NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.P.Soznik Found 42 matches. 2012KU21 Phys.Atomic Nuclei 75, 832 (2012); Yad.Fiz. 75, 887 (2012) V.I.Kuprikov, V.V.Pilipenko, A.P.Soznik Description of deuteron-nucleus scattering in terms of a microscopic optical potential based on Skyrme forces NUCLEAR REACTIONS 24Mg, 48,50Ti, 52Cr, 54,56Fe, 58,60Ni, 64Zn, 90,92,96Zr, 100Mo, 118,120Sn, 208Pb(d, d), E=17, 56 MeV; calculated σ(θ), σ. Skyrme forces, comparison with available data.
doi: 10.1134/S1063778812040084
2010PI03 Phys.Rev. C 81, 044614 (2010) V.V.Pilipenko, V.I.Kuprikov, A.P.Soznik Skyrme interaction and elastic nucleon-nucleus scattering in the optical model NUCLEAR REACTIONS 116Sn(n, n), E=13.9 MeV; 56Fe(n, n), E=0.1, 0.8, 5, 34, 1800 keV; 80Se(n, n), E=1, 8, 50, 300, 1500 keV; 76Se(n, n), E=1, 8 MeV; 82Se(n, n), E=0.01, 0.08, 0.6 keV; 92,98Mo(n, n), E=0.11, 0.9, 7 MeV; 96,100Mo(n, n), E=1.1, 9, 70 eV; 106Pd(n, n), E=0.08, 0.71, 5.9 MeV; 114Cd(n, n), E=1, 8.4, 71 eV; 40Ca(n, n), E=10 MeV; 54Fe(n, n), E=14, 100 keV; 58Ni(n, n), E=14, 100 eV; 116Sn(n, n), E=0.01 eV; 120Sn(n, n), E=1.4, 10 MeV; 208Pb(n, n), E=0.00014, 0.01, 0.09, 40, 70 eV; 208Pb(n, n), E=0.00303, 0.20, 14.6 MeV; analyzed σ(θ, E). 40Ca(polarized n, n), E=10 MeV; 54Fe(polarized n, n), E=14 MeV; 58Ni, 116,120Sn(polarized n, n), E=10, 14 MeV; 208Pb(polarized n, n), E=7, 8, 9, 10, 14 MeV; analyzed vector analyzing powers. Microscopic optical potential (MOP) model and Hartree-Fock method with different Skyrme interactions by perturbation theory. NUCLEAR STRUCTURE 40Ca, 54,56Fe, 58Ni, 76,82Se, 92,100Mo, 106Pd, 114Cd, 116,120Sn, 208Pb; calculated binding energies and charge radii using self-consistent Hartree-Fock theory with SkOP1 and SkOP2 interactions.
doi: 10.1103/PhysRevC.81.044614
2010PI12 Iader.Fiz.Enerh. 11, 367 (2010); Nuc.phys.atom.energ. 11, 367 (2010) V.V.Pilipenko, V.I.Kuprikov, A.P.Soznik Optical potential based on Skyrme forces for describing the elastic nucleon-nucleus scattering NUCLEAR REACTIONS 116Sn(n, n), E=13.9 MeV; 54Fe, 58Ni, 120Sn, 208Pb(n, n), E=14 MeV; 48Ca, 56Fe, 58Ni, 82Se, 90Zr, 116Sn, 124Sn(p, p), E=16 MeV; calculated σ(θ), σ. Calculations of the one-particle Green function mass operator using the effective Skyrme nucleon-nucleon forces.
2009KU08 Phys.Atomic Nuclei 72, 975 (2009); Yad.Fiz. 72, 1019 (2009) V.I.Kuprikov, V.V.Pilipenko, A.P.Soznik, V.N.Tarasov, N.A.Shlyakhov Description of nuclear structure and cross sections for nucleon-nucleus scattering on the basis of effective Skyrme forces
doi: 10.1134/S1063778809060106
2006KU05 Phys.Atomic Nuclei 69, 6 (2006); Yad.Fiz. 69, 8 (2006) V.I.Kuprikov, V.V.Pilipenko, A.P.Soznik Analysis of Nucleon-Nucleus Scattering in Terms of a Microscopic Optical Potential Based on Effective Skyrme Forces NUCLEAR REACTIONS 90Zr(n, X), E ≈ 0-80 MeV; 40Ca(p, X), E ≈ 10-50 MeV; calculated total reaction σ. 40Ca(n, n), E=11, 13.9 MeV; 56Fe(n, n), E=20 MeV; 208Pb(n, n), E=11 MeV; calculated elastic σ(θ). Microscopic nucleon-nucleus optical potential, effective Skyrme forces, comparison with data.
doi: 10.1134/S1063778806010029
2005KU07 Yad.Fiz. 68, 233 (2005); Phys.Atomic Nuclei 68, 208 (2005) V.I.Kuprikov, V.V.Pilipenko, A.P.Soznik Nucleon-Nucleus Optical Potential at Finite Temperatures within a Semimicroscopic Approach for the Case of Skyrme Forces NUCLEAR REACTIONS 40Ca, 208Pb(n, X), E=0-50 MeV; calculated optical potential parameters at finite temperature, rearrangement potential contribution. Semimicroscopic approach, Skyrme forces.
doi: 10.1134/1.1866376
1999KR12 Int.J.Mod.Phys. E8, 137 (1999) Potential of Nucleon Interaction with Odd Nuclei in the Hartree-Fock Theory NUCLEAR REACTIONS 13C(p, p), (n, n), E not given; calculated optical potential for nucleus-nucleon scattering. Hartree-Fock theory.
doi: 10.1142/S0218301399000112
1998KR06 Yad.Fiz. 61, No 3, 461 (1998); Phys.Atomic Nuclei 61, 400 (1998) S.M.Kravchenko, V.I.Kuprikov, A.P.Soznik Semimicroscopic Calculation of the Imaginary Part of the Nucleon-Nucleus Optical Potential NUCLEAR REACTIONS 40Ca(n, n), E=0-50 MeV; calculated imaginary part of optical potential; deduced rearrangement potential role. Skyrme forces.
1998KR18 Int.J.Mod.Phys. E7, 465 (1998) S.M.Kravchenko, V.I.Kuprikov, A.P.Soznik Semimicroscopic Optical Potential with Effective Density-Dependent Nucleon-Nucleon Interaction NUCLEAR REACTIONS 40Ca(n, n), E < 50 MeV; calculated optical potential, phase shifts; deduced parameters. Rearrangement potential, density-dependent forces.
doi: 10.1142/S0218301398000245
1998KR25 Yad.Fiz. 61, No 12, 2147 (1998); Phys.Atomic Nuclei 61, 2036 (1998) Optical Potential for the 13C Nucleus in the Hartree-Fock Approximation Implemented with Skyrme Forces NUCLEAR REACTIONS 13C(p, p), (n, n), E=10, 30, 50 MeV; calculated optical potentials; deduced spin-orbit, spin-spin, tensor contributions. Hartree-Fock method, Skyrme forces.
1998KR30 Bull.Rus.Acad.Sci.Phys. 62, 1834 (1998) S.M.Kravchenko, V.I.Kuprikov, A.P.Soznik Imaginary Part of the Optical Potential with the Generalized Effective Skyrme Interaction NUCLEAR STRUCTURE 40Ca; calculated optical potential for elastic nucleon scattering. Generalized effective Skyrme interaction.
1996AK01 Int.J.Mod.Phys. E5, 107 (1996) A.I.Akhiezer, A.P.Soznik, Yu.A.Berezhnoy Inclusive Tritium Stripping Reaction Theory NUCLEAR REACTIONS 208Pb(t, X), E=795, 975 MeV; calculated nucleon energy, σ(θ), σ, following stripping, two-nucleon transfer.
doi: 10.1142/S0218301396000049
1996AK07 Bull.Rus.Acad.Sci.Phys. 60, 821 (1996) A.I.Akhiezer, Yu.A.Berezhnoi, V.A.Slipko, A.P.Soznik One-Nucleon Transfer Reactions Involving 3H and 3He Nuclei in the Intermediate Energy Range NUCLEAR REACTIONS 208Pb(t, d), E=975 MeV; calculated σ(θ), angle-integrated σ. Diffraction theory.
1996KR18 Bull.Rus.Acad.Sci.Phys. 60, 764 (1996) Optical Potential of Odd Nucleus in the Hartree-FOck Approximation with Generalized Skyrme Forces
1995AK05 Bull.Rus.Acad.Sci.Phys. 59, 523 (1995) A.I.Akhiezer, Yu.A.Berezhnoi, A.P.Soznik Two-Nucleon Transfer Reaction Involving 3H and 3He Nuclei in the Intermediate Energy Range NUCLEAR REACTIONS 208Pb(t, nX), E=975 MeV; calculated σ(θ), En. Inclusive stripping reaction.
1993BE10 Z.Phys. A344, 431 (1993) Yu.A.Berezhnoy, I.N.Kudryavtsev, A.P.Soznik Absorption and Refraction Phenomena in Proton- and Antiproton-Nucleus Scattering NUCLEAR REACTIONS 12C(p-bar, p-bar), E=46.8, 179.7 MeV; 16O(p-bar, p-bar), E=178.4 MeV; 40Ca(p-bar, p-bar), E=47.8, 179.8 MeV; 208Pb(p-bar, p-bar), E=46.8, 180.3 MeV; calculated σ(θ). 12C(p, p), E=185 MeV; 40Ca(p, p), E=181 MeV; 208Pb(p, p), E=182.4 MeV; calculated σ(θ), polarization vs θ. Phenomenological diffraction theory.
1993KU04 Yad.Fiz. 56, No 1, 84 (1993); Phys.Atomic Nuclei 56, 49 (1993) Optical Potential with an Effective Density-Dependent Nucleon-Nucleon Interaction NUCLEAR REACTIONS 40Ca(n, n), E ≈ 0; calculated potential parameter radial dependence. Effective density-dependent nucleon-nucleon interaction. Mass operator, rearrangement potential, two-particle density-dependent effective Skyrme interaction.
1989KU07 Yad.Fiz. 49, 229 (1989) Elastic Scattering of Intermediate-Energy Protons by Spin-1/2 Oriented Nuclei NUCLEAR REACTIONS 13C(polarized p, p), E=547-1000 MeV; calculated σ(θ), polarization observables vs θ. Multiple diffraction scattering theory.
1989KU14 J.Phys.(London) G15, 1377 (1989) Elastic Intermediate-Energy Proton Scattering by Polarized Nuclei NUCLEAR REACTIONS 13N, 13C(p, p), E=550, 800 MeV; calculated σ(θ), polarization observables vs θ. Polarized target.
doi: 10.1088/0954-3899/15/9/008
1989KU17 Yad.Fiz. 49, 1572 (1989) V.I.Kuprikov, A.P.Soznik, V.N.Tarasov Hartree-Fock Calculation of Properties of Long Chains of Ba, Nd, Sm, and Gd Isotopes NUCLEAR STRUCTURE 128,130,132,134,136,138,140,142,144,146,148Ba, 132,134,136,138,140,142,144,146,148,150,152Nd, 134,136,138,140,142,144,146,148,150,152,154Sm, 136,138,140,142,144,146,148,150,152,154,156Gd; calculated binding energy, rms charge radii variations, quadrupole, hexadecapole moments, B(λ). Hartree-Fock method, Skyrme type forces.
1989KU32 Ukr.Fiz.Zh. 34, 1642 (1989) Analysis of Complete Experiment in Elastic Intermediate Energy Proton Scattering by Spin 1/2 Nuclei NUCLEAR REACTIONS 13C(polarized p, p), E=0.8, 1 GeV; calculated σ(θ), analyzing power vs θ. Diffraction model.
1988BE11 Yad.Fiz. 47, 379 (1988) Elastic Nuclear Scattering of 700-MeV Polarized Deuterons NUCLEAR REACTIONS 40Ca, 58Ni(polarized d, d), E=700 MeV; analyzed σ(θ), analyzing power vs θ. S-matrix.
1988BE48 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 915 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.5, 78 (1988) Interactions of 700 MeV Polarized Deuterons with 40Ca and 58Ni NUCLEAR REACTIONS 40Ca, 58Ni(polarized d, d), E=700 MeV; analyzed σ(θ), analyzing power data. Phenomenological model.
1988BE58 Ukr.Fiz.Zh. 33, 993 (1988) Polarization Phenomena in Elastic d4He Scattering at Intermediate Energies NUCLEAR REACTIONS 4He(polarized d, d), E=2 GeV; calculated σ(θ), vector, tensor analyzing power vs θ.
1988BE60 Ukr.Fiz.Zh. 33, 1293 (1988) Inelastic Scattering of Polarized Deuterons of Medium Energy by Atomic Nuclei NUCLEAR REACTIONS 58Ni(polarized d, d'), E=700 MeV; 208Pb(polarized d, d'), E=86 MeV; calculated partial σ(θ), vector, tensor analyzing power vs θ. Optical diffraction model.
1988KU32 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2267 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 189 (1988) Transition Densities of Isoscalar Giant Monopole Resonances within the Framework of Adiabatic Time-Dependent Hartree-Fock Theory NUCLEAR STRUCTURE 16O, 40Ca, 58Ni, 90Zr, 120Sn, 208Pb; calculated isoscalar giant monopole resonance transition densities. Adiabatic TDHF.
1987BE12 Ukr.Fiz.Zh. 32, 5 (1987) Concerning the Theory of Polarization Phenomena in Elastic Nuclear Scattering of High-Energy Deuterons NUCLEAR REACTIONS 124Sn(d, d), (polarized d, d), E=1, 2 GeV; 12C(d, d), (polarized d, d), E=420 MeV; calculated σ(θ), vector, tensor polarizations. Multiple diffration scattering theory.
1987BE18 Ukr.Fiz.Zh. 32, 342 (1987) Polarization of Medium Energy Deuteron-Nucleus Elastic Scattering NUCLEAR REACTIONS 58Ni(polarized d, d), E=79 MeV; calculated σ(θ), vector, tensor polarization vs θ. Diffraction model.
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.
1987KU19 Ukr.Fiz.Zh. 32, 994 (1987) Excitation of Isoscalar Monopole Giant Resonances by Intermediate-Energy Protons NUCLEAR REACTIONS 40Ca(p, p), (p, p'), (polarized p, p'), E=0.497, 1 GeV; analyzed σ(θ), polarization data. 40Ca deduced giant resonance excitation.
1987KU21 Ukr.Fiz.Zh. 32, 1297 (1987) V.I.Kuprikov, A.P.Soznik, A.A.Khomich, N.G.Shevchenko Change of the Skin Thickness in Distribution of Nuclear Charge Density in Selenium Isotopes NUCLEAR REACTIONS 76,78,80,82Se(e, e), E=225, 300 MeV; analyzed σ(θ); deduced nuclear charge distribution skin thickness parameter. Hartree-Fock calculations.
1986PI08 Yad.Fiz. 44, 369 (1986) On Polarization Characteristics of Elastic and Inelastic Proton-Nuclear Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=497, 800, 1000 MeV; calculated σ(θ), polarization, analyzing power vs θ; deduced nucleon-nucleon amplitude parameters.
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.
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.
1982BE23 Ukr.Fiz.Zh. 27, 484 (1982) Yu.A.Berezhnoi, A.P.Soznik, G.A.Khomenko Proton Polarization in Inelastic Nuclear Scattering NUCLEAR REACTIONS 116,124Sn(polarized p, p), (polarized p, p'), E=0.8 GeV; 12C(polarized p, p), (polarized p, p'), E=1 GeV; calculated σ(θ), proton polarization P(θ), asymmetry vs θ. Multipole diffraction scattering theory.
1979BE11 Yad.Fiz. 29, 350 (1979); Sov.J.Nucl.Phys. 29, 174 (1979) Effect of the Internal Structure of Three-Nucleon Particles on Nuclear Scattering at Intermediate Energies NUCLEAR REACTIONS 89Y, 90Zr, 120Sn, 208Pb(3He, 3He), E=217 MeV; calculated σ(θ). Included internal structure of mass-3 nuclei.
1979BE68 Yad.Fiz. 30, 1523 (1979); Sov.J.Nucl.Phys. 30, 789 (1979) Yu.A.Berezhnoi, V.I.Kudryashov, A.P.Soznik, N.A.Shlyakhov Asymmetry in Elastic and Inelastic Diffractive Scattering of Polarized Protons NUCLEAR REACTIONS 58Ni(polarized p, p), (polarized p, p'), E=40 MeV; analyzed σ(θ), analyzing power A(θ). Diffraction model.
1978BE50 Nucl.Phys. A308, 330 (1978) Intermediate Energy Deuteron-Nucleus Diffraction Interaction NUCLEAR REACTIONS 208Pb, 68Zn(d, d), E=80 MeV; Cu(d, X), E=26 MeV; Pb, Cu, Al(d, X), E=650 MeV; calculated σ, deuteron stripping σ.
doi: 10.1016/0375-9474(78)90555-9
1974BE22 Yad.Fiz. 19, 813 (1974); Sov.J.Nucl.Phys. 19, 414 (1974) Contribution to Inelastic High-Energy Diffraction Scattering NUCLEAR REACTIONS 12C, 16O(p, p), (p, p'), E=1 GeV; calculated σ(θ), σ(Ep', θ).
1973VY04 Izv.Akad.Nauk SSSR, Ser.Fiz. 37, 1742 (1973); Bull.Acad.Sci.USSR, Phys.Ser. 37, No.8, 155 (1974) G.L.Vysotskii, A.P.Soznik, M.A.Chegoryan Polarization Effects in Elastic Scattering of Intermediate Energy Deuterons NUCLEAR REACTIONS 58Ni(d, d), (polarized d, d), E=22 MeV; calculated σ(θ), iT(θ).
1972BE87 Ukr.Fiz.Zh. 17, 1828 (1972) On a Bound State for Systems of Three and Four α-Particles NUCLEAR STRUCTURE 12C, 16O; calculated 3-, 4-α particle systems.
Back to query form |