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WEZMH01 |
Spallation Neutron Source at the 1 Gev Synchrocyclotron of PNPI |
90 |
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- O.A. Shcherbakov, E.M. Ivanov, G.F. Mikheev, G.A. Petrov, G.A. Riabov, A.S. Vorobyev
PNPI, Gatchina, Leningrad District, Russia
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A description of the spallation pulsed neutron source and neutron time-of-flight spectrometer GNEIS based on the 1 GeV proton synchrocyclotron of PNPI in Gatchina is presented. The main parameters of the neutron source and GNEIS are given in comparison with the analogous world-class facilities. The experimental capabilities of the GNEIS are demonstrated by the examples of some nuclear physics and applied research experiments carried out during four decades of its operation.
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Slides WEZMH01 [32.810 MB]
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THCAMH01 |
Universal Proton and Neutron Centre for Radiation Resistance of Avionic, Space Electronics and Other Applications at 1 Gev Synchrocyclotron in PNPI |
105 |
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- S.A. Artamonov, D.A. Amerkanov, E.M. Ivanov, J.S. Lebedeva, G.F. Mikheev, G.A. Riabov, O.A. Shcherbakov, A.S. Vorobyev
PNPI, Gatchina, Leningrad District, Russia
- V.S. Anashin, L.R. Bakirov, A.E. Koziukov
United Rocket and Space Corporation, Institute of Space Device Engineering, Moscow, Russia
- P.A. Chubunov
ISDE, Moscow, Russia
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In PNPI RNC KI a universal center for testing electronic components for the needs of aviation and space and other applications is created on the synchrocyclotron SC-1000 with the proton energy of 1 GeV. The center consists of two protons and one neutron stands for test facilities developed at the PNPI in collaboration with the ROSCOSMOS Interagency Testing Center. The PNPI center is equipped with all necessary systems of diagnostics and monitoring of a beam, installation of targets on a beam. There is an opportunity to vary temperature of exemplars in the wide range. A unique conjunction of proton beams with variable energy 60-1000 MeV and atmospheric like neutron beam with broad energy range (1-1000 MeV) spectrum enable to perform complex testing of the semiconductor electronic devices at the SC-1000 within a single testing cycle.
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Slides THCAMH01 [11.652 MB]
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TUCASH03 |
High Efficiency Stripping Extraction on 80 MeV H-minus Isochronous Cyclotron in PNPI |
176 |
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- S.A. Artamonov, A.N. Chernov, E.M. Ivanov, G.A. Riabov, V.A. Tonkikh
PNPI, Gatchina, Leningrad District, Russia
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H-minus cyclotron has the advantage that high intensity internal beam can be extracted from the acceleration chamber with practically 100% efficiency by transformation H-minus ions into H-plus ion by using thin foil. The extraction system is consists from the probe with stripping foil, extraction window in the vacuum chamber and two correct magnets to match the extracted beam with beam transport line. The beam optics calculations in the measured magnetic field make it possible to find optimal relative position of the extraction system elements as well the parameters of the extracted beam with energy 40 - 80 MeV. At present time the beam is extracted from the chamber with efficiency 100 % and there is good agreement with the optic calculations.
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Slides TUCASH03 [5.581 MB]
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TUCASH04 |
Physical Start-up of the C-80 Isochronous Cyclotron |
179 |
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- Yu.N. Gavrish, A.V. Galchuck, S.V. Grigorenko, A.N. Kuzhlev, V.G. Mudrolyubov
NIIEFA, St. Petersburg, Russia
- D.A. Amerkanov, S.A. Artamonov, E.M. Ivanov, G.A. Riabov, V.I. Yurchenko
PNPI, Gatchina, Leningrad District, Russia
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Works on the creation of a cyclotron for the acceleration of H− ions at energies ranging from 40 up to 80 MeV have been carried out over a number of years in PNPI, the National Research Centre Kurchatov Institute. The cyclotron is intended for production of a wide assortment of radioisotopes for medicine including radiation generators (Sr-Rb, Ge-Ga), proton therapy of ophthalmic diseases, tests of radioelectronic components for radiation resistance, studies in the field of nuclear physics and radiation material science. In June, 2016 physical start-up of the cyclotron was realized in the pulsed mode; the beam of ~10 mkA was obtained at the inner probe, the extracted beam at the first diagnostic device was ~8 mkA and ~7.5 mkA at the final diagnostic device of the beamline. In the near future we plan to obtain the design intensity of 100 mkA.
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Slides TUCASH04 [13.477 MB]
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