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Related papers: KATRIN experiment

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With a mass at least six orders of magnitudes smaller than the mass of an electron -- but non-zero -- neutrinos are a clear misfit in the Standard Model of Particle Physics. On the one hand, its tiny mass makes the neutrino one of the most…

Nuclear Experiment · Physics 2016-06-22 Susanne Mertens

The KArlsruhe TRItium Neutrino experiment (KATRIN) aims to measure the effective electron anti-neutrino mass with an unprecedented sensitivity of 0.2 eV/c$^2$, using beta-electrons from tritium decay. Super-conducting magnets will guide the…

Instrumentation and Detectors · Physics 2018-07-31 F. Friedel , C. Röttele , L. Schimpf , G. Drexlin , M. Hackenjos , A. Jansen , M. Steidl , K. Valerius , J. Wolf

We perform a statistical analysis with the prospective results of future experiments on neutrino-less double beta decay, direct searches for neutrino mass (KATRIN) and cosmological observations. Realistic errors are used and the nuclear…

High Energy Physics - Phenomenology · Physics 2009-07-24 Werner Maneschg , Alexander Merle , Werner Rodejohann

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

The \textit{KArlsruhe TRItium Neutrino} (KATRIN) experiment aims to measure the neutrino mass with a sensitivity of \SI{0.2}{\electronvolt} (\SI{90}{\percent} CL). This will be achieved by a precision measurement of the endpoint region of…

Instrumentation and Detectors · Physics 2022-03-23 A. Beglarian , E. Ellinger , N. Haußmann , K. Helbing , S. Hickford , U. Naumann , H. -W. Ortjohann , M. Steidl , J. Wolf , S. Wüstling

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

The method of direct neutrino mass determination based on the kinematics of tritium beta decay, which is adopted by the KATRIN experiment, makes use of a large, high-resolution electrostatic spectrometer with magnetic adiabatic collimation.…

Instrumentation and Detectors · Physics 2011-08-09 K. Valerius , H. Hein , H. Baumeister , M. Beck , K. Bokeloh , J. Bonn , F. Glück , H. -W. Ortjohann , B. Ostrick , M. Zbořil , Ch. Weinheimer

Neutrino oscillation and tritium beta decay experiments taken simultaneously into account are able to access the so far imperceptible absolute neutrino masses at the electronvolt level. The neutrino mass spectrum derived in this way is…

High Energy Physics - Phenomenology · Physics 2011-02-21 M. Czakon , J. Gluza , J. Studnik , M. Zralek

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

This proceedings paper briefly reviews the status of direct experimental probes into the neutrino-mass scale, with an emphasis on recent results from the KATRIN experiment.

Nuclear Experiment · Physics 2026-01-06 Diana S. Parno

The KATRIN experiment will probe the neutrino mass by measuring the beta-electron energy spectrum near the endpoint of tritium beta-decay. An integral energy analysis will be performed by an electro-static spectrometer (Main Spectrometer),…

Instrumentation and Detectors · Physics 2016-05-04 M. Arenz , M. Babutzka , M. Bahr , J. P. Barrett , S. Bauer , M. Beck , A. Beglarian , J. Behrens , T. Bergmann , U. Besserer , J. Blümer , L. I. Bodine , K. Bokeloh , J. Bonn , B. Bornschein , L. Bornschein , S. Büsch , T. H. Burritt , S. Chilingaryan , T. J. Corona , L. De Viveiros , P. J. Doe , O. Dragoun , G. Drexlin , S. Dyba , S. Ebenhöch , K. Eitel , E. Ellinger , S. Enomoto , M. Erhard , D. Eversheim , M. Fedkevych , A. Felden , S. Fischer , J. A. Formaggio , F. Fränkle , D. Furse , M. Ghilea , W. Gil , F. Glück , A. Gonzalez Urena , S. Görhardt , S. Groh , S. Grohmann , R. Grössle , R. Gumbsheimer , M. Hackenjos , V. Hannen , F. Harms , N. Hauÿmann , F. Heizmann , K. Helbing , W. Herz , S. Hickford , D. Hilk , B. Hillen , T. Höhn , B. Holzapfel , M. Hötzel , M. A. Howe , A. Huber , A. Jansen , N. Kernert , L. Kippenbrock , M. Kleesiek , M. Klein , A. Kopmann , A. Kosmider , A. Kovalík , B. Krasch , M. Kraus , H. Krause , M. Krause , L. Kuckert , B. Kuffner , L. La Cascio , O. Lebeda , B. Leiber , J. Letnev , V. M. Lobashev , A. Lokhov , E. Malcherek , M. Mark , E. L. Martin , S. Mertens , S. Mirz , B. Monreal , K. Müller , M. Neuberger , H. Neumann , S. Niemes , M. Noe , N. S. Oblath , A. Off , H. -W. Ortjohann , A. Osipowicz , E. Otten , D. S. Parno , P. Plischke , A. W. P. Poon , M. Prall , F. Priester , P. C. -O. Ranitzsch , J. Reich , O. Rest , R. G. H. Robertson , M. Röllig , S. Rosendahl , S. Rupp , M. Rysavy , K. Schlösser , M. Schlösser , K. Schönung , M. Schrank , J. Schwarz , W. Seiler , H. Seitz-Moskaliuk , J. Sentkerestiova , A. Skasyrskaya , M. Slezak , A. Spalek , M. Steidl , N. Steinbrink , M. Sturm , M. Suesser , H. H. Telle , T. Thümmler , N. Titov , I. Tkachev , N. Trost , A. Unru , K. Valerius , D. Venos , R. Vianden , S. Vöcking , B. L. Wall , N. Wandkowsky , M. Weber , C. Weinheimer , C. Weiss , S. Welte , J. Wendel , K. L. Wierman , J. F. Wilkerson , D. Winzen , J. Wolf , S. Wüstling , M. Zacher , S. Zadoroghny , M. Zboril

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…

With the KATRIN experiment, the determination of the absolute neutrino mass scale down to cosmologically favored values has come into reach. We show that this measurement provides the missing link between the Standard Model and the dark…

High Energy Physics - Phenomenology · Physics 2020-12-04 T. de Boer , M. Klasen , C. Rodenbeck , S. Zeinstra

Recent advances in cosmic observations have brought us to the verge of discovery of the absolute scale of neutrino masses. Nonzero neutrino masses are known evidence of new physics beyond the Standard Model. Our understanding of the…

The KArlsruhe TRItium Neutrino (KATRIN) experiment is a next generation, model independent, large scale tritium beta-decay experiment to determine the effective electron anti-neutrino mass by investigating the kinematics of tritium…

Instrumentation and Detectors · Physics 2011-10-04 F. M. Fränkle , L. Bornschein , G. Drexlin , F. Glück , S. Görhardt , W. Käfer , S. Mertens , N. Wandkowsky , J. Wolf

We introduce a new method to detect the absolute neutrino mass scale. It uses a macroscopic mass of tritium source. We explain that the neutrino mass can be measured by scaling the mass difference of the source between initial and final…

High Energy Physics - Phenomenology · Physics 2014-11-20 Akihiro Matsuzaki , Hidekazu Tanaka

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…

The neutrino mass experiment KATRIN uses conversion electrons from the 32.2 keV transition of the nuclear isomer $^{\mathrm{83m}}$Kr for calibration. Comparing the measured energies to the appropriate literature values allows for an…

Instrumentation and Detectors · Physics 2022-08-23 C. Rodenbeck

The framework of three-flavor neutrino oscillation is a well-established phenomenon, but results from the short-baseline experiments, such as the Liquid Scintillator Neutrino Detector (LSND) and MiniBooster Neutrino Experiment (MiniBooNE),…

High Energy Physics - Phenomenology · Physics 2024-05-08 Srubabati Goswami , Debashis Pachhar , Supriya Pan
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