NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = A.S.Molev Found 37 matches. 2022BE04 Acta Phys.Pol. B53, 2-A1 (2022) S-matrix Description of Refractive Effects in One-nucleon Stripping Reactions Induced by α-particles on 28Si NUCLEAR REACTIONS 28Si(α, 3He), (α, t), E=50-120 MeV; analyzed available data; deduced σ, σ(θ), S-matrix parameters, Airy minima.
doi: 10.5506/APhysPolB.53.2-A1
2018BE26 Int.J.Mod.Phys. E27, 1850061 (2018) Yu.A.Berezhnoy, A.S.Molev, G.M.Onyshchenko, V.V.Pilipenko Unified S-matrix analysis of Airy structures in α + 24Mg elastic and inelastic scattering NUCLEAR REACTIONS 24Mg(α, α), (α, α'), E=50-224 MeV; calculated σ(θ) using the six-parameter S-matrix model. Comparison with available data.
doi: 10.1142/S0218301318500611
2018BE27 Int.J.Mod.Phys. E27, 1850066 (2018) Strong absorption model with antisymmetric S-matrix NUCLEAR REACTIONS 12C, 16O, 28Si(p, p), (n, n), E<135 MeV; analyzed available data; deduced σ, phase shifts, S-matrix parameters.
doi: 10.1142/S0218301318500660
2018KO09 Phys.Rev. C 97, 034606 (2018) V.Yu.Korda, A.S.Molev, L.P.Korda, V.F.Klepikov Systematic model-independent S-matrix analysis of 4He - 40Ca elastic scattering in going from anomalous large-angle scattering to near-Coulomb-barrier scattering NUCLEAR REACTIONS 40Ca(α, α), E=4.5-27 MeV; calculated σ/σR(θ), S-matrix modulii, nuclear phases, deflection functions, and real part of nuclear phase; deduced smooth and monotonic functions of angular momentum, simultaneous description of a variety of scattering processes such as nuclear rainbow, pre-rainbow, anomalous large-angle scattering (ALAS), and near-Coulomb-barrier scattering (NCBS), with no evidence for Airy minima higher than the second order. Evolutionary model-independent S-matrix approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.97.034606
2015KO02 Phys.Rev. C 91, 024619 (2015) V.Yu.Korda, A.S.Molev, V.F.Klepikov, L.P.Korda Unified model-independent S-matrix description of nuclear rainbow, prerainbow, and anomalous large-angle scattering in 4He - 40Ca elastic scattering NUCLEAR REACTIONS 40Ca(α, α), E=29.05-82.0 MeV; calculated σ(θ, E), angular positions of the Airy minima of first and second orders; deduced simultaneous description of nuclear rainbow, prerainbow, and anomalous large-angle scattering (ALAS). Model-independent S-matrix approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.024619
2009KO05 Phys.Rev. C 79, 024601 (2009) V.Yu.Korda, A.S.Molev, L.P.Korda, V.F.Klepikov Model-independent analysis of Airy structures in the 16O+12C and 16O+16O elastic scattering differential cross sections at 13-22 MeV/nucleon NUCLEAR REACTIONS 12C(16O, 16O), E=200, 300 MeV; 16O(16O, 16O), E=250, 350 MeV; calculated cross sections, scattering matrix moduli, nuclear phases, reduced imaginary scattering phases using model-independent S-matrix approach. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.024601
2009KO26 Phys.Atomic Nuclei 72, 1754 (2009); Yad.Fiz. 72, 1812 (2009) V.Yu.Korda, A.S.Molev, L.P.Korda Analysis of refractive effects in 4He + 15N, 18O, 24Mg, 44Ca, and 90Zr scattering processes at energies in the range E(4He) = 13-15 MeV per nucleon by using smooth monotonic dependences of the nuclear phase shift on the orbital angular momentum NUCLEAR REACTIONS 15N, 18O, 24Mg, 44Ca, 90Zr(α, α), E=13-15 MeV/nucleon; analyzed σ(θ) on the basis of S-matrix approach using evolution algorithm; deduced quantitive description of experimental data with smooth monotonic functions of the orbital angular momentum.
doi: 10.1134/
2008KO16 Phys.Atomic Nuclei 71, 1287 (2008); Yad.Fiz. 71, 1314 (2008) V.Yu.Korda, A.S.Molev, L.P.Korda Model-independent analysis of Airy structures in the differential cross sections for the elastic scattering of 4He and 16O nuclei within a single S-matrix systematics NUCLEAR REACTIONS 90Zr(α, α), E=59.1, 118.0 MeV; 12C(16O, 16O), E=200.0, 300.0 MeV; 16O(16O, 16O), E=350.0 MeV; analyzed σ(dθ): S-matrix; Airy structures.
doi: 10.1134/S1063778808070235
2007KO44 Phys.Atomic Nuclei 70, 1047 (2007); Yad.Fiz. 70, 1082 (2007) V.Yu.Korda, A.S.Molev, L.P.Korda Elastic 16O16O scattering at E(16O) = 350 MeV and new method for a model-independent determination of the scattering matrix NUCLEAR REACTIONS 16O(16O, 16O), e=350 MeV; calculated elastic scattering cross sections using S-matrix formalism. Compared results to available data.
doi: 10.1134/S1063778807060075
2007KO81 Iader.Fiz.Enerh. 8 no.4, 81 (2007); Nuc.phys.atom.energ. 8, no.4, 81 (2007) V.Yu.Korda, A.S.Molev, L.P.Korda Model-independent description of the light nucleus-nucleus elastic scattering at intermediate energies NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; calculated scattering matrices. Model-free approach, evolution algorithm.
doi: 10.15407/jnpae
2005KO24 Phys.Rev. C 72, 014611 (2005) V.Yu.Korda, A.S.Molev, L.P.Korda Evolving model-free scattering matrix via evolutionary algorithm: 16O - 16O elastic scattering at 350 MeV NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; calculated scattering matrix, σ(θ). Evolutionary algorithm, comparison with data.
doi: 10.1103/PhysRevC.72.014611
2005KO48 Bull.Rus.Acad.Sci.Phys. 69, 64 (2005) V.Yu.Korda, A.S.Molev, L.P.Korda Model-free study of refracting and absorbing properties of 16O - 16O interaction at energy 22-44 MeV/nucleon by evolution algorithm NUCLEAR REACTIONS 16O(16O, 16O), E=350, 480, 704 MeV; analyzed σ(θ); deduced parameters. Model-free approach, evolution algorithm.
2005KO52 Bull.Rus.Acad.Sci.Phys. 69, 1778 (2005) V.Yu.Korda, A.S.Molev, L.P.Korda Model-free study of scattering matrix for 16O + 12C at energies E(16O)=200-281 MeV NUCLEAR REACTIONS 12C(16O, 16O), E=200-281 MeV; calculated σ(θ). Comparison with data.
2004BE42 Yad.Fiz. 67, 1480 (2004); Phys.Atomic Nuclei 67, 1454 (2004) Interference between Diffractive, Refractive, and Coulomb Effects in the Cross Sections for the Elastic Scattering of Light Nuclei by Nuclei at Intermediate Energies NUCLEAR REACTIONS 26Mg(3He, 3He), E=33.67 MeV; 198Au(9Be, 9Be), E=158 MeV; 12C(3He, 3He), E=82.1 MeV; 12C(13C, 13C), E=260 MeV; calculated σ(θ); deduced interference contributions. S-matrix approach, comparison with data.
doi: 10.1134/1.1788036
2004MO52 Bull.Rus.Acad.Sci.Phys. 68, 229 (2004) A.S.Molev, V.Yu.Korda, L.P.Korda Analysis of refractive effects in 16O-16O scattering using S-matrix approach and genetic algorithm NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; analyzed σ(θ). S-matrix approach, genetic algorithm.
2003BE70 Int.J.Mod.Phys. E12, 827 (2003) Interference of diffractive, refractive and Coulomb effects in light nucleus-nucleus elastic scattering cross-sections at intermediate energies NUCLEAR REACTIONS 26Mg(3He, 3He), E=33.67 MeV; 198Au(9Be, 9Be), E=158.30 MeV; 12C(3He, 3He), E=82.1 MeV; 12C(13C, 13C), E=260.0 MeV; calculated σ(θ), interference contributions. S-matrix approach, comparison with data.
doi: 10.1142/S0218301303001557
2001KU20 Bull.Rus.Acad.Sci.Phys. 65, 31 (2001) A.V.Kuznichenko, A.S.Molev, G.M.Onishchenko Relation of Refraction and Absorption Effects in 3He - 12C Scattering at an Energy of About 20 MeV/Nucleon NUCLEAR REACTIONS 12C(3He, 3He), E=17-20 MeV/nucleon; analyzed σ(θ); deduced S-matrix parameters.
2000MO34 Bull.Rus.Acad.Sci.Phys. 64, 773 (2000) Phase Rule for Refractive Components of Cross Sections for Elastic and Inelastic Scattering of Light Nuclei NUCLEAR REACTIONS 12C(3He, 3He), (3He, 3He'), E=82.1 MeV; 12C(11Li, 11Li), (11Li, 11Li'), E=637 MeV; 40Ca(α, α), (α, α'), E=104 MeV; calculated refractive and farside σ(θ). S-matrix method.
1999MO37 Bull.Rus.Acad.Sci.Phys. 63, 809 (1999) Potentials of Interaction of Exotic 11Li and 14Be Nuclei with Nuclei NUCLEAR REACTIONS 12C(11Li, X), E=637 MeV; 28Si(11Li, X), E=319 MeV; 12C(14Be, X), E=796 MeV; calculated real and imaginary parts of the nuclear potential, reaction σ. Comparison with other calculations and data.
1998MO27 Bull.Rus.Acad.Sci.Phys. 62, 141 (1998) A.S.Molev, A.V.Kuznichenko, G.M.Onishchenko Sensitivity of Cross Sections for 11Li + 12C, 28Si Scattering to Properties at Short Distances NUCLEAR REACTIONS 12C(11Li, 11Li'), E=637 MeV; 28Si(11Li, 11Li'), E=319 MeV; analyzed σ(θ); deduced sensitivity to S-matrix behaviour.
1997MO24 Bull.Rus.Acad.Sci.Phys. 61, 131 (1997) A.S.Molev, A.V.Kuznichenko, G.M.Onishchenko Inelastic Contribution to Quasielastic 11Li-28Si Scattering at E(11Li) = 319 MeV NUCLEAR REACTIONS 28Si(11Li, 11Li), (11Li, X), E=29 MeV/nucleon; analyzed σ(θ); deduced model parameters; deduced inelastic process contribution to quasielastic scattering.
1997MO42 Bull.Rus.Acad.Sci.Phys. 61, 1691 (1997) Nuclear Refraction Effect on Quasielastic Scattering of Neutron-Rich Nuclei with Energy 60 MeV/nucleon NUCLEAR REACTIONS 12C(11Li, 11Li), (11C, 11C), (14Be, 14Be), E ≈ 60 MeV/nucleon; calculated σ(θ); deduced refractive contributions. Comparison with data.
1996MO21 Bull.Rus.Acad.Sci.Phys. 60, 106 (1996) A.S.Molev, A.V.Kuznichenko, G.M.Onishchenko Interference between Nearside and Farside Components in Quasielastic 14Be-12C Scattering at Energy 57 MeV/Nucleon NUCLEAR REACTIONS 12C(14Be, 14Be), (14Be, 14Be'), E=57 MeV/nucleon; analyzed σ(θ); deduced nearside, farside components interference characteristics, quasielastic scattering. Six parameter model representation of S-matrix.
1995MO28 Bull.Rus.Acad.Sci.Phys. 59, 86 (1995) Separation of Refractive and Diffractive Contributions to Cross Sections for Inelastic Scattering of Light Ions with E ≥ 20 MeV/nucleon NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, 6Li'), E=210 MeV; 40Ca(α, α), (α, α'), E=100 MeV; analyzed σ(θ); deduced reaction mechanisms, refractive, diffractive contributions separation.
1994MO43 Bull.Rus.Acad.Sci.Phys. 58, 1822 (1994) A.S.Molev, A.V.Kuznichenko, G.M.Onishchenko, V.V.Adodin, N.T.Burtebaev, A.D.Duisebaev Rainbowlike Phenomena in (3He, α) Reaction of 24Mg, 28,30Si Nuclei at an Energy of 60 MeV NUCLEAR REACTIONS 28,29,30Si, 24Mg(3He, α), E=60 MeV; analyzed σ(θ) data; deduced distant component role, model parameters. Model representation of scattering matrix.
1993KU28 Bull.Rus.Acad.Sci.Phys. 57, 1800 (1993) A.V.Kuznichenko, A.S.Molev, G.M.Onyshchenko Inelastic Scattering of 3,4He Ions by Deformed Nuclei with A = 24-32 at Energies 60-120 MeV NUCLEAR REACTIONS 24,26Mg(α, α), (α, α'), E=81-119 MeV; 24Mg, 28,30Si, 32S(3He, 3He), (3He, 3He'), E=60 MeV; analyzed σ(θ); deduced nucleus-nucleus interaction probing possibility.
1991KU29 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 2249 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.11, 165 (1991) A.V.Kuznichenko, A.S.Molev, G.M.Onishchenko, V.V.Pilipenko Inelastic Rainbow Scattering of 3He Ions at 12C Nuclei at an Energy of 24-33 MeV per Nucleon NUCLEAR REACTIONS 12C(3He, 3He'), E=72-98 MeV; analyzed σ(θ); deduced rainbow scattering features, model parameters. 12C levels deduced deformation parameters. S-matrix approach.
1990KU23 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 848 (1990); Bull.Acad.Sci.Ussr, Phys.Ser. 54, No.5, 31 (1990) A.V.Kuznichenko, A.S.Molev, G.M.Onishchenko Total Cross Sections for Reactions with the Participation of Light Nuclei and the Ericson Parametrization of the Scattering Matrix NUCLEAR REACTIONS, ICPND 24Mg(α, α), E=33.4 MeV; 27Al(3He, 3He), E=29.6 MeV; 58Ni(3He, 3He), E=33.7, 51.3 MeV; 28Si(6Li, 6Li), E=22.8 MeV; 28Si(16O, 16O), E=55 MeV; 40Ca(16O, 16O), E=1.503 GeV; calculated reaction σ. Scattering matrix approach, Ericson parametrization.
1990KU25 Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 2142 (1990); Bull.Acad.Sci.USSR, Phys.Ser. 54, No.11, 57 (1990) A.V.Kuznichenko, A.S.Molev, G.M.Onishchenko, V.V.Pilipenko The Nuclear Rainbow Effect in the Elastic Scattering of 3He by 12C at E(3He) = 72-98 MeV NUCLEAR REACTIONS 12C(3He, 3He), E=72-98 MeV; analyzed σ(θ). S-matrix approach.
1989KU22 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 147 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.1, 142 (1989) A.V.Kuznichenko, A.S.Molev, G.M.Onishchenko Elastic Scattering of 4He Nuclei by 12C Nuclei in the 120-173 MeV Range NUCLEAR REACTIONS 12C(α, α), E=120-173 MeV; calculated σ(θ); deduced model parameters.
1989KU30 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 2211 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.11, 158 (1989) A.V.Kuznichenko, A.S.Molev, G.M.Onishchenko Total Cross Sections of the Reaction between α Particles and 12C Nuclei in the Energy Range 96.6-172.5 MeV NUCLEAR REACTIONS, ICPND 12C(α, α), E ≈ 100-175 MeV; calculated σ, reaction σ. Different models.
1987BE40 Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 933 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.5, 95 (1987) Yu.A.Berezhnoi, A.S.Molev, A.P.Soznik Spin Reversal Function of 800 MeV Protons on Nucleus with One- and Two-Photon Excitation of Nuclear States NUCLEAR REACTIONS 92Zr(p, p'), (polarized p, p'), E=800 MeV; calculated σ(θ), spin reversal function vs θ. Multiple diffraction scattering theory.
1986BE48 Ukr.Fiz.Zh. 31, 1310 (1986) Interaction Potentials between Medium Energy Particles and Nuclei NUCLEAR REACTIONS 208Pb, 90Zr(p, X), E=156, 185 MeV; 9Be(3He, X), E=217 MeV; calculated central, spin-orbit, isospin potentials; deduced nuclear parameters vs radius. Diffraction model.
1985BE19 Ukr.Fiz.Zh. 30, 13 (1985) Yu.A.Berezhnoi, A.S.Molev, A.P.Soznik, G.A.Khomenko Spin-Orbit Part of the Scattering Matrix in the Intermediate Energy Region NUCLEAR REACTIONS 12C, 90Zr, 124Sn, 208Pb(p, p), E=1 GeV; calculated amplitudes; deduced S-matrix spin-orbit component.
1985BE28 Ukr.Fiz.Zh. 30, 814 (1985) Coulomb Effects and Polarization Phenomena in Elastic Nuclear Scattering of Medium Energy Protons NUCLEAR REACTIONS 90Zr, 208Pb(p, p), (polarized p, p), E=40, 185 MeV; calculated σ(θ), analyzing power vs θ, spin rotation function. Coulomb field, proton magnetic moment coupling.
1985BE29 Yad.Fiz. 41, 1420 (1985) Yu.A.Berezhnoi, A.S.Molev, V.V.Pilipenko, A.P.Soznik Spin Rotation Functions of 500 MeV Protons Scattered by 40Ca Nuclei NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=500 MeV; analyzed polarization characteristics, spin-rotation function data, σ(θ); deduced nucleon-nucleon amplitude spin-orbit term role. Multiple diffraction scattering theory.
1984BE04 Yad.Fiz. 39, 24 (1984) Yu.A.Berezhnoy, A.S.Molev, A.P.Soznik Polarization Phenomena in Inelastic Nuclear Scattering of Moderate-Energy Protons NUCLEAR REACTIONS 58Ni(polarized p, p), (polarized p, p'), E=40 MeV; 208Pb(polarized p, p), (polarized p, p'), E=185 MeV; analyzed σ(θ), polarization parameters vs θ. Diffraction model.
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