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Dive into the research topics where O. Kazachenko is active.

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Featured researches published by O. Kazachenko.


Physics Letters B | 1999

High precision measurement of the tritium β spectrum near its endpoint and upper limit on the neutrino mass

Ch. Weinheimer; B. Degenddag; A. Bleile; J. Bonn; L. Bornschein; O. Kazachenko; A. Kovalik; E. W. Otten

Abstract The Mainz neutrino mass experiment investigates the endpoint region of the tritium β decay spectrum to determine the mass of the electron antineutrino. By the recent upgrade the former problem of dewetting T2 films has been solved and the signal-to-background-ratio was improved by a factor of 10. The latest measurement leads to m ν 2 =−3.7±5.3 stat ±2.1 sys eV 2 /c 4 , from which an upper limit of m ν eV/c 2 (95% C.L.) is derived. Some indication for the anomaly, reported by the Troitsk group, was found, but its postulated half year period is contradicted by our data.


Nuclear Physics B - Proceedings Supplements | 2001

Direct search for neutrino mass and anomaly in the tritium beta-spectrum: Status of “Troitsk neutrino mass” experiment

V.M. Lobashev; V.N Aseev; A.I. Belesev; A.I. Berlev; E.V. Geraskin; A.A. Golubev; O. Kazachenko; Yu.E. Kuznetsov; R.P Ostroumov; L.A Rivkis; B.E. Stern; N. A. Titov; C.V Zadoroghny; Yu.I. Zakharov

Abstract Results of the “Troitsk ν-mass” experiment on search for the neutrino rest mass in the tritium beta-decay are presented. New data on the time dependence of the anomalous, bump-like structure at the end of the beta spectrum reported earlier are discussed. Possible systematics is considered in view of contradiction of “Troitsk nu-mass” observation with those of “Mainz neutrino” set-up. An upper limit for electron antineutrino rest mass remains at m ν 2.5eV c 2 at 95% C.L.


Proceedings of International Europhysics Conference on High Energy Physics — PoS(hep2001) | 2001

The Mainz neutrino mass experiment

J. Bonn; H. Ulrich; Ch. Weinheimer; A. Kovalik; E. W. Otten; O. Kazachenko; L. Fickinger; Ch. Kraus; J.P. Schall; B. Flatt; L. Bornschein; B. Bornschein

Abstract The Mainz neutrino mass experiment is investigating the endpoint region of the tritium β decay spectrum to determine the mass of the electron antineutrino. With its recently improved setup data were taken over more than 7 month in 1998 and 1999. For these measurements two different analyses are presented leading to mv2 = +0.6±2.8±2.1 eV2/c4and mv2 = −1.6 ± 2.5 ± 2.1 eV2/c4, from which upper limits of mv


Nuclear Physics B - Proceedings Supplements | 1999

Neutrino mass and anomaly in the tritium beta-spectrum. Results of the “Troitsk ν-mass” experiment

V.M. Lobashev; V.N Aseev; A.I. Belesev; A.I. Berlev; E.V. Geraskin; A.A. Golubev; N. Golubev; O. Kazachenko; Yu.E. Kuznetsov; R.P Ostroumov; L.A. Ryvkis; B.E. Stern; N. A. Titov; S.V. Zadorozhny; Yu.I. Zakharov

Abstract Results of the “Troitsk ν-mass” experiment on the search for the neutrino rest mass in the tritium beta-decay are presented. Study of time dependence of anomalious, bump-like structure at the end of beta spectrum reported earlier gives indication of periodic shift of the position of the bump with respect to end-point energy with period of 0.5 year. New upper limit for electron antineutrino rest mass m ν eV / c 2 is derived after accounting for the bump. Possible variants of more sensitive facility are discussed.


Nuclear Physics B - Proceedings Supplements | 2000

Newest results from the Mainz neutrino mass experiment

J. Bonn; B. Bornschein; L. Bornschein; L. Fickinger; O. Kazachenko; A. Kovalik; Ch. Kraus; H. Ulrich; E. W. Otten; Ch. Weinheimer

The Mainz neutrino-mass experiment investigates the endpoint region of the tritium β-decay spectrum with a MAC-E spectrometer to determine the mass of the electron antineutrino. By the recent upgrade, the former problem of dewetting T2 films has been solved, and the signal-to-background ratio was improved by a factor of 10. The latest measurement leads to \(m_\nu ^2 = - 3.7 \pm 5.3(stat.) \pm 2.1(syst.){{eV^2 } \mathord{\left/ {\vphantom {{eV^2 } {c^4 }}} \right. \kern-\nulldelimiterspace} {c^4 }}\), from which an upper limit of \(m_\nu < 2.8{{eV^2 } \mathord{\left/ {\vphantom {{eV^2 } {c^2 }}} \right. \kern-\nulldelimiterspace} {c^2 }}(95\% C.L.)\) is derived. Some indication for the anomaly, reported by the Troitsk group, was found, but its postulated half-year period is contradicted by our data. To push the sensitivity on the neutrino mass below 1 eV/c2, a new larger MAC-E spectrometer is proposed. Besides its integrating mode, it could run in a new nonintegration operation MAC-E-TOF mode.


Review of Scientific Instruments | 2011

Ion source for tests of ion behavior in the Karlsruhe tritium neutrino experiment beam line

S. Lukic; B. Bornschein; G. Drexlin; F. Glück; O. Kazachenko; M. Schöppner; Ch. Weinheimer; M. C. R. Zoll

An electron-impact ion source based on photoelectron emission was developed for ionization of gases at pressures below 10(-4) mbar in an axial magnetic field in the order of 5 T. The ion source applies only dc fields, which makes it suitable for use in the presence of equipment sensitive to radio-frequency (RF) fields. The ion source was successfully tested under varying conditions regarding pressure, magnetic field, and magnetic-field gradient, and the results were studied with the help of simulations. The processes in the ion source are well understood, and possibilities for further optimization of generated ion currents are clarified.An electron-impact ion source based on photoelectron emission was developed for ionization of gases at pressures below 10 mbar in an axial magnetic field in the order of 5 T. The ion source applies only DC fields, which makes it suitable for use in the presence of equipment sensitive to radiofrequency (RF) fields. The ion source was succesfully tested under varying conditions regarding pressure, magnetic field and magnetic-field gradient, and the results were studied with the help of simulations. The processes in the ion source are well understood and possibilities for further optimization of generated ion currents are clarified.


Physics of Atomic Nuclei | 2000

Newest results from the Mainz neutrino-mass experiment

J. Bonn; B. Bornschein; L. Bornschein; L. Fickinger; O. Kazachenko; A. Kovalik; Ch. Kraus; E. W. Otten; H. Ulrich; Ch. Weinheimer

AbstractThe Mainz neutrino-mass experiment investigates the endpoint region of the tritium β-decay spectrum with a MAC-E spectrometer to determine the mass of the electron antineutrino. By the recent upgrade, the former problem of dewetting T2 films has been solved, and the signal-to-background ratio was improved by a factor of 10. The latest measurement leads to


Nuclear Physics B - Proceedings Supplements | 2000

Direct search for mass of neutrino and anomaly in the tritium beta-spectrum

V.M. Lobashev; V.N Aseev; A.I. Belesev; A.I. Berlev; E.V. Geraskin; A.A. Golubev; O. Kazachenko; Yu.E. Kuznetsov; R.P Ostroumov; L.A Rivkis; B.E. Stern; N. A. Titov; C.V Zadoroghny; Yu.I. Zakharov


Nuclear Physics | 1999

New results from the mainz neutrino mass experiment

H. Barth; A. Bleile; J. Bonn; L. Bornschein; B. Degen; L. Fleischmann; O. Kazachenko; A. Kovalik; E. W. Otten; Michael Przyrembel; Ch. Weinheimer

m_\nu ^2 = - 3.7 \pm 5.3(stat.) \pm 2.1(syst.){{eV^2 } \mathord{\left/ {\vphantom {{eV^2 } {c^4 }}} \right. \kern-\nulldelimiterspace} {c^4 }}


Wissenschaftliche Berichte FZKA | 2001

KATRIN - a next generation tritium beta decay experiment with sub-eV sensitivity for the electron neutrino mass

A. Osipowicz; H. Blümer; G. Drexlin; K. Eitel; G. Meisel; P. Plischke; F. Schwamm; M. Steidl; H. Gemmeke; C. Day; R. Gehring; R. Heller; K.P. Jungst; P. Komarek; W. Lehmann; A. Mack; H. Neumann; M. Noe; T. Schneider; L. Dorr; M. Glugla; R. Lässer; T. Kepcija; J. Wolf; J. Bonn; B. Bornschein; L. Bornschein; B. Flatt; Ch. Kraus; B. Müller

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B. Bornschein

Karlsruhe Institute of Technology

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A.I. Belesev

Russian Academy of Sciences

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E.V. Geraskin

Russian Academy of Sciences

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N. A. Titov

Russian Academy of Sciences

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A.I. Berlev

Russian Academy of Sciences

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