonn , K. Eitel , F. Glück , D. Sevilla-Sanchez , N. Titov

The properties of neutrinos and especially their rest mass play an important role at the intersections of cosmology, particle physics and astroparticle physics. At present there are two complementary approaches to address this topic in…

High Energy Physics - Experiment · Physics 2019-08-13 Thomas Thümmler

The precision measurement of the tritium $\beta$-decay spectrum performed by the KATRIN experiment provides a unique way to search for general neutrino interactions (GNI). All theoretical allowed GNI terms involving neutrinos are…

Nuclear Experiment · Physics 2025-09-19 M. Aker , D. Batzler , A. Beglarian , J. Beisenkötter , M. Biassoni , B. Bieringer , Y. Biondi , F. Block , B. Bornschein , L. Bornschein , M. Böttcher , M. Carminati , A. Chatrabhuti , S. Chilingaryan , B. A. Daniel , 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 , G. Gagliardi , K. Gauda , A. S. Gavin , W. Gil , F. Glück , R. Grössle , N. Gutknecht , V. Hannen , L. Hasselmann , K. Helbing , H. Henke , S. Heyns , R. Hiller , D. Hillesheimer , D. Hinz , T. Höhn , A. Huber , A. Jansen , K. Khosonthongkee , C. Köhler , L. Köllenberger , A. Kopmann , N. Kovač , L. La Cascio , T. Lasserre , J. Lauer , T. L. Le , O. Lebeda , B. Lehnert , G. Li , A. Lokhov , M. Machatschek , M. Mark , A. Marsteller , K. McMichael , 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. L. Poyato , F. Priester , J. Ráliš , S. Ramachandran , R. G. H. Robertson , C. Rodenbeck , M. Röllig , R. Sack , A. Saenz , R. Salomon , P. Schäfer , K. Schlösser , M. Schlösser , L. Schlüter , S. Schneidewind , M. Schrank , J. Schürmann , A. K. Schütz , A. Schwemmer , A. Schwenck , J. Seeyangnok , M. Šefčík , D. Siegmann , F. Simon , J. Songwadhana , 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 , N. Titov , I. Tkachev , K. Urban , K. Valerius , D. Vénos , C. Weinheimer , S. Welte , J. Wendel , M. Wetter , C. Wiesinger , J. F. Wilkerson , J. Wolf , S. Wüstling , J. Wydra , W. Xu , S. Zadorozhny , G. Zeller

Recent proposals to study the mass of the "electron" neutrino at a sensitivity of 0.3 eV can be used to place limits on the right handed and scalar charged currents at a level which improves on the present experimental limits. Indeed the…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. H. J. McKellar , M. Garbutt , G. J. Stephenson , T. Goldman
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