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We discuss four approaches to the determination of absolute neutrino mass. These are the measurement of the zero-neutrino double beta decay rate, of the tritium decay end-point spectrum, of the cosmic ray spectrum above the GZK cutoff (in…

High Energy Physics - Phenomenology · Physics 2009-11-07 H. Päs , T. J. Weiler

Next generation tritium decay experiments to determine the absolute neutrino mass require high-precision measurements of $\beta$-decay electron energies close to the kinematic end point. To achieve this, the development of high phase-space…

The sum of the masses of the three neutrino mass eigenstates is now constrained both from above and below, and lies between 55 and 6900 meV. The lower limit is set by neutrino oscillations and the fact that masses are non-negative. The…

Nuclear Experiment · Physics 2009-07-24 R. G. Hamish Robertson

We report on the data set, data handling, and detailed analysis techniques of the first neutrino-mass measurement by the Karlsruhe Tritium Neutrino (KATRIN) experiment, which probes the absolute neutrino-mass scale via the $\beta$-decay…

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

The paper reviews recent experiments on tritium beta spectroscopy searching for the absolute value of the electron neutrino mass $m(\nu_e)$. By use of dedicated electrostatic filters with high acceptance and resolution, the uncertainty on…

High Energy Physics - Experiment · Physics 2011-05-24 E. W. Otten , C. Weinheimer

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

There are three different methods used to search the neutrino mass: - The electron antineutrino mass can probably best be determined by the Triton decay. - The neutrinoless Double Beta Decay yields information, if the neutrino is a Dirac or…

Nuclear Theory · Physics 2017-03-21 Amand Faessler

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

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…

We propose a beta decay experiment based on a sample of ultracold atomic tritium. These initial conditions enable detection of the helium ion in coincidence with the beta. We construct a two-dimensional fit incorporating both the shape of…

Nuclear Experiment · Physics 2010-05-11 M. Jerkins , J. R. Klein , J. H. Majors , F. Robicheaux , M. G. Raizen

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

Recent advances in cosmic observations have brought us to the verge of discovery of the absolute scale of neutrino masses. Nonzero neutrino masses are known evidence of new physics beyond the Standard Model. Our understanding of the…

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 turn of the 21st century witnessed a sudden shift in our fundamental understanding of particle physics. While the minimal Standard Model predicts that neutrino masses are exactly zero, the discovery of neutrino oscillations proved the…

Nuclear Experiment · Physics 2021-05-21 Joseph A. Formaggio , André Luiz C. de Gouvêa , R. G. Hamish Robertson

The KATRIN experiment aims to determine the neutrino mass scale with a sensitivity of 200 meV/c^2 (90% C.L.) by a precision measurement of the shape of the tritium $\beta$-spectrum in the endpoint region. The energy analysis of the decay…

Recent constrains on the sum of neutrino masses inferred by analyzing cosmological data, show that detecting a non-zero neutrino mass is within reach of forthcoming cosmological surveys, implying a direct determination of the absolute…

Cosmology and Nongalactic Astrophysics · Physics 2019-04-15 Raul Jimenez , Carlos Pena-Garay , Licia Verde

Nearly 70 years since the neutrino was discovered, and 25 years since discovery of neutrino oscillations established its non-zero mass, the absolute neutrino-mass scale remains unknown. Due to its unique characteristics, determining this…

Nuclear Experiment · Physics 2024-11-14 Larisa A. Thorne

We give a comprehensive account of our proposed experimental method of using atoms or molecules in order to measure parameters of neutrinos still undetermined; the absolute mass scale, the mass hierarchy pattern (normal or inverted), the…

The absolute neutrino masses are obtained in terms of the atmospheric and solar mass-squared differences within the framework of low energy phenomenology by suggestion of a quantitative analogy between the hierarchies of the neutrino and…

High Energy Physics - Phenomenology · Physics 2009-11-10 E. M. Lipmanov
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