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Related papers: Effective neutrino masses in KATRIN and future tri…

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The Karlsruhe Tritium Neutrino (KATRIN) experiment will provide a measurement of the effective electron-neutrino mass, $m(\nu_e)$, based on a precision measurement of the tritium beta decay spectrum near its endpoint. The effective mass is…

Instrumentation and Detectors · Physics 2018-09-28 Gregg B. Franklin

The properties of neutrinos and especially their rest mass play an important role at the intersections of cosmology, particle physics and astroparticle physics. At present there are two complementary approaches to address this topic in…

High Energy Physics - Experiment · Physics 2019-08-13 Thomas Thümmler

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

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 2007-05-23 Christian Weinheimer

In this contribution we review the status and perspectives of direct neutrino mass experiments. These experiments investigate the kinematics of $\beta$-decays of specific isotopes ($^3$H, $^{187}$Re, $^{163}$Ho) to derive model-independent…

Instrumentation and Detectors · Physics 2013-07-02 G. Drexlin , V. Hannen , S. Mertens , C. Weinheimer

The fact that neutrinos carry a non-vanishing rest mass is evidence of physics beyond the Standard Model of elementary particles. Their absolute mass bears important relevance from particle physics to cosmology. In this work, we report on…

Nuclear Experiment · Physics 2025-09-19 M. Aker , D. Batzler , A. Beglarian , J. Behrens , J. Beisenkötter , M. Biassoni , B. Bieringer , Y. Biondi , F. Block , S. Bobien , M. Böttcher , B. Bornschein , L. Bornschein , T. S. Caldwell , M. Carminati , A. Chatrabhuti , S. Chilingaryan , B. A. Daniel , 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 , C. Fengler , C. Fiorini , J. A. Formaggio , C. Forstner , F. M. Fränkle , K. Gauda , A. S. Gavin , W. Gil , F. Glück , S. Grohmann , R. Grössle , R. Gumbsheimer , N. Gutknecht , V. Hannen , L. Hasselmann , N. Haußmann , K. Helbing , H. Henke , S. Heyns , S. Hickford , R. Hiller , D. Hillesheimer , D. Hinz , T. Höhn , A. Huber , A. Jansen , C. Karl , J. Kellerer , K. Khosonthongkee , M. Kleifges , M. Klein , J. Kohpeiß , C. Köhler , L. Köllenberger , A. Kopmann , N. Kovač , A. Kovalík , H. Krause , L. La Cascio , T. Lasserre , J. Lauer , T. Le , O. Lebeda , B. Lehnert , G. Li , A. Lokhov , M. Machatschek , M. Mark , A. Marsteller , E. L. Martin , 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. Lopez Poyato , S. Pozzi , F. Priester , J. Ráliš , S. Ramachandran , R. G. H. Robertson , C. Rodenbeck , M. Röllig , C. Röttele , M. Ryšavý , R. Sack , A. Saenz , R. Salomon , P. Schäfer , M. Schlösser , K. Schlösser , L. Schlüter , S. Schneidewind , U. Schnurr , M. Schrank , J. Schürmann , A. Schütz , A. Schwemmer , A. Schwenck , M. Šefčík , D. Siegmann , F. Simon , 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 , S. Tirolf , N. Titov , I. Tkachev , K. Urban , K. Valerius , D. Vénos , C. Weinheimer , S. Welte , J. Wendel , C. Wiesinger , J. F. Wilkerson , J. Wolf , S. Wüstling , J. Wydra , W. Xu , S. Zadorozhny , G. Zeller

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

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

We report on the neutrino mass measurement result from the first four-week science run of the Karlsruhe Tritium Neutrino experiment KATRIN in spring 2019. Beta-decay electrons from a high-purity gaseous molecular tritium source are energy…

High Energy Physics - Experiment · Physics 2019-12-04 M. Aker , K. Altenmüller , M. Arenz , M. Babutzka , J. Barrett , S. Bauer , M. Beck , A. Beglarian , J. Behrens , T. Bergmann , U. Besserer , K. Blaum , F. Block , S. Bobien , K. Bokeloh , J. Bonn , B. Bornschein , L. Bornschein , H. Bouquet , T. Brunst , T. S. Caldwell , L. La Cascio , S. Chilingaryan , W. Choi , T. J. Corona , K. Debowski , M. Deffert , M. Descher , P. J. Doe , O. Dragoun , G. Drexlin , J. A. Dunmore , S. Dyba , F. Edzards , L. Eisenblätter , K. Eitel , E. Ellinger , R. Engel , S. Enomoto , M. Erhard , D. Eversheim , M. Fedkevych , A. Felden , S. Fischer , B. Flatt , J. A. Formaggio , F. M. Fränkle , G. B. Franklin , H. Frankrone , F. Friedel , D. Fuchs , A. Fulst , D. Furse , K. Gauda , H. Gemmeke , W. Gil , F. Glück , S. Görhardt , S. Groh , S. Grohmann , R. Grössle , R. Gumbsheimer , M. Ha Minh , M. Hackenjos , V. Hannen , F. Harms , J. Hartmann , N. Haußmann , F. Heizmann , K. Helbing , S. Hickford , D. Hilk , B. Hillen , D. Hillesheimer , D. Hinz , T. Höhn , B. Holzapfel , S. Holzmann , T. Houdy , M. A. Howe , A. Huber , A. Jansen , A. Kaboth , C. Karl , O. Kazachenko , J. Kellerer , N. Kernert , L. Kippenbrock , M. Kleesiek , M. Klein , C. Köhler , L. Köllenberger , A. Kopmann , M. Korzeczek , A. Kosmider , A. Kovalí , B. Krasch , M. Kraus , H. Krause , L. Kuckert , B. Kuffner , N. Kunka , T. Lasserre , T. L. Le , O. Lebeda , M. Leber , B. Lehnert , J. Letnev , F. Leven , S. Lichter , V. M. Lobashev , A. Lokhov , M. Machatschek , E. Malcherek , K. Müller , M. Mark , A. Marsteller , E. L. Martin , C. Melzer , A. Menshikov , S. Mertens , L. I. Minter , S. Mirz , B. Monreal , P. I. Morales Guzman , K. Müller , U. Naumann , W. Ndeke , H. Neumann , S. Niemes , M. Noe , N. S. Oblath , H. -W. Ortjohann , A. Osipowicz , B. Ostrick , E. Otten , D. S. Parno , D. G. Phillips , P. Plischke , A. Pollithy , A. W. P. Poon , J. Pouryamout , M. Prall , F. Priester , M. Röllig , C. Röttele , P. C. -O. Ranitzsch , O. Rest , R. Rinderspacher , R. G. H. Robertson , C. Rodenbeck , P. Rohr , Ch. Roll , S. Rupp , M. Rysavy , R. Sack , A. Saenz , P. Schäfer , L. Schimpf , K. Schlösser , M. Schlösser , L. Schlüter , H. Schön , K. Schönung , M. Schrank , B. Schulz , J. Schwarz , H. Seitz-Moskaliuk , W. Seller , V. Sibille , D. Siegmann , A. Skasyrskaya , M. Slezak , A. Spalek , F. Spanier , M. Steidl , N. Steinbrink , M. Sturm , M. Suesser , M. Sun , D. Tcherniakhovski , H. H. Telle , T. Thümmler , L. A. Thorne , N. Titov , I. Tkachev , N. Trost , K. Urban , D. Venos , K. Valerius , B. A. VanDevender , R. Vianden , A. P. Vizcaya Hernandez , B. L. Wall , S. Wüstling , M. Weber , C. Weinheimer , C. Weiss , S. Welte , J. Wendel , K. J. Wierman , J. F. Wilkerson , J. Wolf , W. Xu , Y. -R. Yen , M. Zacher , S. Zadorozhny , M. Zboril , G. Zeller

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

Neutrino masses are yet unknown. We discuss the present state of effective electron anti-neutrino mass from $\beta$ decay experiments; effective Majorana neutrino mass from neutrinoless double-beta decay experiments; neutrino mass squared…

High Energy Physics - Experiment · Physics 2023-10-31 Jyotsna Singh , M. Ibrahim Mirza

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

In the presence of mixing between massive neutrino states, the distortion of the electron spectrum in beta decay is, in general, a function of several masses and mixing angles. For $3\nu$-schemes which describe the solar and atmospheric…

High Energy Physics - Phenomenology · Physics 2009-11-07 Y. Farzan , A. Yu. Smirnov

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

The investigation of the endpoint region of the tritium beta decay spectrum is still the most sensitive direct method to determine the neutrino mass scale. In the nineties and the beginning of this century the tritium beta decay experiments…

High Energy Physics - Experiment · Physics 2009-12-10 C. Weinheimer

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

Taking as input the best fit solar neutrino anomaly description, MSW LMA, and the tritium beta decay results we estimate the allowed range of neutrino masses independently of their nature. Adding the present bound on the effective neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Czakon , J. Gluza , J. Studnik , M. Zralek

We discuss the physics potential of future tritium beta-decay experiments having a sensitivity to a neutrino mass ~\sqrt{|\Delta m^{2}_{23}|}~5x10^{-2} eV. The case of three-neutrino mixing is analised. A negative result of such an…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. M. Bilenky , M. D. Mateev , S. T. Petcov

The determination of the neutrino mass is one of the major challenges in astroparticle physics today. Direct neutrino mass experiments, based solely on the kinematics of beta-decay, provide a largely model-independent probe to the neutrino…

Instrumentation and Detectors · Physics 2020-04-22 M. Aker , K. Altenmüller , M. Arenz , W. -J. Baek , J. Barrett , A. Beglarian , J. Behrens , A. Berlev , U. Besserer , K. Blaum , F. Block , S. Bobien , B. Bornschein , L. Bornschein , H. Bouquet , T. Brunst , T. S. Caldwell , S. Chilingaryan , W. Choi , K. Debowski , M. Deffert , M. Descher , D. Díaz Barrero , P. J. Doe , O. Dragoun , G. Drexlin , S. Dyba , F. Edzards , K. Eitel , E. Ellinger , R. Engel , S. Enomoto , D. Eversheim , M. Fedkevych , A. Felden , J. A. Formaggio , F. M. Fränkle , G. B. Franklin , H. Frankrone , F. Friedel , D. Fuchs , A. Fulst , K. Gauda , W. Gil , F. Glück , S. Grohmann , R. Grössle , R. Gumbsheimer , M. Hackenjos , V. Hannen , J. Hartmann , N. Haußmann , M. Ha Minh , F. Heizmann , J. Heizmann , K. Helbing , S. Hickford , D. Hillesheimer , D. Hinz , T. Höhn , B. Holzapfel , S. Holzmann , T. Houdy , M. A. Howe , A. Huber , A. Jansen , C. Karl , J. Kellerer , N. Kernert , L. Kippenbrock , M. Kleesiek , M. Klein , C. Köhler , L. Köllenberger , A. Kopmann , M. Korzeczek , A. Kovalík , B. Krasch , H. Krause , B. Kuffner , N. Kunka , T. Lasserre , L. La Cascio , O. Lebeda , M. Lebert , B. Lehnert , J. Letnev , F. Leven , T. L. Le , S. Lichter , A. Lokhov , M. Machatschek , E. Malcherek , M. Mark , A. Marsteller , E. L. Martin , F. Megas , C. Melzer , A. Menshikov , S. Mertens , M. Meier , S. Mirz , B. Monreal , P. I. Morales Guzmán , K. Müller , U. Naumann , H. Neumann , S. Niemes , M. Noe , A. Off , H. -W. Ortjohann , A. Osipowicz , E. Otten , D. S. Parno , A. Pollithy , A. W. P. Poon , J. M. L. Poyato , F. Priester , P. C. -O. Ranitzsch , O. Rest , R. Rinderspacher , R. G. H. Robertson , C. Rodenbeck , P. Rohr , M. Röllig , C. Röttele , M. Ryšavý , R. Sack , A. Saenz , P. Schäfer , L. Schimpf , K. Schlösser , M. Schlösser , L. Schlüter , M. Schrank , B. Schulz , H. Seitz-Moskaliuk , W. Seller , V. Sibille , D. Siegmann , M. Slezák , F. Spanier , M. Steidl , M. Steven , M. Sturm , M. Suesser , M. Sun , D. Tcherniakhovski , H. H. Telle , L. A. Thorne , T. Thümmler , N. Titov , I. Tkachev , N. Trost , K. Urban , K. Valerius , D. Vénos , R. Vianden , A. P. Vizcaya Hernández , M. Weber , C. Weinheimer , C. Weiss , S. Welte , J. Wendel , J. F. Wilkerson , J. Wolf , S. Wüstling , W. Xu , Y. -R. Yen , S. Zadorozhny , G. Zeller

Although neutrinos are probably the most abundant particles of the universe their mass is not yet known. Oscillation experiments have proven that at least one of the neutrino mass states has m_{i}>0.05 eV while various interpretations of…

High Energy Physics - Experiment · Physics 2016-10-13 Otokar Dragoun , Drahoslav Vénos
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