NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = V.I.Bondarenko Found 9 matches. 2022BO10 Phys.Atomic Nuclei 85, 241 (2022) On Tensor Correlations in the Formation of Charge-Exchange Giant Spin-Multipole Resonances in Medium-Heavy Magic Parent Nuclei NUCLEAR STRUCTURE 208Bi; calculated the Gamow-Teller resonance and its overtone (isovector giant spin-monopole resonance) with a modified version of the particle-hole dispersive optical model (PHDOM) and, as a limiting case, of the continuum random-phase approximation (CRPA).
doi: 10.1134/S106377882203005X
2022BO13 Phys.Rev. C 106, 024331 (2022) Properties of Gamow-Teller and charge-exchange giant spin-monopole resonances in medium-heavy closed-shell parent nuclei: A semimicroscopic description NUCLEAR STRUCTURE 48Ca, 90Zr, 132Sn, 208Pb; calculated Gamow-Teller resonance strength distributions, isovector giant spin-monopole resonance strength distributions in β- and β+ channels, transition densities. Semimicroscopic particle-hole dispersive optical model. Comparison to available experimental data.
doi: 10.1103/PhysRevC.106.024331
1990BO53 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 2071 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.10, 180 (1990) V.I.Bondarenko, V.I.Kauts, M.G.Urin ' Direct ' Photonucleon Reactions NUCLEAR REACTIONS 89Zr, 54,56Fe, 58Ni(γ, n), E < 25 MeV; calculated σ(E) for direct neutron emission. Direct+semi-direct E1 radiative capture.
1988BO35 Yad.Fiz. 48, 623 (1988) V.I.Bondarenko, B.A.Nemashkalo, V.E.Storizhko, M.G.Urin, K.V.Shebeko Partial Cross Sections of the 52Cr(p(pol), γ(i))53Mn Reaction and Radiative Strength Functions in the 53Mn Nucleus NUCLEAR REACTIONS, ICPND 52Cr(polarized p, γ), E=1.5-3.5 MeV; measured σ(E); 53Mn deduced radiative strength function.
1987BO51 Yad.Fiz. 46, 1068 (1987) The Simplest Photonuclear Reactions in the Model of Interacting Independently Damping Quasiparticles NUCLEAR REACTIONS 52Cr(γ, X), E ≈ 12-22 MeV; 89Y(γ, p), E ≈ 13-22 MeV; 56Fe(γ, n), E ≈ 15-26 MeV; 56Fe(γ, p), E ≈ 16-29 MeV; calculated photonuclear σ(E). Independently interacting quasiparticle damping model. NUCLEAR STRUCTURE 52Cr, 89Y, 90Zr, 140Ce, 208Pb; calculated GDR, isospin splitting. Independently interacting quasiparticle damping model.
1986BO42 Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 1821 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 550, No.9, 151 (1986) Adequacy of Optical-Shell Analysis for Partial E1-Transition Strength Function of Compound Resonances NUCLEAR REACTIONS 52,53Cr, 56,57,58Fe, 58,61Ni, 90,91Zr, 140Ce, 208Pb(γ, n), E=6-22 MeV; calculated partial E1 transition strength functions, σ(E). Optical, shell model analyses.
1985BO54 Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 2222 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.11, 131 (1985) On the Partial Cross Sections for Radiative Nucleon Capture with Excitation of Giant Resonances NUCLEAR REACTIONS 90Zr(γ, n), E=13-21 MeV; 140Ce(γ, n), E=11-19 MeV; measured E1 photoneutron production σ(E). 89Y, 140Ce(n, γ), E ≈ 5-14 MeV; calculated partial σ(E).
1983BO25 Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 972 (1983) Description of E1-Giant Resonances in the Framework of the Spherical Optical Model of Nuclear Reactions NUCLEAR REACTIONS 90Zr(γ, X), E=10-25 MeV; 124Sn(γ, X), E=8-25 MeV; 52Cr, 140Ce(γ, X), E=7-25 MeV; 208Pb(γ, X), E=7-20 MeV; 76Se(γ, X), E=8-20 MeV; 60Ni(γ, X), E=1-25 MeV; calculated photoproduction σ(E). Optical model.
1982BO20 Yad.Fiz. 35, 675 (1982) Average Total Radiative Widths of Neutron Resonances and the E1 Transitions between the Nuclear Compound States NUCLEAR REACTIONS 94Mo, 117Sn, 123Sb, 123Te, 143Nd, 198Hg, 230,232Th, 231,233Pa, 234,238U, 239,242Pu, 241Am, 244,246Cm(n, γ), E not given; analyzed E1 photoabsorption data. 95Mo, 118Sn, 124Sb, 124Te, 144Nd, 199Hg, 231,233Th, 232,234Pa, 235,239U, 240,243Pu, 242Am, 245,247Cm resonances deduced total Γγ. Semi-microscopic shell model.
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