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Sterile neutrinos emerge in minimal extensions of the Standard Model which can solve a number of open questions in astroparticle physics. For example, sterile neutrinos in the keV-mass range are viable dark matter candidates. Their…

We present a framework to combine data from the latest neutrinoless double-beta decay experiments for multiple isotopes and derive a limit on the effective neutrino mass using the experimental energy distributions. The combined limits on…

High Energy Physics - Experiment · Physics 2015-06-12 Pawel Guzowski , Luke Barnes , Justin Evans , Georgia Karagiorgi , Nathan McCabe , Stefan Soldner-Rembold

We consider tritium beta decay with additional emission of light pseudoscalar or vector bosons coupling to electrons or neutrinos. The electron energy spectrum for all cases is evaluated and shown to be well estimated by approximated…

The KATRIN (KArlsruhe TRItium Neutrino) experiment will be analyzing the tritium beta-spectrum to determine the mass of the neutrino with a sensitivity of 0.2 eV (90% C.L.). This approach to a measurement of the absolute value of the…

Nuclear Experiment · Physics 2013-05-29 Anna Sejersen Riis , Steen Hannestad , Christian Weinheimer

The determination of the absolute neutrino mass scale remains a fundamental open question in particle physics, with profound implications for both the Standard Model and cosmology. Direct kinematic measurements, independent of…

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 method of the statistical sample moments was used for the analysis of neutrino events from SN1987A burst in Cherenkov detectors. In particular the coefficients of correlation $Q(E,t)$ between the energies $E$ of electron antineutrinos…

Astrophysics · Physics 2007-10-01 B. I. Goryachev

The width for the mu decay is calculated in the V-A theory leaving open the possibility of non zero neutrino masses. It is shown that not only the agreement with the experimental data is kept, but the smallness of the experimental error…

High Energy Physics - Phenomenology · Physics 2026-03-23 M. M. Giannini

We avaluate the contribution of electron scattering on the rear wall of a windowless gaseous tritium source in the Troitsk nu-mass setup. There is a finite probability for them to scatter, return back and reach the detector. A such…

Instrumentation and Detectors · Physics 2024-09-27 V. G. Chernov , V. S. Pantuev

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

Processes of the inelastic magnetic and weak scattering of tritium-beta-source antineutrinos on the bound electrons of a germanium atom are considered. The results obtained by calculating the spectra and cross sections are presented for the…

High Energy Physics - Experiment · Physics 2009-12-17 V. I. Kopeikin , L. A. Mikaelyan , V. V. Sinev

A review of the direct determinations of the upper limit on the tau-neutrino mass from the LEP experiments is given. The experimental methods, the results and the comparison with non LEP measurements are also discussed. The study of the…

High Energy Physics - Experiment · Physics 2007-05-23 F. Cerutti , ALEPH Collaboration

The KArlsruhe TRItium Neutrino experiment (KATRIN) aims to determine the effective mass of the electron antineutrino via a high-precision measurement of the tritium beta-decay spectrum in its end-point region. The target neutrino-mass…

Data Analysis, Statistics and Probability · Physics 2026-04-29 S. Schneidewind , J. Schürmann , A. Lokhov , C. Weinheimer , A. Saenz

In the paper Int.J.Mod.Phys.E 23 (2014) 1450004, the potential of short-baseline experiments was proposed to measure the mass (and parameters of Lorentz-violating effects) of the muon neutrino, where a roughly estimated upper bound of 420…

High Energy Physics - Phenomenology · Physics 2024-05-03 A. M. Attia , I. G. Márián , B. Ujvári

We apply Bayesian methods to study the sensitivity to neutrino masses of a Galactic supernova neutrino signal. Our procedure makes use of the full statistics of events and is remarkably independent of astrophysical assumptions. Present…

High Energy Physics - Phenomenology · Physics 2007-05-23 Enrico Nardi

The issue of step-like anomalies in the tritium \beta-decay spectrum as measured in the Troitsk-\nu-mass experiment is addressed in the context of the new analysis in a systematic fashion using efficient statistical tests specifically…

High Energy Physics - Experiment · Physics 2013-12-02 A. V. Lokhov , F. V. Tkachov , P. S. Trukhanov

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…

Limits at 90 % c.l. on the square of the mixing strength |U_tau4|^2 between nu_tau and a mostly isosinglet heavy neutrino with mass in the range 10-290 MeV/c^2 are reported. The results were derived using the negative result of a search for…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. Orloff , A. Rozanov , C. Santoni

The KATRIN experiment is going to search for the average mass of the electron antineutrino with a sensitivity of 0.2 eV/c2. It uses a retardation spectrometer of MAC-E filter type to accurately measure the shape of the electron spectrum at…

Instrumentation and Detectors · Physics 2015-06-23 M. Beck , K. Bokeloh , H. Hein , S. Bauer , H. Baumeister , J. Bonn , H. -W. Ortjohann , B. Ostrick , S. Rosendahl , S. Streubel , K. Valerius , M. Zboril , C. Weinheimer

The Heidelberg-Moscow experiment gives the most stringent limit on the Majorana neutrino mass. After 24 kg yr of data with pulse shape measurements, we set a lower limit on the half-life of the neutrinoless double beta decay in 76Ge of…