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The KATRIN experiment is designed to determine the absolute neutrino mass scale with a sensitivity of 200 meV (90 % CL) by measuring the electron energy spectrum close to the endpoint of molecular tritium beta decay. Electrons from a…

Instrumentation and Detectors · Physics 2013-04-25 Ferenc Glück , Guido Drexlin , Benjamin Leiber , Susanne Mertens , Alexander Osipowicz , Jan Reich , Nancy Wandkowsky

ADC non-linearities are a major systematic effect in the search for keV-scale sterile neutrinos with tritium $\beta$-decay experiments like KATRIN. They can significantly distort the spectral shape and thereby obscure the tiny kink-like…

Instrumentation and Detectors · Physics 2017-03-08 K. Dolde , S. Mertens , D. Radford , T. Bode , A. Huber , M. Korzeczek , T. Lasserre , M. Slezak

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

Sterile neutrinos are hypothetical particles in the minimal extension of the Standard Model of Particle Physics. They could be viable dark matter candidates if they have a mass in the keV range. The Karlsruhe tritium neutrino (KATRIN)…

The KATRIN experiment aims to determine the effective electron neutrino mass with a sensitivity of $0.2\,{\text{eV}/c^2}$ (90\% C.L.) by precision measurement of the shape of the tritium \textbeta-spectrum in the endpoint region. The energy…

Instrumentation and Detectors · Physics 2018-10-02 KATRIN Collaboration , M. Arenz , W. -J. Baek , S. Bauer , M. Beck , A. Beglarian , J. Behrens , R. Berendes , T. Bergmann , A. Berlev , U. Besserer , K. Blaum , T. Bode , B. Bornschein , L. Bornschein , T. Brunst , W. Buglak , N. Buzinsky , S. Chilingaryan , W. Q. Choi , M. Deffert , P. J. Doe , O. Dragoun , G. Drexlin , S. Dyba , F. Edzards , K. Eitel , E. Ellinger , R. Engel , S. Enomoto , M. Erhard , D. Eversheim , M. Fedkevych , J. A. Formaggio , F. M. Fränkle , G. B. Franklin , F. Friedel , A. Fulst , D. Furse , W. Gil , F. Glück , A. Gonzalez Urena , S. Grohmann , R. Grössle , R. Gumbsheimer , M. Hackenjos , V. Hannen , F. Harms , N. Haußmann , F. Heizmann , K. Helbing , W. Herz , S. Hickford , D. Hilk , M. A. Howe , A. Huber , A. Jansen , J. Kellerer , N. Kernert , L. Kippenbrock , M. Kleesiek , M. Klein , A. Kopmann , M. Korzeczek , A. Kovalík , B. Krasch , M. Kraus , L. Kuckert , T. Lasserre , O. Lebeda , J. Letnev , A. Lokhov , M. Machatschek , A. Marsteller , E. L. Martin , S. Mertens , S. Mirz , B. Monreal , H. Neumann , S. Niemes , A. Off , A. Osipowicz , E. Otten , D. S. Parno , A. Pollithy , A. W. P. Poon , F. Priester , P. C. -O. Ranitzsch , O. Rest , R. G. H. Robertson , F. Roccati , C. Rodenbeck , M. Röllig , C. Röttele , M. Ryšavý , R. Sack , A. Saenz , L. Schimpf , K. Schlösser , M. Schlösser , K. Schönung , M. Schrank , H. Seitz-Moskaliuk , J. Sentkerestiová , V. Sibille , M. Slezák , M. Steidl , N. Steinbrink , M. Sturm , M. Suchopar , H. H. Telle , L. A. Thorne , T. Thümmler , N. Titov , I. Tkachev , N. Trost , K. Valerius , D. Vénos , R. Vianden , A. P. Vizcaya Hernández , N. Wandkowsky , M. Weber , C. Weinheimer , C. Weiss , S. Welte , J. Wendel , J. F. Wilkerson , J. Wolf , S. Wüstling , S. Zadoroghny

We consider the effect of general neutrino interactions (scalar, vector, pseudoscalar, axial vector and tensor) in neutrino-electron scattering at the DUNE near detector. Those interactions can be associated with heavy new physics and their…

High Energy Physics - Phenomenology · Physics 2019-02-13 Ingolf Bischer , Werner Rodejohann

The aim of the Karlsruhe Tritium Neutrino experiment (KATRIN) is the direct (model-independent) measurement of the neutrino mass. For that purpose a windowless gaseous tritium source is used, with a tritium throughput of 40 g/day. In order…

Instrumentation and Detectors · Physics 2012-03-20 M. Schlösser , S. Fischer , M. Hötzel , W. Käfer

The KATRIN experiment in Karlsruhe Germany will monitor the decay of tritium, which produces an electron-antineutrino. While the present upper bound for its mass is 2 eV/$c^2$, KATRIN will search down to 0.2 eV$/c^2$. If the dark matter of…

Cosmology and Nongalactic Astrophysics · Physics 2011-04-01 Theo M. Nieuwenhuizen , Andrea Morandi

We investigate neutrino-nucleus interactions at energies around 1 GeV. In this regime, the main contributions to the cross sections come from quasi-elastic and $\Delta$ production processes. Our formalism, based on the Impulse Approximation…

High Energy Physics - Phenomenology · Physics 2008-11-26 Omar Benhar , Davide Meloni

We investigate the sensitivity of the FASER$\nu$ detector, a novel experimental setup at the LHC, to probe and constrain generalized neutrino interactions (GNI). Employing a comprehensive theoretical framework, we model the effects of…

High Energy Physics - Phenomenology · Physics 2023-08-31 F. J. Escrihuela , L. J. Flores , O. G. Miranda , Javier Rendón , R. Sánchez-Vélez

Experimental results and perspectives of different methods to measure the absolute mass scale of neutrinos are briefly reviewed. The mass sensitivities from cosmological observations, double beta decay searches and single beta decay…

Nuclear Experiment · Physics 2009-06-03 Markus Steidl

The interference of charge-changing interactions, weaker than the V-A Standard Model (SM) interaction and having a different Lorentz structure, with that SM interaction, can, in principle, produce effects near the end point of the Tritium…

High Energy Physics - Phenomenology · Physics 2012-08-27 G. J. Stephenson, , T. Goldman , B. H. J. McKellar

We present a showcase for deriving bounds on the neutrino masses from laboratory experiments and cosmological observations. We compare the frequentist and Bayesian bounds on the effective electron neutrino mass m_beta which the KATRIN…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ole Host , Ofer Lahav , Filipe B. Abdalla , Klaus Eitel

In this work, we present the first spectroscopic measurements of conversion electrons originating from the decay of metastable gaseous $^\mathrm{83m}$Kr with the Karlsruhe Tritium Neutrino (KATRIN) experiment. The results obtained in this…

Instrumentation and Detectors · Physics 2020-06-24 K. Altenmüller , M. Arenz , W. -J. Baek , M. Beck , A. Beglarian , J. Behrens , T. Bergmann , A. Berlev , U. Besserer , K. Blaum , F. Block , S. Bobien , T. Bode , B. Bornschein , L. Bornschein , T. Brunst , N. Buzinsky , S. Chilingaryan , W. Q. Choi , M. Deffert , P. J. Doe , O. Dragoun , G. Drexlin , S. Dyba , F. Edzards , K. Eitel , E. Ellinger , R. Engel , S. Enomoto , D. Eversheim , M. Fedkevych , J. A. Formaggio , F. M. Fränkle , G. B. Franklin , F. Friedel , A. Fulst , W. Gil , F. Glück , A. Gonzalez Ureña , S. Grohmann , R. Grössle , R. Gumbsheimer , M. Hackenjos , V. Hannen , F. Harms , N. Haußmann , F. Heizmann , K. Helbing , S. Hickford , D. Hilk , D. Hillesheimer , D. Hinz , M. A. Howe , A. Huber , A. Jansen , J. Kellerer , N. Kernert , L. Kippenbrock , M. Klein , A. Kopmann , M. Korzeczek , A. Kovalík , B. Krasch , M. Kraus , T. Lasserre , O. Lebeda , J. Letnev , A. Lokhov , M. Machatschek , A. Marsteller , E. L. Martin , S. Mertens , S. Mirz , B. Monreal , H. Neumann , S. Niemes , A. Off , A. Osipowicz , E. Otten , D. S. Parno , P. Plischke , A. Pollithy , A. W. P. Poon , F. Priester , P. C. -O. Ranitzsch , O. Rest , R. G. H. Robertson , F. Roccati , C. Rodenbeck , M. Röllig , C. Röttele , M. Ryšavý , R. Sack , A. Saenz , L. Schimpf , K. Schlösser , M. Schlösser , K. Schönung , M. Schrank , H. Seitz-Moskaliuk , J. Sentkerestiová , V. Sibille , M. Slezák , M. Steidl , N. Steinbrink , M. Sturm , M. Suchopar , M. Suesser , H. H. Telle , L. A. Thorne , T. Thümmler , N. Titov , I. Tkachev , N. Trost , K. Valerius , D. Vénos , R. Vianden , A. P. Vizcaya Hernández , M. Weber , C. Weinheimer , S. Welte , J. Wendel , J. F. Wilkerson , J. Wolf , S. Wüstling , S. Zadoroghny , G. Zeller

The Karlsruhe Tritium Neutrino Experiment (KATRIN) aims to determine the absolute mass of the electron antineutrino from a precise measurement of the tritium beta-spectrum near its endpoint at 18.6 keV with a sensitivity of 0.2 eV. KATRIN…

Instrumentation and Detectors · Physics 2009-10-29 Th. Thümmler , R. Marx , Ch. Weinheimer

Using the general connection between the upper limit on the neutrino mass and the upper limits on certain types of non-Standard Model interaction that can generate loop corrections to the neutrino mass, we derive constraints on some…

High Energy Physics - Phenomenology · Physics 2007-05-23 Takeyasu M. Ito , Gary Prezeau

The KArlsruhe TRItium Neutrino (KATRIN) experiment aims to search for the effective electron antineutrino mass with a sensitivity of 0.2 eV (90 % C.L.). In order to achieve this goal, KATRIN measurement phases focusing on the neutrino mass…

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

Within the Standard Model, the weak interaction of quarks and leptons is characterized by certain symmetry properties, such as maximal breaking of parity and favored helicity. These are related to the $V-A$ structure of the weak…

Nuclear Experiment · Physics 2017-06-08 Ayala Glick-Magid , Yonatan Mishnayot , Ish Mukul , Michael Hass , Guy Ron , Sergey Vaintraub , Doron Gazit

Neutrino non-standard interactions (NSI) with the first generation of standard model fermions can span a parameter space of large dimension and exhibit degeneracies that cannot be broken by a single class of experiment. Oscillation…

High Energy Physics - Phenomenology · Physics 2020-09-22 Bhaskar Dutta , Rafael F. Lang , Shu Liao , Samiran Sinha , Louis Strigari , Adrian Thompson
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