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Related papers: Tritium beta decay with additional emission of new…

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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

Tritium beta-decay is the most promising approach to measure the absolute masses of active light neutrinos in the laboratory and in a model-independent fashion. The development of Cyclotron Radiation Emission Spectroscopy techniques and the…

High Energy Physics - Phenomenology · Physics 2023-04-05 James A. L. Canning , Frank F. Deppisch , Wenna Pei

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

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 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

The shape of the electron energy spectrum in 3H beta-decay permits a direct assay of the absolute scale of the neutrino mass; a highly accurate theoretical description of the electron energy spectrum is necessary to the empirical task. We…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. Gardner , V. Bernard , U. -G. Meißner

We compute the spectrum of $\beta$-decay, assuming that (Majorana or Dirac) neutrinos propagate in constant potentials. We study the modifications of the spectrum due to the effect of these potentials. Data on tritium decay and on…

High Energy Physics - Phenomenology · Physics 2009-10-30 Francesco Vissani

We analyse the possible role of new interactions of neutrino in the forthcoming tritium beta decay experiment KATRIN aimed at detecting the neutrino mass with the sensitivity of 0.3 - 0.2 eV. It is shown that under certain circumstances the…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Yu. Ignatiev , B. H. J. McKellar

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

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

Ionization of the final ${}^{3}$He$^{+}$ ion during the nuclear $\beta^{-}$-decay of the tritium atom is discussed. The velocity spectrum of the emitted secondary electrons is derived in the explicit form. Our method allows to determine the…

Nuclear Theory · Physics 2016-06-22 Alexei M. Frolov

The objective of the Karlsruhe Tritium Neutrino (KATRIN) experiment is to determine the effective electron neutrino mass $m(\nu_\text{e})$ with an unprecedented sensitivity of $0.2\,\text{eV}$ (90\% C.L.) by precision electron spectroscopy…

Data Analysis, Statistics and Probability · Physics 2019-03-27 M. Kleesiek , J. Behrens , G. Drexlin , K. Eitel , M. Erhard , J. A. Formaggio , F. Glück , S. Groh , M. Hötzel , S. Mertens , A. W. P. Poon , C. Weinheimer , K. Valerius

Past and current direct neutrino mass experiments set limits on the so-called effective neutrino mass, which is an incoherent sum of neutrino masses and lepton mixing matrix elements. The electron energy spectrum which neglects the…

High Energy Physics - Phenomenology · Physics 2020-01-15 Guo-yuan Huang , Werner Rodejohann , Shun Zhou

A series of high presicion atomic experiments was carried out last decade to get a better estimate for the electron (anti)neutrino mass $m_\nu$. The reaction to be observed is molecular tritium $\beta$- decay. The $m_\nu$ value serves as…

Quantum Physics · Physics 2007-05-23 Vladimir Savichev

Recent measurements of the electron and muon neutrino masses squared are interpreted as an indication that neutrinos are faster than light particles -- tachyons. The tritium beta decay amplitude is calculated for the case of the tachyonic…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jacek Ciborowski , Jakub Rembielinski

The beta decay of tritium in the form of molecular TT is the basis of sensitive experiments to measure neutrino mass. The final-state electronic, vibrational, and rotational excitations modify the beta spectrum significantly, and are…

Precision spectroscopy of the electron spectrum of the tritium $\beta$ decay near the kinematic endpoint is a direct method to determine the effective electron antineutrino mass. The KArlsruhe TRItium Neutrino (KATRIN) experiment aims to…

Instrumentation and Detectors · Physics 2025-06-18 Moritz Machatschek

Numerous recent measurements indicate an excess of counts near the endpoint of the electron energy spectrum in tritium decay. We show that this effect is expected if the neutrino is a tachyon. Results of calculations, based on a unitary…

High Energy Physics - Phenomenology · Physics 2011-09-13 Jacek Ciborowski , Jakub Rembielinski

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

The electron neutrino mass has been measured in several tritium beta decay experiments. These experiments are sensitive to a small neutrino mass because the energy release of the decay is small. But the very smallness of the energy release…

High Energy Physics - Phenomenology · Physics 2009-10-28 Lowell Brown , Chengxing Zhai
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