NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = V.V.Pilipenko Found 58 matches. 2022BE34 East.Eur.J.Phys 2022, 48 (2022) Y.A.Berezhnoy, G.M.Onyshchenko, P.E.Kuznietsov, V.V.Pilipenko, I.I.Yakymenko Analysis of α-208Pb Elastic Scattering at a Wide Energies by the S-Matrix Model NUCLEAR REACTIONS 208Pb(α, α), E=104-699 MeV; analyzed available data; deduced energy evolution of the S-matrix parameters, the total reaction σ, nuclear rainbow and Fraunhofer crossover angles.
doi: 10.26565/2312-4334-2022-4-03
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
2018PI10 Int.J.Mod.Phys. E27, 1850088 (2018) Model of multiple Dirac eikonal scattering of protons by nuclei NUCLEAR REACTIONS 40Ca, 208Pb(p, p), E=800 MeV; calculated σ(θ), analyzing powers using model of multiple Dirac eikonal scattering.
doi: 10.1142/S021830131850088X
2017BE09 Int.J.Mod.Phys. E26, 1750027 (2017) Yu.A.Berezhnoy, G.M.Onyshchenko, V.V.Pilipenko Analysis of α-12C elastic scattering at intermediate energies by the S-matrix model NUCLEAR REACTIONS 12C(α, α), E=65-386 MeV; calculated σ, S-matrix parameters. Comparison with available data.
doi: 10.1142/S0218301317500276
2016KU25 Phys.Rev. C 94, 064612 (2016) Microscopic optical potential for 4He scattering based on the effective Skyrme interaction NUCLEAR REACTIONS 58Ni(α, α), E=29, 34, 58, 82, 104 MeV; 90Zr(α, α), E=40, 59.1, 79.5, 99.5, 104 MeV; 120,124Sn(α, α), E=50.5, 104 MeV; 208Pb(α, α), E=50, 58, 104, 139 MeV; calculated σ(θ, E) by single-folding α+A microscopic optical potentials (MOP) with different NA potentials. 28Si(α, α), (α, α'), E=45 MeV; 58Ni(α, α), (α, α'), E=58, 104 MeV; 58Fe(α, α), (α, α'), E=64.5 MeV; 90Zr(α, α), (α, α'), E=40 MeV; 208Pb(α, α), (α, α'), E=79 MeV; calculated σ(θ, E) using α+A MOP with the SkOP4 force for elastic and inelastic scattering. 28Si, 58Ni, 120Sn, 208Pb(α, X), E=20-200 MeV; calculated reaction σ(E) by the α+A MOP with the SkOP4 force, by the SFM using the global NA potential KD2003, and global α+A potential. Comparison with experimental results.
doi: 10.1103/PhysRevC.94.064612
2015BE12 Int.J.Mod.Phys. E24, 1530004 (2015) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko Intermediate energy multiple scattering of particles by light α-cluster nuclei NUCLEAR REACTIONS 12C, 16O, 20Ne, 24Mg, 13C, 13N, 9Be(p, p), (p, p'), E<200 MeV; calculated charge radii and densities, form factors, σ(θ), scattering parameters, polarization. Multiple diffraction scattering theory (MDST) and the α-cluster model with dispersion, comparison with experimental data.
doi: 10.1142/S0218301315300040
2015PI07 Phys.Rev. C 92, 014616 (2015) Description of elastic polarized-deuteron scattering in the optical model with Skyrme forces NUCLEAR REACTIONS 208Pb(polarized d, d), E=28.8 MeV; 58Ni, 120Sn(polarized d, d), E=28.6 MeV; 60Ni(polarized d, d), E=15, 22, 34.4 MeV; 90Zr(polarized d, d), E=15, 22, 28.8 MeV; 58Ni, 208Pb(polarized p, p), E=16 MeV; 58Ni, 208Pb(polarized n, n), E=14 MeV; calculated σ(θ), analyzing powers Ay(θ), vector (iT11(θ)) and tensor (T2m(θ)) analyzing powers. Microscopic optical potentials (MOP) with Watanabe-type approximation and different Skyrme forces of SkOP, SkOP3, SLy5*, SLyIII.0.8, CH89, and BSk24. Comparison with experimental data, and with calculations with CDCC model using FRESCO code.
doi: 10.1103/PhysRevC.92.014616
2014BE17 Phys.Rev. C 90, 014611 (2014) Yu.A.Berezhnoy, D.V.Fedorchenko, V.V.Pilipenko, V.P.Mikhailyuk Intermediate-energy deuteron scattering from α-cluster nuclei NUCLEAR REACTIONS 4He, 12C, 16O(d, d), E=400, 700 MeV; calculated σ(θ, E), Ay(θ, E), Ayy(θ, E) and Axx(θ, E) analyzing powers. Three-body n+p+α (TB), and rigid projectile (RP) approximations. Multiple diffraction scattering theory and α-cluster model with dispersion. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.014611
2014KU29 Phys.Atomic Nuclei 77, 1378 (2014); Yad.Fiz. 77, 1443 (2014) Elastic proton-nucleus scattering in the Glauber-Sitenko approach and relativistic and nonrelativistic nuclear mean fields NUCLEAR REACTIONS 40Ca, 208Pb(p, p), E=800 MeV; calculated σ(θ), analyzing power, spin-rotation functions. Glauber-Sitenko approach.
doi: 10.1134/S106377881410010X
2013BE27 Phys.Atomic Nuclei 76, 862 (2013); Yad.Fiz. 76, 914 (2013) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko, D.V.Fedorchenko Elastic deuteron scattering on 12C and 16O nuclei in the alpha-cluster model NUCLEAR REACTIONS 12C, 16O(d, d), E=400, 700 MeV; calculated σ(θ), amplitude parameters. Comparison with available data.
doi: 10.1134/S1063778813060045
2012BE05 Eur.Phys.J. A 48, 4 (2012); Erratum Eur.Phys.J. A 48, 26 (2012) Yu.A.Berezhnoy, D.V.Fedorchenko, V.P.Mikhailyuk, V.V.Pilipenko Polarization phenomena in the intermediate energy elastic deuteron scattering from 16C and 16O nuclei NUCLEAR REACTIONS 16C, 16O(d, d), E=400, 700 MeV; calculated σ(θ), analyzing powers using multiple diffraction α cluster model scattering theory. Comparison with published data.
doi: 10.1140/epja/i2012-12004-y
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
2012PI15 Phys.Rev. C 86, 064613 (2012) Extended Skyrme interaction in the microscopic optical model of nucleon-nucleus scattering NUCLEAR REACTIONS 58Ni(n, n), E=10, 13.9, 17, 24 MeV; 58Ni(p, p), E=10.7, 16, 20.4, 24.6 MeV; 90Zr(p, p), E=16, 30 MeV; 120Sn(n, n), E=13.9 MeV; 120Sn(p, p), E=16, 30.3 MeV; 208Pb(n, n), E=8, 10, 13.9, 40 MeV; 208Pb(p, p), E=21, 30.3, 40 MeV; calculated σ(E, θ), Ay(E, θ). 90Zr, 208Pb(n, X), E=1-75 MeV; 58Ni, 116Sn, 208Pb(p, X), E=10-70 MeV; calculated Reaction σ, total σ. Nucleon-nucleus microscopic optical potential model, with one-particle Green function mass operator, and extended Skyrme-force variant. Comparison with experimental data. NUCLEAR STRUCTURE 208Pb; calculated proton and neutron single-particle levels using different Skyrme forces. 40,48Ca, 54Fe, 58Ni, 82Se, 90Zr, 92Mo, 116,120Sn, 208Pb; calculated relative deviations in binding energies and charge radii using extended Skyrme forces. Comparison with experimental values.
doi: 10.1103/PhysRevC.86.064613
2011BE13 Phys.Atomic Nuclei 74, 580 (2011); Yad.Fiz. 74, 604 (2011) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko Interaction of intermediate-energy protons with 20Ne and 24Mg nuclei within the multiple-scattering model NUCLEAR REACTIONS 20Ne, 24Mg(p, p), (p, p'), E=250, 800 MeV; calculated σ(θ), polarization parameters. Multiple-scattering model, comparison with experimental data.
doi: 10.1134/S106377881104003X
2010BE07 Int.J.Mod.Phys. E19, 243 (2010) Y.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko The intermediate energy elastic scattering of protons by α-cluster 20Ne and 24Mg nuclei NUCLEAR REACTIONS 20Ne, 24Mg(p, p), E=200, 250, 297, 800 MeV; calculated density parameters, rms radii, charge formfactors, σ(θ).
doi: 10.1142/S0218301310014698
2010GR01 Int.J.Mod.Phys. E19, 449 (2010) K.A.Gridnev, V.N.Tarasov, D.V.Tarasov, D.K.Gridnev, V.V.Pilipenko, W.Greiner Theoretical prediction of extremely neutron rich Zr and Pb NUCLEAR STRUCTURE 150,152Zr, 224,226,230,232,266,268,270,272,274,276,278,280,282,284,286,288Pb;calculated one-neutron separation energies, neutron and proton parameters of quadrupole deformation; deduced existence of island of stability around 152Zr; Deformed HF calculations with Skyrme forces.
doi: 10.1142/S0218301310014868
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.
2009BE05 Eur.Phys.J. A 39, 125 (2009) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko Intermediate energy elastic scattering of protons on 24Mg in the α-cluster model with dispersion NUCLEAR REACTIONS 4He(p, p), E=200, 800 MeV; 24Mg(p, p), E=250, 800 MeV; calculated σ(θ), other observables using an α-cluster model. Comparison with data.
doi: 10.1140/epja/
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
2008TA20 Phys.Atomic Nuclei 71, 1255 (2008); Yad.Fiz. 71, 1283 (2008) V.N.Tarasov, D.V.Tarasov, K.A.Gridnev, D.K.Gridnev, W.Greiner, V.G.Kartavenko, V.V.Pilipenko Properties of lead isotopes in the vicinity of the neutron drip line NUCLEAR STRUCTURE 266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282,283,284,285,286,287,288Pb; calculated S(1n), S(2n), quadrupole deformation parameters, root mean square radii; HF+BCS, HFB approximation; Skyrme forces.
doi: 10.1134/S1063778808070193
2007BE67 Vis.Khar.Nat.Univ. 777, n.2(34) p.33 (2007) Analysis of charge form factors of the 61Li nucleus on the basis of cluster mode NUCLEAR STRUCTURE 6Li; calculated form factors. Cluster model.
2007KU11 Phys.Atomic Nuclei 70, 1036 (2007); Yad.Fiz. 70, 1071 (2007) A.V.Kuznichenko, G.M.Onyshchenko, V.V.Pilipenko, N.Burtebayev, G.S.Zhurynbaeva Analysis of elastic and inelastic α + 24Mg scattering within the S matrix model involving Regge poles NUCLEAR REACTIONS 24Mg(α, α), E=50-119 MeV; analyzed elastic scattering cross sections data using a phenomenological S-matrix model.
doi: 10.1134/S1063778807060063
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
2005BE46 Yad.Fiz. 68, 978 (2005); Phys.Atomic Nuclei 68, 940 (2005) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko Elastic and Inelastic Scattering of 800-MeV Protons on 16O and 20Ne Nuclei NUCLEAR REACTIONS 16O, 20Ne(p, p), (p, p'), E=800 MeV; calculated σ(θ), polarization observables. Multiple diffractive scattering, α-cluster model, comparison with data.
doi: 10.1134/1.1954820
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
2005KU41 Bull.Rus.Acad.Sci.Phys. 69, 27 (2005) A.V.Kuznichenko, G.M.Onishchenko, V.V.Pilipenko, N.Burtebaev Analysis of 16O + 28Si scattering cross sections, based on S-matrix approach NUCLEAR REACTIONS 28Si(16O, 16O'), E=32-142.5 MeV; analyzed σ(θ); deduced role of isolated Regge poles in describing anomalous backward scattering. Phenomenological S-matrix model.
2005KU45 Vis.Khar.Nat.Univ. 610, n.3(28) p.21 (2005) A.V.Kuznichenko, G.M.Onyshchenko, V.V.Pilipenko, N.Burtebaev Description of elastic scattering and quasielastic charge-exchange reaction of 3He on carbon nuclei in the S-matrix model with regge poles NUCLEAR REACTIONS 13,14C(3He, t), E=39.6, 72 MeV; analyzed σ(θ); deduced new model for elastic and charge-exchange reactions.
2004BE62 Bull.Rus.Acad.Sci.Phys. 68, 1743 (2004) Yu.A.Berezhnoi, V.P.Mikhailyuk, V.V.Pilipenko Multiple elastic scattering of protons form 16O and 20Ne nuclei within an independent nucleon model NUCLEAR REACTIONS 16O, 20Ne(p, p), E=800 MeV; calculated σ(θ), polarization, spin rotation function. Independent nucleon mode, comparison with data.
2003BE79 Iader.Fiz.Enerh. 4 no.1, 7 (2003) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko Polarization phenomena in the elastic scattering of protons on 4He nuclei and energy dependence of p-α amplitude parameters NUCLEAR REACTIONS 4He, 16O(p, p), E=200-1000 MeV; calculated σ(θ), polarization observables. Multiple diffraction scattering theory and dispersive α-cluster model. Comparison with experimental data.
doi: 10.15407/jnpae
2003BE80 Iader.Fiz.Enerh. 4 no.3, 17 (2003) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko Charge densities of light nuclei in the α-cluster model with dispersion NUCLEAR STRUCTURE 9Be, 12,13C, 13N, 16O, 20Ne; calculated charge densities distribution, mean-square radii. Dispersive α-cluster model. Comparison to experimental data.
doi: 10.15407/jnpae
2003KU47 Bull.Rus.Acad.Sci.Phys. 67, 776 (2003) A.V.Kuznichenko, V.V.Pilipenko, G.M.Onishchenko, A.S.Dem'yanova, N.Burtebaev Refraction effects in 16O + 16O scattering at 124-1120 MeV and S-matrix model with Regge poles NUCLEAR REACTIONS 16O(16O, 16O), E=124-1120 MeV; analyzed σ(θ), refraction effects; deduced parameters. Phenomenological S-matrix model.
2002KU41 Bull.Rus.Acad.Sci.Phys. 66, 768 (2002) A.V.Kuznichenko, V.V.Pilipenko, G.M.Onishchenko, A.S.Demianova Analysis of Refraction Effects in 4He + 15N, 16O, and 16O + 12C Scattering within S-Matrix Model with Regge Poles NUCLEAR REACTIONS 15N, 16O(α, α), E ≈ 48-56 MeV; 12C(16O, 16O), E=200, 230 MeV; calculated σ(θ), refraction effects. S-matrix model, comparison with data.
2000AK04 Fiz.Elem.Chastits At.Yadra 31, 458 (2000); Phys.Part.Nucl. 31, 225 (2000) A.I.Akhiezer, Yu.A.Berezhnoi, V.V.Pilipenko Quantum Interference and Nuclear Optics
2000KU19 Yad.Fiz. 63, No 5, 852 (2000); Phys.Atomic Nuclei 63, 782 (2000) Analysis of Elastic Proton-Nucleus Scattering on the Basis of the Glauber-Sitenko Approach with Allowance for Intermediate Excitations of Nuclei NUCLEAR REACTIONS 40Ca, 54Fe, 208Pb(p, p), E=800 MeV; calculated σ(θ), polarization, spin-rotation function; deduced nuclear excitation effects. Glauber-Sitenko approach, comparisons with data.
doi: 10.1134/1.855707
1999PI15 Yad.Fiz. 62, No 9, 1576 (1999); Phys.Atomic Nuclei 62, 1482 (1999) Refraction Effects in Cross Sections for Nuclear Scattering and Poles of the S Matrix NUCLEAR REACTIONS 90Zr(α, α), E=40, 59.1, 79.5 MeV; 16O(16O, 16O), E=350 MeV; calculated σ(θ); deduced refraction effects, role of Regge poles. S-matrix model, comparison with data.
1998PI02 Yad.Fiz. 61, No 3, 467 (1998); Phys.Atomic Nuclei 61, 406 (1998) Elastic Scattering of 6Li Nuclei by Nuclei and S-Matrix Approach NUCLEAR REACTIONS 12C, 28Si(6Li, 6Li), E=210, 318 MeV; 40Ca(6Li, 6Li), E=210 MeV; calculated σ(θ). S-matrix approach. Comparison with optical model, data.
1998PI08 Mod.Phys.Lett. A 13, 211 (1998) 16O-16O Elastic Scattering at 350 MeV and Pole Structure of the S-Matrix NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; calculated σ(θ); deduced S-matrix features. Comparison with data.
doi: 10.1142/S0217732398000267
1996BE93 Bull.Rus.Acad.Sci.Phys. 60, 791 (1996) Cross Sections for Elastic Scattering of 158 MeV 9Be Nuclei by Various Nuclei NUCLEAR REACTIONS 12C, 16O, 26Mg, 27Al, 40Ca, 60Ni, 197Au(9Be, 9Be), E=158 MeV; analyzed σ(θ). S-matrix model.
1996BF04 Acta Phys.Hung.N.S. 3, 249 (1996) S-Matrix Approach for Description of Refraction and Absorption Effects in 9Be Elastic Scattering NUCLEAR REACTIONS 12C, 16O, 26Mg, 27Al, 40Ca, 60Ni, 197Au(9Be, 9Be), E=158 MeV; analyzed σ(θ); deduced S-matrix parameters. Comparison with optical model.
1995BE60 Bull.Rus.Acad.Sci.Phys. 59, 528 (1995) S-Matrix Approach to Scattering of Light Nuclei by Nuclei NUCLEAR REACTIONS 90Zr(α, α), E=118, 99.5 MeV; 90Zr, 12C, 40Ca(6Li, 6Li), E=156 MeV; 28Si(18O, 18O), E=352 MeV; 28Si(16O, 16O), E=1503 MeV; analyzed σ(θ). S-matrix approach, scattering amplitude decomposition into close, distant composition.
1993BE09 Z.Phys. A344, 411 (1993) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko The Antiproton-Nucleus Elastic Scattering and the Alpha-Cluster Model with Dispersion NUCLEAR REACTIONS 16O, 4He, 12C(polarized p-bar, p-bar), E=179 MeV; calculated polarization, σ(θ), spin rotation function vs θ. Dispersion, multiple diffraction theories, α-cluster model.
1992BE03 J.Phys.(London) G18, 85 (1992) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko Elastic and Inelastic Intermediate-Energy Proton Multiple Scattering on 12C and 16O Nuclei NUCLEAR REACTIONS 12C(polarized p, p), E=398, 800 MeV; 16O(polarized p, p), E=800 MeV; calculated σ(θ), polarization spin rotation parameter vs θ. Multiple diffraction scattering theory, α-cluster model, nucleon transition densities.
doi: 10.1088/0954-3899/18/1/008
1992BE24 Yad.Fiz. 55, 1885 (1992); Sov.J.Nucl.Phys. 55, 1044 (1992) Yu.A.Berezhnoi, V.P.Mikhailyuk, V.V.Pilipenko Elastic and Inelastic Scattering of Intermediate-Energy Protons by Carbon and Oxygen Nuclei NUCLEAR REACTIONS 12C(polarized p, p), (polarized p, p'), E=398, 800 MeV; 16O(polarized p, p'), E=800 MeV; calculated σ(θ), P(θ), spin rotation function vs θ. Multiple diffraction scattering, α-cluster model transition densities.
1991BE45 Acta Phys.Pol. B22, 873 (1991) Yu.A.Berezhnoy, V.P.Mikhailyuk, V.V.Pilipenko The 200 and 398 MeV Elastic Scattering of Protons on α-Cluster Nuclei NUCLEAR REACTIONS 12C, 16O(polarized p, p), E=200, 398 MeV; calculated σ(θ), polarization observables. Multiple diffraction scattering, α-cluster model with dispersion.
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.
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.
1988BE57 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2185 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 104 (1988) Yu.A.Berezhnoi, V.P.Mikhailyuk, V.V.Pilipenko Polarization Phenomena in the Elastic Scattering of Protons by Oxygen Nuclei and the α-Particle Model NUCLEAR REACTIONS 16O(polarized p, p), E=800 MeV; calculated σ(θ), polarization, spin-rotation function vs θ. 4He(polarized p, p), E=800 MeV; calculated σ, P vs transmitted four momentum square.
1986BE45 Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 2050 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.10, 177 (1986) Yu.A.Berezhnoi, A.V.Kuznichenko, G.M.Onishchenko, V.V.Pilipenko Rainbow Scattering in Nuclear Processes NUCLEAR REACTIONS 40Ca, 58Ni, 90Zr, 116Sn(3He, 3He), E=109.2 MeV; 40,42,44,48Ca, 50Ti, 52Cr, 58Ni(α, α), E=104, 139, 141.7 MeV; 12C, 28Si(6Li, 6Li), E=90, 54 MeV; 58Ni(3He, 3He), (3He, t), E=118.5 MeV; calculated elastic, reaction σ ratios, σ(θ); deduced rainbow effect role.
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.
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.
1985BE36 J.Phys.(London) G11, 1161 (1985) Rainbow Scattering in Quasi-Elastic Nuclear Reactions NUCLEAR REACTIONS 40Ca, 58Ni(3He, 3He), E=109.2 MeV; 58Ni(3He, 3He), E=118.5 MeV; 24Mg, 32S(α, α), E=166 MeV; 40Ca(α, α), E=141.7 MeV; 58Ni(α, α'), E=139 MeV; 58Ni(3He, t), E=118 MeV; calculated σ(θ); deduced rainbow scattering role. Nuclear scattering phase real part model independent determination.
doi: 10.1088/0305-4616/11/10/012
1984BE01 J.Phys.(London) G10, 63 (1984) Yu.A.Berezhnoy, V.V.Pilipenko, G.A.Khomenko Polarization in Proton-Carbon Elastic Scattering and the α-Particle Model with Dispersion NUCLEAR REACTIONS 12C(p, p), (polarized p, p), E=1 GeV; calculated σ(θ), polarization, spin rotation function vs θ, form factor vs transferred momentum. Dispersion theory, α-particle model.
doi: 10.1088/0305-4616/10/1/011
1983BE24 Yad.Fiz. 37, 891 (1983) Charge Exchange Reactions Involving Three-Nucleon Nuclei at Intermediate Energies NUCLEAR REACTIONS 58,60,62Ni(3He, t), E=37.5 MeV; 11B(3He, t), E=217 MeV; calculated σ(θ), σ. Multiple diffraction scattering theory.
1983BE58 Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 2240 (1983) Elastic and Inelastic Scattering of Light Ions by Nuclei in the Intermediate Energy Region NUCLEAR REACTIONS 58Ni(α, α), (α, α'), E=139 MeV; calculated σ(θ), phase shifts. Legendre-Bessel function method.
1981BE61 Izv.Akad.Nauk SSSR, Ser.Fiz. 45, 1953 (1981) Yu.A.Berezhnoi, V.V.Pilipenko, G.A.Khomenko Proton Polarization Elastic Scattering by 12C and the α-Particle Model NUCLEAR REACTIONS 4He, 12C(polarized p, p), E=1 GeV; calculated σ(θ), P(θ). Alpha particle model.
1980BE58 Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 1950 (1980) Yu.A.Berezhnoi, V.V.Pilipenko, G.A.Khomenko Elastic Electron and Proton Scattering by 12C in the α-Particle Model NUCLEAR REACTIONS 12C(p, p), E=1.04 GeV; calculated σ(θ); 12C(e, e), E=600-800 MeV; calculated form factor. Alpha-particle model.
1979BE63 Izv.Akad.Nauk SSSR, Ser.Fiz. 43, 1006 (1979); Bull.Acad.Sci.USSR, Phys.Ser. 43, No.5, 93 (1979) Diffraction Model of Charge-Exchange Reactions NUCLEAR REACTIONS 46,47,48,49,50Ti, 58,60,61,62,64Ni, Fe(3He, t), E not given; calculated σ(θ). Diffraction model.
Back to query form |