Zobrazeno 1 - 10
of 201
pro vyhledávání: '"M.I. Krivopustov"'
Publikováno v:
HNPS Proceedings. 4:163
We investigate the charge changing collisions for 16O and 32S beams, using the experimental method of Solid State Nuclear Track Detectors (SSNTD). Sample reading was performed by an automatic measurement system. We determined the total charge changin
Publikováno v:
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 664:154-160
Calibration factors w, for determination of fission rate in metallic foils of natU, 235U, 232Th, natPb and 197Au were determined for foils in contact with synthetic mica track detectors. Proton-induced fission at proton energies of 0.7 GeV and 1.5 Ge
Autor:
M. Zamani-Valasiadou, M.I. Krivopustov, R. Brandt, Reinhard Odoj, Wolfgang Ensinger, W. Westmeier, S.R. Hashemi-Nezhad
Publikováno v:
Physics Research International. 2011:1-12
The neutron production in thick targets irradiated with 1 GeV protons was studied experimentally, and results are well understood with model calculations, including MCNPX 2.7a. However, one observes very large neutron production rates in the interact
Publikováno v:
Annals of Nuclear Energy. 37:923-926
The inelastic cross section of relativistic protons in Pb was determined indirectly by measuring the neutron distribution along a Lead spallation neutron source. The spallation neutron source was irradiated by 1, 1.5 and 2 GeV protons. The experiment
Autor:
J. Adam, M.I. Krivopustov, F. Křížek, Mitja Majerle, V. Wagner, A. Kugler, O. Svoboda, A. Krása
Publikováno v:
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 615:70-77
A thick Pb-target with a U-blanket surrounded by a polyethylene moderator was irradiated with 0.7–2.5 GeV proton and deuteron beams. Neutron production was studied with activation detectors. Neutron multiplicity was determined using a modified form
Autor:
Karel Katovsky, V. Kumar, V. M. Tsoupko-Sitnikov, A. A. Solnyshkin, Chitra Bhatia, Mitja Majerle, M.I. Krivopustov, Manish Sharma, J. Adam
Publikováno v:
The European Physical Journal A. 43:159-173
The spallation lead target in the “Energy plus Transmutation” set-up, covered with uranium blanket, was irradiated by the 1.6GeV deuteron beam from the Nuclotron accelerator at the Joint Institute for Nuclear Research in Dubna. The neutrons gener
Autor:
M. Manolopoulou, M. Fragopoulou, A. N. Sosnin, M.I. Krivopustov, Stylianos Stoulos, M. Zamani
Publikováno v:
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. 599:106-112
Spallation sources are able to produce intense neutron fluxes using massive targets when irradiated by relativistic proton beams. Such sub-critical Accelerator Driven Systems (ADSystem) can be used for transmutation or incineration of long-lived radi
Autor:
N. A. Demekhina, J. Adam, G. H. Hovhannisyan, V. M. Tsoupko-Sitnikov, A. S. Danagulyan, A. R. Balabekyan, V. G. Kalinnikov, M.I. Krivopustov
Publikováno v:
Nuclear Physics A. 814:109-117
The analysis of isotope effect in experimental data from reactions on enriched tin isotopes with 12C-ions at energy 26.4 GeV is presented and compared with previous data obtained in protons, deuterons induced reactions on the same targets. Dependence
Autor:
M.I. Krivopustov, W. Westmeier, R. Brandt, A. N. Sosnin, M. Fragopoulou, M. Zamani, Stylianos Stoulos, M. Manolopoulou
Publikováno v:
Radiation Measurements. 43:S151-S155
A new spallation source, efficient for transmutation experiments, was designed and constructed at the Dubna High Energy Laboratory (LHE). The spallation source has a cylindrical shape Pb target surrounded by nat U rods. Experiments with protons of 0.
Publikováno v:
Radiation Measurements. 43:S199-S203
Experiments with a U/Pb assembly (lead target with a natural uranium blanket) were carried out using the nuclotron accelerator of the Joint Institute for Nuclear Research (JINR). The profile of the deuteron beam (E = 1.26GeV/nucleon) and the spatial