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The KATRIN experiment is designed for a direct and model-independent determination of the effective electron anti-neutrino mass via a high-precision measurement of the tritium $\beta$-decay endpoint region with a sensitivity on $m_\nu$ of…

Instrumentation and Detectors · Physics 2021-07-21 M. Aker , A. Beglarian , J. Behrens , A. Berlev , U. Besserer , B. Bieringer , F. Block , B. Bornschein , L. Bornschein , M. Böttcher , T. Brunst , T. S. Caldwell , R. M. D. Carney , S. Chilingaryan , W. Choi , K. Debowski , M. Deffert , M. Descher , D. Díaz Barrero , P. J. Doe , O. Dragoun , G. Drexlin , F. Edzards , K. Eitel , E. Ellinger , A. El Miniawy , R. Engel , S. Enomoto , A. Felden , J. A. Formaggio , F. M. Fränkle , G. B. Franklin , F. Friedel , A. Fulst , K. Gauda , W. Gil , F. Glück , S. Groh , R. Grössle , R. Gumbsheimer , V. Hannen , N. Haußmann , F. Heizmann , K. Helbing , S. Hickford , R. Hiller , D. Hillesheimer , D. Hinz , T. Höhn , T. Houdy , A. Huber , A. Jansen , C. Karl , J. Kellerer , M. Kleesiek , M. Klein , C. Köhler , L. Köllenberger , A. Kopmann , M. Korzeczek , A. Kovalík , B. Krasch , H. Krause , N. Kunka , T. Lasserre , L. La Cascio , O. Lebeda , B. Lehnert , T. L. Le , A. Lokhov , M. Machatschek , E. Malcherek , M. Mark , A. Marsteller , E. L. Martin , M. Meier , C. Melzer , A. Menshikov , S. Mertens , J. Mostafa , K. Müller , S. Niemes , P. Oelpmann , D. S. Parno , A. W. P. Poon , J. M. L. Poyato , F. Priester , P. C. -O. Ranitzsch , R. G. H. Robertson , W. Rodejohann , C. Rodenbeck , M. Röllig , C. Röttele , M. Ryšavý , R. Sack , A. Saenz , P. Schäfer , A. Schaller , L. Schimpf , K. Schlösser , M. Schlösser , L. Schlüter , S. Schneidewind , M. Schrank , B. Schulz , C. Schwachtgen , M. Šefčík , H. Seitz-Moskaliuk , V. Sibille , D. Siegmann , M. Slezák , M. Steidl , M. Sturm , M. Sun , D. Tcherniakhovski , H. H. Telle , L. A. Thorne , T. Thümmler , N. Titov , I. Tkachev , N. Trost , K. Urban , K. Valerius , D. Vénos , A. P. Vizcaya Hernández , C. Weinheimer , S. Welte , J. Wendel , J. F. Wilkerson , J. Wolf , S. Wüstling , W. Xu , Y. -R. Yen , S. Zadoroghny , G. Zeller

The aim of the KArlsruhe TRItium Neutrino experiment KATRIN is the determination of the absolute neutrino mass scale down to 0.2 eV, with essentially smaller model dependence than from cosmology and neutrinoless double beta decay. For this…

High Energy Physics - Phenomenology · Physics 2011-09-07 J. Bonn , K. Eitel , F. Glück , D. Sevilla-Sanchez , N. Titov

While the mass differences between neutrino mass states are known, their absolute masses and mass hierarchy have not yet been determined. Determining the mass of neutrinos provides access to physics beyond the Standard Model and the…

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 international project ``Microcalorimeter Arrays for a Rhenium Experiment'' (MARE) aims at the direct and calorimetric measurement of the electron neutrino mass with sub-electronvolt sensitivity. Calorimetric neutrino mass experiments…

High Energy Physics - Experiment · Physics 2019-08-13 A. Nucciotti

The KArlsruhe TRItium Neutrino experiment (KATRIN) aims to measure the absolute neutrino mass scale with an unprecedented sensitivity of 0.2 eV/c2 (90% C.L.), using beta decay electrons from tritium decay. The kinetic energy of the decay…

Instrumentation and Detectors · Physics 2018-09-26 J. Letnev , W. Hazenbiller , A. Osipowicz , A. Beglarian , H. Bouquet , G. Drexlin , F. Glück , J. Garbe , H. Hillmer , P. Marte , T. Thümmler , Ch. Weinheimer

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…

Nuclear Experiment · Physics 2025-09-19 H. Acharya , 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 , 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 , V. Gupta , K. Habib , V. Hannen , L. Hasselmann , K. Helbing , S. Heyns , R. Hiller , D. Hillesheimer , D. Hinz , T. Höhn , A. Huber , A. Jansen , K. Khosonthongkee , M. Klein , J. Kohpeiß , C. Köhler , A. Kopmann , N. Kovac , L. La Cascio , L. Laschinger , T. Lasserre , J. Lauer , T. L. Le , O. Lebeda , B. Lehnert , A. Lokhov , M. Machatschek , M. Mark , A. Marsteller , E. L. Martin , K. McMichael , C. Melzer , S. Mertens , S. Mohanty , J. Mostafa , A. Nava , H. Neumann , S. Niemes , I. Nutini , A. Onillon , R. Ostertag , D. S. Parno , U. Pinsook , J. Plößner , 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 , M. Slezák , K. Schlösser , M. Schlösser , L. Schlüter , S. Schneidewind , U. Schnurr , 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 , K. Trost , K. Valerius , D. Vénos , C. Weinheimer , S. Welte , J. Wendel , C. Wiesinger , J. F. Wilkerson , J. Wolf , S. Wüstling , J. Wydra , W. Xu , G. Zeller

Since the discovery of neutrino oscillations, it is known that neutrinos have small but non-zero masses. The neutrino mass scale, which is of fundamental importance for cosmology, astrophysics and particle physics, can be measured directly…

Nuclear Experiment · Physics 2026-01-13 Guido Drexlin , 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

The atomic transition from an excited state $|{\rm e}\rangle$ to the ground state $|{\rm g}\rangle$ by emitting a neutrino pair and a photon, i.e., $|{\rm e}\rangle \to |{\rm g}\rangle + |\gamma\rangle + |\nu^{}_i\rangle +…

High Energy Physics - Phenomenology · Physics 2016-07-06 Jue Zhang , Shun Zhou

The phenomenology of absolute neutrino masses is reviewed, focusing on tritium beta decay, cosmological measurements and neutrinoless double-beta decay.

High Energy Physics - Phenomenology · Physics 2009-11-10 Carlo Giunti

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

Electron capture can determine the electron neutrino mass, while the beta decay of Tritium measures the electron antineutrino mass and the neutrinoless double beta decay observes the Majorana neutrino mass. Electron capture e. g. on 163Ho…

Nuclear Theory · Physics 2017-04-19 Amand Faessler , Loredana Gastaldo , Fedor Simkovic

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 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…

We give a comprehensive account of our proposed experimental method of using atoms or molecules in order to measure parameters of neutrinos still undetermined; the absolute mass scale, the mass hierarchy pattern (normal or inverted), the…

The standard kinematic method for determining neutrino mass from the beta decay of tritium or other isotope is to measure the shape of the electron spectrum near the endpoint. It has been known for 30 years that a similar distortion of the…

Nuclear Theory · Physics 2015-03-25 R. G. H. Robertson

The Karlsruhe Tritium Neutrino (KATRIN) experiment will measure the absolute mass scale of neutrinos with a sensitivity of $\m_{\nu}$ = 200 meV/c$^2$ by high-precision spectroscopy close to the tritium beta-decay endpoint at 18.6 keV. Its…

Since the discovery of nuclear beta decay, nuclear physicists have studied the weak interaction and the nature of neutrinos. Many recent and current experiments have been focused on the elucidation of neutrino oscillations and neutrino…

Instrumentation and Detectors · Physics 2014-12-04 R. D. McKeown