A. V. Ignatyuk
Kurchatov Institute
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Featured researches published by A. V. Ignatyuk.
Physical Review C | 2008
Yu. E. Titarenko; V. F. Batyaev; A. Yu. Titarenko; M. A. Butko; K. V. Pavlov; S. N. Florya; R. S. Tikhonov; S. G. Mashnik; A. V. Ignatyuk; N. N. Titarenko; Waclaw Gudowski; Milan Tesinsky; Carl-Magnus Persson; H. Ait Abderrahim; H. Kumawat; H. Duarte
This work presents the cross sections for radioactive nuclide production in Fe-56( p, x) reactions determined in six experiments using 300, 500, 750, 1000, 1500, and 2600 MeV protons of the externa ...
Physics of Atomic Nuclei | 2011
Yu. E. Titarenko; V. F. Batyaev; A. Yu. Titarenko; M. A. Butko; K. V. Pavlov; S. N. Florya; R. S. Tikhonov; V. M. Zhivun; A. V. Ignatyuk; S. G. Mashnik; S. Leray; A. Boudard; Joseph Cugnon; Davide Mancusi; Y. Yariv; K. Nishihara; N. Matsuda; H. Kumawat; G. Mank; Waclaw Gudowski
The cross sections for nuclide production in thin natWand 181Ta targets irradiated by 0.04–2.6-GeV protons have been measured by direct γ spectrometry using two γ spectrometers with the resolutions of 1.8 and 1.7 keV in the 60Co 1332-keV γ line. As a result, 1895 yields of radioactive residual product nuclei have been obtained. The 27Al(p, x)22Na reaction has been used as a monitor reaction. The experimental data have been compared with the MCNPX (BERTINI, ISABEL), CEM03.02, INCL4.2, INCL4.5, PHITS, and CASCADE07 calculations.
Physics of Atomic Nuclei | 2011
Yu. E. Titarenko; V. F. Batyaev; A. Yu. Titarenko; M. A. Butko; K. V. Pavlov; S. N. Florya; R. S. Tikhonov; V. M. Zhivun; A. V. Ignatyuk; S. G. Mashnik; S. Leray; A. Boudard; Joseph Cugnon; Davide Mancusi; Y. Yariv; K. Nishihara; N. Matsuda; H. Kumawat; G. Mank; Waclaw Gudowski
The cross sections for nuclide production in thin 93Nb and natNi targets irradiated by 0.04- to 2.6-GeV protons have been measured by direct γ spectrometry using two γ spectrometers with the resolutions of 1.8 and 1.7 keV in the 60Co 1332-keV γ line. As a result, 1112 yields of radioactive residual nuclei have been obtained. The 27Al(p, x)22Na reaction has been used as a monitor reaction. The experimental data have been compared with the MCNPX (BERTINI, ISABEL), CEM03.02, INCL4.2, INCL4.5, PHITS, and CASCADE07 calculations.
Physical Review C | 2011
Yu. E. Titarenko; V. F. Batyaev; M. A. Butko; D. V. Dikarev; S. N. Florya; K. V. Pavlov; A. Yu. Titarenko; R. S. Tikhonov; V. M. Zhivun; A. V. Ignatyuk; S. G. Mashnik; A. Boudard; S. Leray; J-C David; Joseph Cugnon; Davide Mancusi; Y. Yariv; H. Kumawat; K. Nishihara; N. Matsuda; G. Mank; Waclaw Gudowski
High-energy transport codes (HETCs) based on various versions of nuclear reaction models [generally, an intranuclear cascade model (INC) followed by different deexcitation models] are widely used in many nuclear centers for the analysis of experimental data, for calculations of nuclear accelerator shielding, and for design of new nuclear facilities. Each of the available codes was developed originally for well-specified tasks and the model parameters were estimated on the basis of fitting the corresponding data. With an expansion of tasks,
Physics of Atomic Nuclei | 2011
Yu. E. Titarenko; V. F. Batyaev; A. Yu. Titarenko; M. A. Butko; K. V. Pavlov; S. N. Florya; R. S. Tikhonov; V. M. Zhivun; A. V. Ignatyuk; S. G. Mashnik; S. Leray; A. Boudard; Joseph Cugnon; Davide Mancusi; Y. Yariv; K. Nishihara; N. Matsuda; H. Kumawat; G. Mank; Waclaw Gudowski
The cross sections for nuclide production in thin 56Fe and natCr targets irradiated by 0.04–2.6-GeV protons are measured by direct γ spectrometry using two γ spectrometers with the resolutions of 1.8 and 1.7 keV for the 60Co 1332-keV γ line. As a result, 649 yields of radioactive residual product nuclei have been obtained. The 27Al(p, x)22Na reaction has been used as a monitor reaction. The experimental data are compared with the MCNPX (BERTINI, ISABEL), CEM03.02, INCL4.2, INCL4.5, PHITS, and CASCADE07 calculations.
Nuclear Science and Engineering | 2000
A. V. Ignatyuk; V. P. Lunev; Y. N. Shubin; E. V. Gai; N. N. Titarenko; A. Ventura; Waclaw Gudowski
Abstract Investigations aimed at the development of neutron cross-section evaluations for 238U at intermediate energies are briefly described. The coupled-channels optical model is used to calculate the neutron total, the elastic and reaction cross sections, and the elastic-scattering angular distributions. Evaluations of the neutron and charged particle emission cross sections and of the fission cross sections are obtained on the basis of the statistical description that includes direct, preequilibrium, and equilibrium mechanisms of nuclear reactions. The Kalbach parameterization of angular distributions is used to describe the double-differential cross sections of emitted neutrons and charged particles in ENDF/B-VI format.
Physics of Atomic Nuclei | 2011
Yu. E. Titarenko; V. F. Batyaev; A. Yu. Titarenko; M. A. Butko; K. V. Pavlov; S. N. Florya; R. S. Tikhonov; V. M. Zhivun; A. V. Ignatyuk; S. G. Mashnik; S. Leray; A. Boudard; Joseph Cugnon; Davide Mancusi; Y. Yariv; K. Nishihara; N. Matsuda; H. Kumawat; G. Mank; Waclaw Gudowski
The cross sections for the production of 148Gd in natW and 181Ta targets irradiated by 0.4-, 0.6-, 0.8-, 1.2-, 1.6-, and 2.6-GeV protons at the ITEP accelerator complex have been measured by direct α spectrometry without chemical separation. The experimental data have been compared with the data obtained at other laboratories and with the theoretical simulations of the yields on the basis of the BERTINI, ISABEL, CEM03.02, INCL4.2, INCL4.5, CASCADE07, and PHITS codes.
Nuclear Science and Engineering | 2002
A. V. Ignatyuk; V. P. Lunev; Y. N. Shubin; E. V. Gai; N. N. Titarenko; Waclaw Gudowski
Abstract Investigations aimed at the development of neutron and proton cross-section evaluations for 232Th at intermediate energies in the range of 0 to 200 MeV are described. The coupled-channel optical model has been used to calculate the neutron total, elastic, and reaction cross sections and the elastic scattering angular distributions. Evaluations of the neutron and charged particle emission cross sections and of the fission cross sections have been obtained on the basis of the statistical description that includes direct, preequilibrium, and equilibrium mechanisms of nuclear reactions. The Kalbach parameterization of angular distributions has been used to describe the double-differential cross sections of emitted neutrons and charged particles in ENDF/B-VI format.
INTERNATIONAL CONFERENCE ON NUCLEAR DATA FOR SCIENCE AND TECHNOLOGY | 2005
V. Artisyuk; A. V. Ignatyuk; Yu. A. Korovin; A. V. Lopatkin; I. Matveenko; A. Stankovskiy; Yu. E. Titarenko
Transmutation of nuclear wastes (Minor Actinides and Long‐Lived Fission Products) remains an important option to reduce the burden of high‐level waste on final waste disposal in deep geological structures. Accelerator‐Driven Systems (ADS) are considered as possible candidates to perform transmutation due to their subcritical operation mode that eliminates some of the serious safety penalties unavoidable in critical reactors. Specific requirements to nuclear data necessary for ADS transmutation analysis is the main subject of the ISTC Project ♯2578 which started in 2004 to identify the areas of research priorities in the future. The present paper gives a summary of ongoing project stressing the importance of nuclear data for blanket performance (reactivity behavior with associated safety characteristics) and uncertainties that affect characteristics of neutron producing target.
INTERNATIONAL CONFERENCE ON NUCLEAR DATA FOR SCIENCE AND TECHNOLOGY | 2005
A. V. Ignatyuk; N. T. Kulagin; V.P. Lunev; Yu.N. Shubin; N. N. Titarenko; V. F. Batyaev; Yu.E. Titarenko; V. M. Zhivun
Spallation and fission residues produced by the proton irradiation of 206Pb, 207Pb, and 208Pb targets at energies from 0.15 up to 2.6 GeV have been studied recently at ITEP. These data allow testing various versions of the intranuclear cascade models widely used for simulation of spallation product yields. The main differences between codes are briefly reviewed. Modifications of the LAHET and CASCADO codes, which are required to reduce the deviations from experimental data, are discussed.