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The Karlsruhe Tritium Neutrino (KATRIN) experiment investigating tritium beta-decay close to the endpoint with unprecedented precision has stringent requirements on the background level of less than 10^(-2) counts per second. Electron…

Instrumentation and Detectors · Physics 2015-06-15 N. Wandkowsky , G. Drexlin , F. M. Fränkle , F. Glück , S. Groh , S. Mertens

To resolve the effective neutrino mass $m_\beta$ with an energy resolution of 50~meV, the PTOLEMY experiment has proposed a novel transverse electromagnetic filtering process. Substantially reducing the kinetic energy of tritium…

The new concept of antineutrino source for future short-baseline experiments is discussed. The source ensures: 1) well defined hard antineutrino flux; 2) the rate of counts more than ~(1E+2 - 1E+3) per day in the detector volume about cubic…

Instrumentation and Detectors · Physics 2022-10-12 V. I. Lyashuk

The Gallium anomaly is an unexplained deficit in the neutrinos observed during the calibration of GALLEX and SAGE using a $^{51}$Cr radioactive source and recently confirmed by BEST. The possible explanations for this deficit include an…

High Energy Physics - Phenomenology · Physics 2025-04-30 Emilio Ciuffoli , Jarah Evslin , Ruixuan Gao , Haixing Lin , Jian Tang

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

This paper introduces a novel, high-intensity source of electron antineutrinos from the production and subsequent decay of 8Li. When paired with an existing ~1 kton scintillator-based detector, this <E_\nu>=6.4 MeV source opens a wide range…

A sterile neutrino with mass in the eV range, mixing with the electron antineutrino, is allowed and possibly even preferred by cosmology and oscillation experiments. If such eV-mass neutrinos exist they provide a much better target for…

Cosmology and Nongalactic Astrophysics · Physics 2011-03-18 Anna Sejersen Riis , Steen Hannestad

The standard three-neutrino oscillation paradigm, associated with small squared mass splittings $\ll 0.1\ \mathrm{eV^2}$, has been successfully built up over the last 15 years using solar, atmospheric, long baseline accelerator and reactor…

Instrumentation and Detectors · Physics 2015-04-16 J. Gaffiot , T. Lasserre , G. Mention , M. Vivier , M. Cribier , M. Durero , V. Fischer , A. Letourneau , E. Dumonteil , I. S. Saldikov , G. V. Tikhomirov

We propose a concept for a cryogenic source of atomic tritium at sub-Kelvin temperatures and energies suitable for magnetic trapping. The source is based on the dissociation of solid molecular T2 films below 1 K by electrons from a pulsed…

The determination of the absolute scale of the neutrino masses is one of the most challenging present questions in particle physics. The most stringent limit, $m(\bar{\nu}_{\mathrm{e}})<2$eV, was achieved for the electron anti-neutrino mass…

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 KArlsruhe TRItium Neutrino (KATRIN) experiment, which aims to make a direct and model-independent determination of the absolute neutrino mass scale, is a complex experiment with many components. More than 15 years ago, we published a…

Instrumentation and Detectors · Physics 2021-09-01 M. Aker , K. Altenmüller , J. F. Amsbaugh , M. Arenz , M. Babutzka , J. Bast , S. Bauer , H. Bechtler , M. Beck , A. Beglarian , J. Behrens , B. Bender , R. Berendes , A. Berlev , U. Besserer , C. Bettin , B. Bieringer , K. Blaum , F. Block , S. Bobien , J. Bohn , K. Bokeloh , H. Bolz , B. Bornschein , L. Bornschein , M. Böttcher , H. Bouquet , N. M. Boyd , T. Brunst , T. H. Burritt , T. S. Caldwell , Z. Chaoui , S. Chilingaryan , W. Choi , T. J. Corona , G. A. Cox , K. Debowski , M. Deffert , M. Descher , D. Díaz Barrero , P. J. Doe , O. Dragoun , G. Drexlin , J. A. Dunmore , S. Dyba , F. Edzards , F. Eichelhardt , K. Eitel , E. Ellinger , R. Engel , S. Enomoto , M. Erhard , D. Eversheim , M. Fedkevych , A. Felden , S. Fischer , J. A. Formaggio , F. M. Fränkle , G. B. Franklin , H. Frenzel , F. Friedel , A. Fulst , K. Gauda , R. Gehring , W. Gil , F. Glück , S. Görhardt , J. Grimm , S. Grohmann , S. Groh , R. Grössle , R. Gumbsheimer , M. Hackenjos , D. Häßler , V. Hannen , F. Harms , G. C. Harper , J. Hartmann , N. Haußmann , F. Heizmann , K. Helbing , M. Held , S. Hickford , D. Hilk , B. Hillen , R. Hiller , D. Hillesheimer , D. Hinz , T. Höhn , S. Holzmann , S. Horn , M. Hötzel , T. Houdy , M. A. Howe , A. Huber , T. James , A. Jansen , M. Kaiser , C. Karl , O. Kazachenko , J. Kellerer , L. Kippenbrock , M. Kleesiek , M. Kleifges , J. Kleinfeller , M. Klein , L. Köllenberger , A. Kopmann , M. Korzeczek , A. Kosmider , A. Kovalík , B. Krasch , H. Krause , M. Kraus , L. Kuckert , A. Kumb , N. Kunka , T. Lasserre , L. La Cascio , O. Lebeda , M. L. Leber , B. Lehnert , B. Leiber , J. Letnev , R. J. Lewis , T. L. Le , S. Lichter , A. Lokhov , J. M. Lopez Poyato , M. Machatschek , E. Malcherek , M. Mark , A. Marsteller , E. L. Martin , K. Mehret , M. Meloni , C. Melzer , A. Menshikov , S. Mertens , L. I. Minter , B. Monreal , J. Mostafa , K. Müller , A. W. Myers , U. Naumann , H. Neumann , S. Niemes , P. Oelpmann , A. Off , H. -W. Ortjohann , A. Osipowicz , B. Ostrick , D. S. Parno , D. A. Peterson , P. Plischke , A. W. P. Poon , M. Prall , F. Priester , P. C. -O. Ranitzsch , J. Reich , P. Renschler , O. Rest , R. Rinderspacher , R. G. H. Robertson , W. Rodejohann , C. Rodenbeck , P. Rohr , M. Röllig , C. Röttele , S. Rupp , M. Ryšavý , R. Sack , A. Saenz , M. Sagawe , P. Schäfer , A. Schaller , L. Schimpf , K. Schlösser , M. Schlösser , L. Schlüter , S. Schneidewind , H. Schön , K. Schönung , M. Schrank , B. Schulz , J. Schwarz , M. Šefčík , H. Seitz-Moskaliuk , W. Seller , V. Sibille , D. Siegmann , M. Slezák , F. Spanier , M. Steidl , M. Sturm , M. Sun , D. Tcherniakhovski , H. H. Telle , L. A. Thorne , T. Thümmler , N. Titov , I. Tkachev , N. Trost , K. Valerius , B. A. VanDevender , T. D. Van Wechel , D. Vénos , A. Verbeek , R. Vianden , A. P. Vizcaya Hernández , K. Vogt , B. L. Wall , N. Wandkowsky , M. Weber , H. Weingardt , C. Weinheimer , C. Weiss , S. Welte , J. Wendel , K. J. Wierman , J. F. Wilkerson , J. Wolf , S. Wüstling , W. Xu , Y. -R. Yen , M. Zacher , S. Zadoroghny , M. Zboril , G. Zeller

We propose an experimental setup to observe coherent elastic neutrino-atom scattering (CE$\nu$AS) using electron antineutrinos from tritium decay and a liquid helium target. In this scattering process with the whole atom, that has not beeen…

High Energy Physics - Phenomenology · Physics 2019-11-06 M. Cadeddu , F. Dordei , C. Giunti , K. A. Kouzakov , E. Picciau , A. I. Studenikin

Sterile neutrinos are a minimal extension of the Standard Model of Particle Physics. A promising model-independent way to search for sterile neutrinos is via high-precision beta spectroscopy. The Karlsruhe Tritium Neutrino (KATRIN)…

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

Electron diffraction through a thin patterned silicon membrane can be used to create complex spatial modulations in electron distributions by varying the intensity of different reflections using parameters such as crystallographic…

Accelerator Physics · Physics 2019-05-30 L. E. Malin , W. S. Graves , M. Holl , J. C. H. Spence , E. A. Nanni , R. K. Li , X. Shen , S. Weathersby

An electron-impact ion source based on photoelectron emission was developed for ionization of gases at pressures below 1e-4 mbar in an axial magnetic field in the order of 5 T. The ion source applies only DC fields, which makes it suitable…

Instrumentation and Detectors · Physics 2011-01-25 S. Lukic , B. Bornschein , G. Drexlin , F. Glück , O. Kazachenko , M. Schöppner , Ch. Weinheimer , M. C. R. Zoll

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 KATRIN experiment will determine the effective electron anti-neutrino mass with a sensitivity of 200 meV/c$^2$ at 90% CL. The energy analysis of tritium $\beta$-decay electrons will be performed by a tandem setup of electrostatic…

Sterile neutrinos in the mass range of a few keV are candidates for both cold and warm dark matter. An ad-mixture of a heavy neutrino mass eigenstate to the electron neutrino would result in a minuscule distortion - a 'kink' - in a…

High Energy Physics - Phenomenology · Physics 2015-03-05 S. Mertens , K. Dolde , M. Korzeczek , F. Glueck , S. Groh , R. D. Martin , A. W. P. Poon , M. Steidl
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