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Related papers: Neutrino mass limit from tritium beta decay

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Although neutrinos are probably the most abundant particles of the universe their mass is not yet known. Oscillation experiments have proven that at least one of the neutrino mass states has m_{i}>0.05 eV while various interpretations of…

High Energy Physics - Experiment · Physics 2016-10-13 Otokar Dragoun , Drahoslav Vénos

The KATRIN experiment has recently reported a new upper limit to the mass of the electron neutrino of $m<0.8 eV$ (90\%CL), and a best value of $m^2= 0.26 \pm 0.34 eV^2/c^4$ based on a fit to the observed tritium beta decay spectrum. Here…

High Energy Physics - Phenomenology · Physics 2021-11-23 Robert Ehrlich

An electron antineutrino mass has been measured in tritium beta-decay in the "Troitsk nu-mass" experiment. The setup consists of a windowless gaseous tritium source and an electrostatic electron spectrometer. The whole data set acquired…

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

The definition method of the limit for the neutrino mass of rest by using the analysis of the extreme values of the beta-particles distribution under beta-decay is given. The anomaly of distribution at the end of the curve was analyzed. The…

General Physics · Physics 2010-02-09 A. A. Akmarov , K. A. Akmarov

The discovery of neutrino oscillations has shown that neutrinos, in contradiction to a prediction of the minimal standard model, have mass. Oscillations do not yield a value for the mass, but do set a lower limit of 0.02 eV on the average…

Nuclear Experiment · Physics 2015-02-03 R. G. Hamish Robertson

We performed a search for any sign of an additional neutrino mass state in beta-electron spectrum based on data reanalysis of direct electron antineutrino mass measurements in Tritium beta-decay in the Troitsk nu-mass experiment. The…

High Energy Physics - Experiment · Physics 2015-06-12 A. I. Belesev , A. I. Berlev , E. V. Geraskin , A. A. Golubev , N. A. Likhovid , A. A. Nozik , V. S. Pantuev , V. I. Parfenov , A. K. Skasyrskaya

The shape of the beta decay energy distribution is sensitive to the mass of the electron neutrino. Attempts to measure the endpoint shape of tritium decay have so far seen no distortion from the zero-mass form, thus placing an upper limit…

Nuclear Experiment · Physics 2009-09-24 Benjamin Monreal , Joseph A. Formaggio

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 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

We discuss the physics potential of future tritium beta-decay experiments having a sensitivity to a neutrino mass ~\sqrt{|\Delta m^{2}_{23}|}~5x10^{-2} eV. The case of three-neutrino mixing is analised. A negative result of such an…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Bilenky , M. D. Mateev , S. T. Petcov

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 beta decay of molecular tritium currently provides the highest sensitivity in laboratory-based neutrino mass measurements. The upcoming Karlsruhe Tritium Neutrino (KATRIN) experiment will improve the sensitivity to 0.2 eV, making a…

Nuclear Experiment · Physics 2015-06-23 L. I. Bodine , D. S. Parno , R. G. H. Robertson

The paper reports on the improved Mainz experiment on tritum $\beta$ spectroscopy which yields a 10 times' higher signal to background ratio than before. The main experimental effects and systematic uncertainties have been investigated in…

High Energy Physics - Experiment · Physics 2009-09-29 Ch. Kraus , B. Bornschein , L. Bornschein , J. Bonn , B. Flatt , A. Kovalik , B. Ostrick , E. W. Otten , J. P. Schall , Th. Thümmler , Ch. Weinheimer

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

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

Taking into account mixings among neutrino states, the end of the energy spectrum of the electron in the tritium beta decay is investigated. It is shown that for real energy resolutions of a spectrometer, $ \Delta E > 0.08$ eV, the…

High Energy Physics - Phenomenology · Physics 2016-08-16 J. Studnik , M. Zrałek

Taking as input the best fit solar neutrino anomaly description, MSW LMA, and the tritium beta decay results we estimate the allowed range of neutrino masses independently of their nature. Adding the present bound on the effective neutrino…

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

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 motivation, present status, and future plans of the search for the neutrinoless double beta decay are reviewed. It is argued that, motivated by the recent observations of neutrino oscillations, there is a reasonable hope that…

High Energy Physics - Phenomenology · Physics 2011-07-19 Steven R. Elliott , Petr Vogel
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