NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = G.I.Kosenko Found 26 matches. 2020LI21 Phys.Rev. C 101, 064616 (2020) V.L.Litnevsky, F.A.Ivanyuk, G.I.Kosenko, S.Chiba Formation of superheavy nuclei in 36S 238U and 64Ni 238U reactions NUCLEAR REACTIONS 238U(36S, X)274Hs*, E*=35.8, 41.6, 47.3, 57.7 MeV; 238U(64Ni, X)302120*, E*=23.2, 33.5, 45.2, 64.1 MeV; calculated capture, fusion, fission, and evaporation residue formation σ(E), and neutron emission probabilities. Comparison with experimental results for 238U+36S, and with other theoretical calculations for 238U+64Ni.
doi: 10.1103/PhysRevC.101.064616
2019LI27 Phys.Rev. C 99, 054624 (2019) V.L.Litnevsky, F.A.Ivanyuk, G.I.Kosenko, S.Chiba Description of the mass-asymmetric fission of the Pt isotopes, obtained in the reaction 36Ar + 142Nd within the two-stage fusion-fission model NUCLEAR REACTIONS 142Nd(36Ar, X)178Pt*,142Nd(36Ar, xn), E(cm)=122.78, 134.68, 142.58 MeV; calculated potential energy of projectile-target system, partial σ(E), fission fragment mass distribution, mass-energy distribution of fission events, and deformation energy and potential energy surface of 178Pt compound nucleus before neutron evaporation, neutron evaporation probability. Two-stage dynamical stochastic model. Comparison with experimental data. 178Pt; calculated deformation and potential energy surfaces.
doi: 10.1103/PhysRevC.99.054624
2016LI32 Phys.Rev. C 93, 064606 (2016) V.L.Litnevsky, G.I.Kosenko, F.A.Ivanyuk Description of fusion and evaporation residue formation cross sections in reactions leading to the formation of element Z=122 within the Langevin approach NUCLEAR REACTIONS 248Cm(58Fe, xn), 244Pu(64Ni, xn), 208Pb(90Zr, xn), E not given; calculated cross sections of touching, fusion, and evaporation residue formation, dependence of the touching and fusion cross sections on the angular momentum in connection with the synthesis of Z=122 isotopes. Dynamical multidimensional stochastic approach, based on Langevin equations.
doi: 10.1103/PhysRevC.93.064606
2016LI55 Phys.Atomic Nuclei 79, 342 (2016); Yad.Fiz. 79, 236 (2016) V.L.Litnevsky, G.I.Kosenko, F.A.Ivanyuk Allowance for the tunnel effect in the entrance channel of fusion-fission reactions NUCLEAR REACTIONS 238U, 244Pu, 248Cm(48Ca, x), E*=20-50 MeV;248Cm(54Cr, x), E*=20-50 MeV;248Cm(58Fe, x), E*=20-50 MeV;208Pb(90Zr, x), E=20-50 MeV;244Pu(64Ni, x), E*=20-50 MeV;248Cm(58Fe, x), E*=20-50 MeV; calculated grazing σ, capture σ using two-stage model with and without allowance for tunelling effect. Compared with data. 208Pb(48Ca, x), E*=20-50 MeV; calculated capture σ. Compared with data. Deduced possibility for tunelling effect.
doi: 10.1134/S1063778816020113
2014LI06 Phys.Rev. C 89, 034626 (2014) V.L.Litnevsky, V.V.Pashkevich, G.I.Kosenko, F.A.Ivanyuk Description of synthesis of super-heavy elements within the multidimensional stochastic model NUCLEAR REACTIONS 238U(64Ni, xn), E(cm)=250-350 MeV; 244Pu(58Fe, xn), E=230-350 MeV; 248Cm(48Ca, xn), E=180-280 MeV; 248Cm(54Cr, xn), E(cm)=225-350 MeV; calculated capture σ(E), yield of quasi-fission fragments in the fission of Z=116 isotopes produced in 248Cm+48Ca reaction, fission barrier heights of Z=116 and 120 systems, crossing fission barrier σ(E), evaporation residue σ(E) for Z=116 and 120 superheavy elements. Two-stage reaction model for fusion-fission processes. Comparison with experimental data.
doi: 10.1103/PhysRevC.89.034626
2012LI13 Phys.Atomic Nuclei 75, 37 (2012); Yad.Fiz. 75, 39 (2012) V.L.Litnevsky, G.I.Kosenko, F.A.Ivanyuk, V.V.Pashkevich Allowance for the shell structure of the 10042Mo and 11046Pd nuclei in the synthesis of 20084Po, 21088Ra, and 22092U NUCLEAR REACTIONS 100Mo(100Mo, X)200Po, 100Mo(110Pd, X)210Ra, 110Pd(110Pd, X)220U, E(cm) < 300 MeV; calculated potential energy surfaces, σ, touching probabilities. Fusion-fission reactions involving nuclei deformed in the ground state.
doi: 10.1134/S1063778812010115
2012LI17 Phys.Rev. C 85, 034602 (2012) V.L.Litnevsky, V.V.Pashkevich, G.I.Kosenko, F.A.Ivanyuk Influence of the shell structure of colliding nuclei in fusion-fission reactions NUCLEAR REACTIONS 208Pb(16O, X)224Th, 208Pb(18O, X)226Th, E(cm)=70-96 MeV; 208Pb(48Ca, X)256No, E(cm)=170-205 MeV; calculated fusion and evaporation residue cross sections, yield of fission fragments, mass-energy distribution of fission fragments. Two-stage reaction model for fusion-fission process, Langevin equations for the collective coordinates. Comparison with experimental data.
doi: 10.1103/PhysRevC.85.034602
2012LI55 Phys.Atomic Nuclei 75, 1500 (2012); Yad.Fiz. 75, 1579 (2012) V.L.Litnevsky, G.I.Kosenko, F.A.Ivanyuk, V.V.Pashkevich Allowance for the orientation of colliding ions in describing the synthesis of heavy nuclei NUCLEAR REACTIONS 100Mo(100Mo, X)200Po, 208Pb(16O, X)224Th, 100Mo(110Pd, X)210Ra, 110Pd(110Pd, X)220U, E(cm)<95 MeV; analyzed available data; calculated σ. Comparison with available data.
doi: 10.1134/S1063778812110142
2010LI50 Iader.Fiz.Enerh. 11, 341 (2010); Nuc.phys.atom.energ. 11, 341 (2010) V.L.Litnevsky, F.A.Ivanyuk, G.I.Kosenko, V.V.Pashkevich The fusion of heavy ions within the two step reaction model NUCLEAR REACTIONS 100Mo(100Mo, X)200Po, 208Pb(18O, X)226Th, E(cm)<260 MeV; calculated deformation energy, touching probability. Two stage model of fusion-fission reactions is extended by the account of the shell structure of colliding nuclei.
2008KO30 Phys.Atomic Nuclei 71, 2052 (2008); Yad.Fiz. 71, 2086 (2008) G.I.Kosenko, F.A.Ivanyuk, V.V.Pashkevich, D.V.Dinner Application of a two-step dynamical model to calculating properties of fusion-fission reactions NUCLEAR REACTIONS 244Pu(48Ca, X), E=238 MeV; calculated partial touching cross sections.
doi: 10.1134/S1063778808120065
2008NE07 Phys.Atomic Nuclei 71, 1373 (2008); Yad.Fiz. 71, 1401 (2008) Dynamical calculations of the cross section for heavy-ion fusion with allowance for tunneling NUCLEAR REACTIONS 208Pb(16O, X), 208Pb, 244Pu(48Ca, X), E(cm)=65-105 MeV; calculated fusion σ; surface friction model including tunneling; sub-barrier reaction.
doi: 10.1134/S1063778808080061
2006AB33 Phys.Atomic Nuclei 69, 1101 (2006) Y.Abe, G.I.Kosenko, C.W.Shen, B.Bouriquet, A.Marchix, D.Boilley, B.Giraud Fusion Hindrance and Synthesis of Superheavy Elements NUCLEAR REACTIONS 208Pb(58Ni, X), (64Ni, X), (70Zn, X), (71Ga, X), (76Ge, X), E(cm) ≈ 210-310 MeV; 209Bi(70Zn, X), E(cm) ≈ 260-300 MeV; 160Gd(132Sn, X), E(cm) ≈ 325-350 MeV; calculated fusion excitation functions. 208Pb(58Fe, n), (64Ni, n), (70Zn, n), (71Ga, n), (76Ge, n), E(cm) ≈ 215-285 MeV; 209Bi(64Ni, n), (70Zn, n), E(cm) ≈ 235-275 MeV; 160Gd(132Sn, γ), (132Sn, n), (132Sn, 2n), (132Sn, 3n), E(cm) ≈ 325-350 MeV; calculated σ. Fusion hindrance mechanism discussed.
doi: 10.1134/S1063778806070027
2004KU22 Yad.Fiz. 67, 2094 (2004); Phys.Atomic Nuclei 67, 2073 (2004) New Method for Calculating the Potential Energy of Deformed Nuclei within the Liquid-Drop Model
doi: 10.1134/1.1825532
2003AB17 Yad.Fiz. 66, 1093 (2003); Phys.Atomic Nuclei 66, 1057 (2003) Y.Abe, C.W.Shen, G.I.Kosenko, D.Boilley Theory of Fusion for Superheavy Elements NUCLEAR REACTIONS 238U, 244Pu, 248Cm, 252Cf(48Ca, X), E(cm) ≈ 180-240 MeV; calculated fusion σ, maximum evaporation residue σ. Two-step model, comparison with data.
doi: 10.1134/1.1586418
2002KO47 Yad.Fiz. 65, 1629 (2002); Phys.Atomic Nuclei 65, 1588 (2002) G.I.Kosenko, F.A.Ivanyuk, V.V.Pashkevich Multidimensional Langevin Approach to Describing the 18O + 208Pb Fusion-Fission Reaction NUCLEAR REACTIONS 208Pb(18O, X), E(cm) ≈ 70-100 MeV; calculated potential energy features, fusion σ, fission fragment mass distributions, related features. Multi-step approach, Langevin equations.
doi: 10.1134/1.1508690
2002KO71 J.Nucl.Radiochem.Sci. 3, No 1, 19 (2002) A Dynamical Approach to Heavy-ion Fusion: 48Ca + 244Pu NUCLEAR REACTIONS 244Pu(48Ca, X), (48Ca, 2n), (48Ca, 3n), (48Ca, 4n), (48Ca, 5n), E* ≈ 30-70 MeV; calculated fusion, evaporation residue σ.
2002KO72 J.Nucl.Radiochem.Sci. 3, No 1, 71 (2002) G.I.Kosenko, F.A.Ivanyuk, V.V.Pashkevich The Multi-dimensional Langevin Approach to the Description of Fusion-fission Reaction NUCLEAR REACTIONS 208Pb(18O, X), E(cm) ≈ 70-95 MeV; calculated fusion, fission σ, fragment mass distributions, neutron multiplicity. Comparison with data.
2000KU37 Yad.Fiz. 63, No 11, 1978 (2000); Phys.Atomic Nuclei 63, 1885 (2000) R.S.Kurmanov, G.I.Kosenko, G.D.Adeev New Formula for Calculating Coulomb Energies in the Liquid-Drop Model
doi: 10.1134/1.1326978
2000VA27 Yad.Fiz. 63, No 11, 1957 (2000); Phys.Atomic Nuclei 63, 1865 (2000) D.V.Vanin, P.N.Nadtochy, G.I.Kosenko, G.D.Adeev Langevin Description of Mass Distributions of Fragments Originating from the Fission of Excited Nuclei NUCLEAR REACTIONS 232Th(12C, F), E=97 MeV; 249Cf(16O, F), E=145 MeV; calculated fission fragment mass distributions, neutron yields following compound nucleus decay. Liquid drop model.
doi: 10.1134/1.1326976
1999VA06 Phys.Rev. C59, 2114 (1999) D.V.Vanin, G.I.Kosenko, G.D.Adeev Langevin Calculations of Fission Fragment Mass Distribution in Fission of Excited Nuclei NUCLEAR STRUCTURE 105Ag, 117I, 124Ba, 210Po, 244Cm, 249Fm; calculated potential energy surfaces, fission fragment mass distributions, variances vs fissility parameter. Two-dimensional stochastic approach, two liquid drop models compared. NUCLEAR REACTIONS 165Ho(40Ar, F), E=180-280 MeV; calculated fission fragment mass distributions. Two-dimensional stochastic approach, two liquid drop models compared. Comparison with data.
doi: 10.1103/PhysRevC.59.2114
1998BA05 J.Phys.(London) G24, L1 (1998) S.I.Bastrukov, D.V.Podgainy, I.V.Molodtsova, G.I.Kosenko Macroscopic Calculus for the Fission Barrier Height of Superheavy Elements NUCLEAR STRUCTURE 265Hs, 269,271,275,276Ds, 272Rg, 275,277,281,282Cn, 276Nh, 283,287,288Fl, 291,292Lv; calculated elastic deformation energy, fission barrier height. Elastic globe, liquid drop models.
doi: 10.1088/0954-3899/24/1/002
1998KO12 Yad.Fiz. 61, No 3, 416 (1998); Phys.Atomic Nuclei 61, 356 (1998) G.I.Kosenko, D.V.Vanin, G.D.Adeev Multiplicity of Postscission Neutrons Produced in the Fission of Excited Nuclei
1998KO68 Yad.Fiz. 61, No 12, 2142 (1998); Phys.Atomic Nuclei 61, 2031 (1998) G.I.Kosenko, D.V.Vanin, G.D.Adeev Application of the Combined Dynamics-Evaporation Model to the Fission of Excited Nuclei NUCLEAR REACTIONS 232Th, 238U(α, F), E=47-220 MeV; calculated neutron, proton, alpha multiplicities, fission fragments mean kinetic energy; deduced charged particle emission role in fragment deexcitation. Comparisons with data. Combined dynamics-evaporation model.
1997KO14 Yad.Fiz. 60, No 3, 404 (1997); Phys.Atomic Nuclei 60, 334 (1997) G.I.Kosenko, I.G.Cagliari, G.D.Adeev Using the Combined Dynamical Evaporation Approach to Describe Fission Induced by Heavy Ions NUCLEAR REACTIONS 184W(16O, F), E=288 MeV; 181Ta(19F, F), E=124 MeV; 197Au(18O, F), E=159 MeV; calculated fission fragment mean kinetic energy, variance prescission n-, α-, p-multiplicities, postscission n-multiplicities. Combined dynamical evaporation approach.
1993KO06 Yad.Fiz. 56, No 2, 77 (1993); Phys.Atomic Nuclei 56, 189 (1993) Choice of Inital Conditions in Dynamical Calculations of Distributions of Nuclear Fission Fragments NUCLEAR STRUCTURE 248Cf, 235U; calculated fission barrier characteristics, fragment momentum distribution at barrier; deduced best fit for Kramer distribution. Langevin fluctuation-dissipation dynamics.
1992GO08 Yad.Fiz. 55, 920 (1992); Sov.J.Nucl.Phys. 55, 514 (1992) I.I.Gonchar, G.I.Kosenko, N.I.Pischasov, O.I.Serdyuk Calculation of the Moments of the Fission-Fragment Energy Distribution by the Method of Langevin Equations NUCLEAR STRUCTURE Z=54-104; calculated fission fragment energy distribution, moments. Langevin equations, fluctuation dissipation dynamics.
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