NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = A.Osman Found 75 matches. 2012OS02 J.Korean Phys.Soc. 60, 722 (2012) 12C-induced multifragmentation of heavy-ion reactions NUCLEAR REACTIONS 197Au(12C, X), E=84 MeV/nucleon; calculated σ(θ). Comparison with available data.
doi: 10.3938/jkps.60.722
2009OS01 Acta Phys.Pol. B40, 2345 (2009) Density Dependent Nucleon-Nucleus Optical Potential in the (p, n) Reactions NUCLEAR REACTIONS 13C, 70Zn, 96Zr, 112Sn, 124Sn, 208Pb(p, n), E=23, 26, 35 MeV; calculated neutron spectra, σ(θ). DWBA calculations with the optical model potential.
2002OS03 Acta Phys.Slovaca 52, 173 (2002) Electromagnetic Properties of 3He NUCLEAR STRUCTURE 3He; calculated electromagnetic form factors. Hyperspherical formalism, comparison with data, other models.
1999OS05 Acta Phys.Hung.N.S. 10, 73 (1999) Angular Distributions of the Multifragmentation of Deformed Nuclei in Heavy Ion Reactions NUCLEAR REACTIONS 19F(9Be, X), E=35-407 MeV; calculated fission fragments angular distributions following compound nucleus decay. Statistical scission model.
1996OS07 Nuovo Cim. 109A, 1449 (1996) Multifragmentation of 24Mg + 24Mg Heavy-Ion Reactions Leading to Alpha-Particles NUCLEAR REACTIONS 24Mg(24Mg, F), E(cm)=35-80 MeV; calculated σ(θα) following primary fission fragment breakup. Statistical scission model.
doi: 10.1007/BF02780615
1995OS04 Nuovo Cim. 108A, 155 (1995) Angular Distributions of Alpha Fragments from Carbon-Induced Fission NUCLEAR REACTIONS 12C(12C, F), E=70-160 MeV; calculated σ(θα) following fission at various temperatures. Statistical scission model, 6α fragmentation product.
doi: 10.1007/BF02816736
1994OS01 Nuovo Cim. 107A, 207 (1994) The J-Dependent Distorting Optical-Model Potential in Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 24Mg(16O, 20Ne), E=27.8 MeV; 24Mg(16O, 12C), E=27.8-32.6 MeV; 32S(16O, 12C), E=45.5 MeV; 54Fe(16O, 12C), E=46 MeV; 48Ca(16O, 14C), E=50.5 MeV; 64Ni(16O, 14C), 76Ge(16O, 12C), E=56 MeV; 24Mg(18O, 16O), E=50 MeV; analyzed σ(θ). 20Ne, 28Si, 36Ar, 58Ni, 50Ti, 66Zn, 80Se, 26Mg levels deduced spectroscopic factors. Exact finite range DWBA.
doi: 10.1007/BF02781553
1994OS05 Can.J.Phys. 72, 175 (1994); Erratum Can.J.Phys. 72, 686 (1994) Contributions of Density-Dependent Interactions in Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 16O(6Li, d), E=75.4 MeV; 16O(6Li, α), E=34 MeV; 16O(16O, 12C), E=22.75-27.25 MeV; 24Mg(16O, 12C), E=35.5, 36.2 MeV; 28Si(16O, 12C), E=26.3 MeV; 32S(16O, 12C), E=45.5 MeV; 18O(6Li, d), E=72.3 MeV; 24Mg(12C, 16O), E=25.2 MeV; calculated σ(θ); deduced model parameters. 18F, 22,20Ne, 28Si, 32S, 36Ar levels deduced spectroscopic factors. DWBA, density-dependent interactions.
doi: 10.1139/p94-028
1994OS08 Int.J.Mod.Phys. E3, 219 (1994) Contribution of the Parity Dependent Potential in Heavy Ion Transfer Reactions NUCLEAR REACTIONS 9Be(16O, 12C), E=7.2-10.2 MeV; 16O(7Li, α), E=20 MeV; 154Sm(12C, 14C), E=65 MeV; 186W, 192Os(12C, 14C), E=70 MeV; 186W(12C, 10Be), E=70 MeV; analyzed σ(θ). 19F, 152Sm, 184W, 190,188Os, 13C levels deduced spectroscopic factors. Exact finite-range DWBA.
doi: 10.1142/S0218301394000097
1993OS08 Can.J.Phys. 71, 455 (1993) Magnetic Form Factors for a Trinucleon System using Different Meson Exchange Nucleon-Nucleon Interactions NUCLEAR STRUCTURE 3He, 3H; calculated magnetic form factors. Faddeev approach, realistic two-body potentials with different meson exchange effects.
doi: 10.1139/p93-071
1992OS06 Indian J.Pure Appl.Phys. 30, 137 (1992) The Dynamical Mass Asymmetry-Neck Mixing Mass Parameter in Nuclear Fission NUCLEAR STRUCTURE 236,238U; calculated fission mass asymmetry-neck mixing mass parameter vs mass asymmetry, fragment deformation; deduced collective coordinates role.
1992OS08 Acta Phys.Acad.Sci.Hung. 71, 99 (1992) A.Osman, S.S.Abdel-Aziz, M.M.Gogary Trajectory Studies for the Fusion of Two Heavy Nuclei NUCLEAR STRUCTURE 255Db; 286Mc; A=210; A=193; calculated neck size, asymmetry trajectories. Two fusing nuclei, dynamical equations of motion.
1991OS04 Nuovo Cim. 104A, 1563 (1991) Differential Cross-Sections of Cluster Transfer Heavy-Ion Reactions in the Whole Angle Region NUCLEAR REACTIONS 16O(7Li, α), E=20 MeV; 24Mg(16O, 12C), E=27.8, 36.2 MeV; 28Si(16O, 12C), E=26.23 MeV; analyzed σ(θ). 19F, 28Si, 32S levels deduced spectroscopic factor. Exact finite-range DWBA.
doi: 10.1007/BF02817439
1991OS05 Ann.Phys.(Leipzig) 48, 248 (1991) The Deformations Energy and Barrier Height of Super Heavy Nuclei NUCLEAR STRUCTURE 250Rf, 251Rf, 250,251Es; calculated deformation energy, fission barrier height.
doi: 10.1002/andp.19915030403
1990OS02 Acta Phys.Acad.Sci.Hung. 67, 367 (1990) Dependence of the Interaction Potential and Fusion Cross-Section on Temperature NUCLEAR REACTIONS 166Er(84Kr, X), 122Sn(129Xe, X), E not given; calculated interaction potential vs internuclear distance; deduced fusion σ, interaction potential temperature dependences. Thomas-Fermi model.
1990OS03 Nuovo Cim. 103A, 1693 (1990) Cluster-Stripping Reactions in the Heavy-Ion Collisions NUCLEAR REACTIONS 14C(6Li, d), E=34 MeV; 16O(7Li, α), E=20 MeV; 16O(16O, 12C), E=50-68 MeV; 24Mg(16O, 12C), E=27.8-36.2 MeV; 28Si(16O, 12C), E=50-72 MeV; calculated σ(θ), form factors. 28Si, 30S, 18O, 19F, 20Ne levels deduced spectroscopic factors. Cluster-stripping, exact finite-range DWBA.
doi: 10.1007/BF02887294
1989OS02 J.Phys.(London) G15, 871 (1989) Direct Reaction Mechanism for Heavy Ion Reactions with Particle Transfer NUCLEAR REACTIONS 16O(12C, 8Be), (13C, 9Be), (16O, 12C), 58,62Ni(28Si, 30Si), 28Si(32S, 36Ar), E=13-140 MeV; calculated σ(θ). 20Ne, 56,60Ni, 24Mg levels deduced spectroscopic factors. Exact finite-range DWBA analysis.
doi: 10.1088/0954-3899/15/6/016
1989OS07 Nuovo Cim. 102A, 965 (1989) Dependence of Neck Mass Parameter on Collective Coordinates in Nuclear Fission NUCLEAR STRUCTURE 235U; calculated fission neck parameter vs fragment mass asymmetry, fragment deformation. Cranking model, collective coordinates.
1989OS08 Nuovo Cim. 102A, 1223 (1989) Mass Distributions in Different Fissioning Nuclei NUCLEAR REACTIONS 236U(γ, F), E ≈ 5-7 MeV; 238U(γ, F), E ≈ 6-28 MeV; calculated fission σ(E), fragment mass, charge distributions. Asymmetric two-center shell model.
doi: 10.1007/BF02800333
1989OS09 Ann.Phys.(Leipzig) 46, 408 (1989) Dynamical Behaviour of the Mass Asymmetry Mass Parameter in Nuclear Fission NUCLEAR STRUCTURE 236,238U; calculated fission mass asymmetry mass parameter vs neck parameter, temperature. Dynamical treatment.
doi: 10.1002/andp.19895010603
1989OS10 Ann.Phys.(Leipzig) 46, 587 (1989) Mass Distributions and Charge Dispersion for the Nuclear Fission NUCLEAR STRUCTURE 238U; calculated fission fragment yield mass, charge distributions. Asymmetric two center shell model.
doi: 10.1002/andp.19895010805
1988OS03 Nuovo Cim. 100A, 271 (1988) Total Disintegration of Three-Nucleon Systems from Charged π-Mesons Reactions NUCLEAR REACTIONS 3He(π-, π+), E=140 MeV; analyzed σ(θ). Faddeev formalism.
doi: 10.1007/BF02804923
1988OS04 Ann.Phys.(Leipzig) 45, 331 (1988) Bound Three Alpha Particles Model for the 12C Nucleus as a Three-Body Problem NUCLEAR STRUCTURE 12C; calculated α-α interaction form factor for different levels.
doi: 10.1002/andp.19885000503
1988OS05 Ann.Phys.(Leipzig) 45, 379 (1988) Coulomb Forces in Three Charged Particles Interacting via Stripping Nuclear Reactions NUCLEAR REACTIONS 12C(6Li, d), E=42 MeV; calculated σ(θ). Alpha particle transfer.
doi: 10.1002/andp.19885000509
1988OS06 Czech.J.Phys. B38, 837 (1988) Collective Mass Parameters in the Nuclear Fission Process NUCLEAR STRUCTURE 236,238U; calculated effective mass parameter in fission.
doi: 10.1007/BF01601831
1988OS07 Nuovo Cim. 100A, 927 (1988) Fragmentation of Nuclei to Three Heavy Fragments NUCLEAR STRUCTURE A=120; calculated average temperature, fragment mass distributions, mass spectra. Three heavy fragment emission.
doi: 10.1007/BF02789011
1987OS02 Acta Phys.Pol. B18, 381 (1987) Coulomb Effects in Deuteron Stripping Reactions as a Three-Body Problem NUCLEAR REACTIONS 28Si(d, p), E=18 MeV; 40Ca(d, p), E=7 MeV; analyzed σ(θ). 29Si, 41Ca level deduced spectroscopic factors. Three-body interpretation of Coulomb effects.
1987OS03 Indian J.Pure Appl.Phys. 25, 1 (1987) Four-Body Problem for Four Bound Alpha Particles in 16O NUCLEAR STRUCTURE 8Be, 12C, 16O; calculated binding energy. α-cluster model.
1987OS04 Ann.Phys.(Leipzig) 44, 612 (1987) Dependence of the Three-Nucleon Binding Energy on Some Different Effects NUCLEAR STRUCTURE 3H; calculated binding energy. Faddeev formalism.
doi: 10.1002/andp.19874990810
1986OS04 Acta Phys.Pol. B17, 209 (1986) The Effect of Including Tensor Forces in Nucleon-Nucleon Interaction on Three-Nucleon Binding Energy NUCLEAR STRUCTURE 3H, 3He; calculated binding energy; deduced tensor forces role. Faddeev equations, separable interactions.
1986OS05 Indian J.Pure Appl.Phys. 21, 65 (1986) Rearrangement Heavy Ion Collisions with a Single Nucleon Transfer NUCLEAR REACTIONS 26Mg(13C, 12C), E=35 MeV; 40Ca(13C, 12C), E=60, 68 MeV; 74Ge(18O, 17O), E=75 MeV; 144Sm(13C, 14C), E=66 MeV; 208Pb(16O, 17O), E=104, 138.5, 216.6 MeV; 48Ca(14N, 13C), E=50 MeV; 40Ca(13C, 14N), E=40 MeV; 60Ni(18O, 19F), E=65 MeV; calculated σ(θ). Rearrangement process, DWBA formalism.
1986OS07 Radiat.Eff. 95, 145 (1986) The Effect of Tensor Forces in the Three-Body Calculations NUCLEAR STRUCTURE 3H, 3He, 6Li; calculated binding energies. Three body model.
doi: 10.1080/00337578608208682
1985OS03 Acta Phys.Pol. B16, 59 (1985) Study of the 6Li Nucleus as a Three-Body Problem NUCLEAR STRUCTURE 6Li; calculated binding energies, form factors. Three-body model.
1985OS06 Acta Phys.Pol. B16, 865 (1985) Heavy Ion Reactions with Alpha Particle Transfer NUCLEAR REACTIONS 12C(13C, 9Be), E=36 MeV; calculated σ(θ); deduced potential parameters. 16O levels deduced spectroscopic factors. Coulomb wave, distorted wave Born approximations.
1984OS01 Int.J.Theor.Phys. 23, 15 (1984) Three-Body Model for Stripping Nuclear Reactions NUCLEAR REACTIONS 28Si(d, d), (d, p), E=18 MeV; 40Ca(d, d), (d, p), E=7 MeV; calculated σ(θ). 29Si, 41Ca level deduced spectroscopic factors. Three-body model, separable potentials.
doi: 10.1007/BF02080669
1983OS01 Phys.Rev. C27, 650 (1983) A.Osman, M.Y.Ismail, M.M.Osman Heavy-Ion Reactions with Nucleon Transfer using Skyrme-Type Potential NUCLEAR REACTIONS 28Si(13C, 12C), 32S(13C, 14N), E=36 MeV; 29,30Si(16O, 15N), E=60 MeV; 28Si(10B, 9Be), E=59 MeV; 27Al(32S, 31P), E=100 MeV; calculated σ(θ). 28,29Si, 29,30,31P levels deduced S. Finite-range DWBA calculations, Skyrme type interaction potential.
doi: 10.1103/PhysRevC.27.650
1983OS02 Nuovo Cim. 73A, 27 (1983) Two-Nucleon Transfer Reactions with Form Factor Models NUCLEAR REACTIONS 31P(t, p), E=12.1 MeV; 96Zr, 116,118Sn, 208Pb(t, p), E=20 MeV; 210Pb(p, t), E=20 MeV; analyzed σ(θ). Form factor models.
doi: 10.1007/BF02728065
1983OS03 Int.J.Theor.Phys. 22, 341 (1983) Coulomb Forces in the Three-Body Problem with Application to Direct Nuclear Reactions NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, d), E=42 MeV; 16O(6Li, d), E=32 MeV; 12C(6Li, α), E=33 MeV; calculated σ(θ). Modified Faddeev equations, Coulomb Green's functions.
doi: 10.1007/BF02082899
1983OS05 Phys.Rev. C28, 1025 (1983) Elastic and Rearrangement Scattering between Two Interacting Deuterons as a Four-Body Problem NUCLEAR REACTIONS 2H(d, p), (d, n), (d, d), E=6.1-51.5 MeV; calculated σ(θ); deduced spectroscopic, normalization factors. Four-body model.
doi: 10.1103/PhysRevC.28.1025
1983OS07 Acta Phys.Acad.Sci.Hung. 54, 9 (1983) Rearrangement Heavy Ion Collisions with Two Nucleon Transfer NUCLEAR REACTIONS 16O(10B, 8Li), (10B, 8B), E=100 MeV; 42,48Ca(16O, 14C), E=56 MeV; 26Mg, 48Ca(18O, 16O), E=50 MeV; 42,48Ca(16O, 18O), E=65 MeV; 76Ge(16O, 18O), E=77.56 MeV; analyzed σ(θ); deduced optical model parameters. 18Ne, 18O, 44,50Ti, 28Mg, 40,46,50Ca, 62Ni, 74,76Ge levels deduced spectroscopic factors. Rearrangement heavy ion collisions.
1983OS08 Acta Phys.Acad.Sci.Hung. 54, 25 (1983) Heavy Ion Reactions with Single Neutron Transfer NUCLEAR REACTIONS 16O, 32S(13C, 12C), E=36 MeV; 60Ni(13C, 12C), E=60.83 MeV; 12C(14N, 13N), E=100 MeV; 208Pb(16O, 15O), E=139 MeV; 28Si, 40,48Ca, 54Fe(18O, 17O), E=50 MeV; 16O(10B, 11B), E=100 MeV; 16O(14N, 15N), E=155 MeV; 27Al(32S, 33S), E=100 MeV; analyzed σ(θ); deduced model parameters. 17O, 33S, 61Ni, 13C, 209Pb, 29Si, 41,49Ca, 55Fe, 15O, 26Al levels deduced spectroscopic factors.
1981OS06 J.Phys.(London) G7, 347 (1981) A.Osman, M.Y.Ismail, M.M.Osman Optical-Model Potential Using a Generalised Skyrme Force NUCLEAR REACTIONS 28Si, 32S, 40Ca, 208Pb(n, n), E=11, 14.5, 20, 26 MeV; 40Ca, 58Ni, 208Pb(p, p), E=21.3, 30.3, 61.4 MeV; calculated σ(θ), polarization vs θ. Microscopic optical model, generalized Skyrme force.
doi: 10.1088/0305-4616/7/3/010
1979OS02 Phys.Rev. C19, 1127 (1979) Validity and Accuracy of Separable Potentials in Three-Body Calculations NUCLEAR STRUCTURE 3H, 3He, 6Li, 9Be, 12C; calculated binding energies, three-body model, separable potentials, Faddeev equations.
doi: 10.1103/PhysRevC.19.1127
1979OS08 Nuovo Cim. 50A, 287 (1979) Three-Body Forces in the Nuclear Three-Body Problem NUCLEAR STRUCTURE 3H; calculated binding energy. Three-body forces treated to all orders, perturbation approach.
doi: 10.1007/BF02902008
1979OS09 Nuovo Cim. 50A, 13 (1979) Three-Body Correlations and Tensor Forces NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated binding energies. Three-body correlations, tensor forces.
doi: 10.1007/BF02804767
1979OS10 Ann.Phys.(Leipzig) 36, 56 (1979) 9Be(3He, n)11C and 11B(3He, n)13N Reactions at Energies below Coulomb Barrier NUCLEAR REACTIONS 9Be, 11B(3He, n), E=0.9-1.9 MeV; measured σ(θ). Coulomb distorted wave calculations.
doi: 10.1002/andp.19794910110
1979OS11 Ann.Phys.(Leipzig) 36, 64 (1979) The (d, p) Reactions below 3.0 MeV NUCLEAR REACTIONS 12C, 23Na, 27Al(d, p), E=1.5-3 MeV; measured σ(E, θ). Subcoulomb barrier stripping theory.
doi: 10.1002/andp.19794910111
1979OS12 Ann.Phys.(Leipzig) 36, 479 (1979) Cluster Description of Light Nuclei as a Three-Body Problem NUCLEAR STRUCTURE 6Li, 9Be, 12C; calculated binding energies. Cluster description, Faddeev three-body formalism.
doi: 10.1002/andp.19794910609
1978OS01 Phys.Rev. C17, 341 (1978) Three-Body Model of 9Be and 12C Nuclei NUCLEAR STRUCTURE 9Be, 12C; calculated binding energies. Three-body model.
doi: 10.1103/PhysRevC.17.341
1978OS07 Nuovo Cim. 48A, 121 (1978) Faddeev Equations for the 6Li Nucleus NUCLEAR STRUCTURE 6Li; calculated ground, excited state energies. Faddeev equations with α+p+n model.
doi: 10.1007/BF02799670
1977EL10 Ann.Phys.(Leipzig) 34, 91 (1977) Classical Description of Two-Cluster Transfer Reactions in a Coulomb Field NUCLEAR REACTIONS 16O(12C, α), E=3-18.5 MeV; 9Be(6Li, α), E=3.25 MeV; calculated σ(θ).
doi: 10.1002/andp.19774890203
1977OS03 Nuovo Cim. 37A, 201 (1977) Repulsive-Core Effects in (t, p) Stripping Reactions by Using a Tabakin Potential NUCLEAR REACTIONS 31P, 96Zr, 116Sn, 208Pb(t, p); calculated form factor.
doi: 10.1007/BF02858051
1977OS04 Phys.Rev. C16, 619 (1977) Short-Range Correlations with Pseudopotentials. VI NUCLEAR REACTIONS 28Si(d, p), E=18.0 MeV; 40Ca(d, p), E=7.0 MeV; measured σ(Ep, θ); deduced S. DWBA analysis.
doi: 10.1103/PhysRevC.16.619
1977OS05 Phys.Rev. C16, 873 (1977) Short-Range Correlations and Pseudopotentials. V NUCLEAR STRUCTURE 44,46,48,50Ti, 48,50,52,54Cr, 52,54,56,58Fe, 58,60,62,64Ni; calculated quadrupole moment, B(E2), levels. Hartree-Fock-Bogoliubov method.
doi: 10.1103/PhysRevC.16.873
1977OS06 Lett.Nuovo Cim. 19, 491 (1977) Nucleon-Nucleon Interaction in the Deuteron Break-up Process NUCLEAR REACTIONS 4He(d, pn), E < 30 MeV; calculated σ(E).
doi: 10.1007/BF02748209
1977OS07 Nuovo Cim. 41A, 199 (1977) Deuteron Stripping Reactions with the Tabakin Potential NUCLEAR REACTIONS 28Si, 32,34S, 36Ar, 40,48Ca, 50,52,54Cr(d, p); calculated σ(θ).
doi: 10.1007/BF02730102
1977OS08 Nuovo Cim. 39A, 138 (1977) Coulomb (3He, n) Stripping Reactions NUCLEAR REACTIONS 9Be, 11B(3He, n), E < 2 MeV; calculated σ(θ).
doi: 10.1007/BF02786502
1977OS09 Nuovo Cim. 42A, 330 (1977) Two-Nucleon Stripping Reactions with Tabakin Potential NUCLEAR REACTIONS 31P, 96Zr, 116,118Sn, 206Pb(t, p), E ≈ 20 MeV; calculated σ(θ).
doi: 10.1007/BF02862399
1976OS01 Phys.Rev. C13, 1 (1976) Spectroscopic Factors for (d, p) Stripping Reactions with Different Repulsive Core Nucleon-Nucleon Potentials NUCLEAR REACTIONS 28Si(d, p), E=18.0 MeV; 40Ca(d, p), E=7.0 MeV; measured σ(Ep, θ); deduced optical model parameters. 29Si, 41Ca levels deduced S. DWBA analysis.
doi: 10.1103/PhysRevC.13.1
1976OS07 Nuovo Cim. 35A, 201 (1976) Coulomb (d, p) Stripping Reactions NUCLEAR REACTIONS 12C, 23Na, 27Al(d, p), E < Coulomb barrier; calculated σ. 13C, 24Na, 28Al levels deduced S.
doi: 10.1007/BF02730051
1975OS01 Nuovo Cim. 25A, 571 (1975) Heavy-Ion Reactions with Nucleon Transfer NUCLEAR REACTIONS 14N, 10B(14N, 13N), 11B, 27Al(16O, 15N), 27Al(19F, 18F), E < 43 MeV; calculated σ(θ), Coulomb distortion.
doi: 10.1007/BF02729301
1975OS02 Lett.Nuovo Cim. 14, 413 (1975) Surface Distributions of Alpha-Particles in Heavy Nuclei NUCLEAR REACTIONS Au, Bi(C, α), E=126 MeV; Bi(C, α), E=105, 85 MeV; Bi, Au(O, α), E=168 MeV; Au(14N, α), E=147 MeV; analyzed σ(Eα, θ).
doi: 10.1007/BF02746867
1974OS02 Nuovo Cim. 22A, 345 (1974) Short-Range Correlations in (d, p) Stripping Reactions NUCLEAR REACTIONS 28Si, 32,34S, 36Ar(d, p), E=18 MeV; 40Ca(d, p), E=7, 8, 9, 10, 11, 12 MeV; calculated σ(Ep, θ). 29Si, 33,35S, 37Ar, 41Ca levels deduced S.
doi: 10.1007/BF02790623
1974OS03 Atomkernenergie 24, 55 (1974) Repulsive Core Effects in (d, p) Stripping Reactions Using a Tabakin Potential NUCLEAR REACTIONS 24Mg, 52Cr(d, p); calculated form factors.
1973OS03 Atomkernenergie 22, 62 (1973) Three-Body Model for Heavy Ion Reactions Using Projection Operators NUCLEAR REACTIONS 10B, 14N(14N, 13N); 11B, 27Al(16O, 15N), E=10-36 MeV; calculated σ(θ).
1973OS04 Atomkernenergie 22, 208 (1973) Rupulsive Core Effects via Direct Reactions NUCLEAR REACTIONS 28Si, 40Ca(d, p); calculated form factors, σ(θ); 96Zr, 118Sn(t, p); calculated form factors.
1972EL04 Phys.Lett. 39B, 156 (1972) Coulomb Disintegration of 6Li NUCLEAR REACTIONS Au(6Li, αd), E=22-36 MeV; calculated σ(E). Cluster model.
doi: 10.1016/0370-2693(72)90760-5
1972OS01 Particles Nucl. 3, 28 (1972) Theoretical Study of 6Li Induced Reactions. A Three-Body Problem Approach NUCLEAR REACTIONS 12C(6Li, d), E=13.33 MeV cms; 20Ne(6Li, d), E=13.85 MeV cms; calculated σ(θ). Soluble 3-body model.
1972OS04 Lett.Nuovo Cim. 4, 246 (1972) Repulsive Core Effects in (t, p) Stripping Reactions
doi: 10.1007/BF02757238
1972OS05 Part.Nucl. 4, 209 (1972) Short-Range Correlations in One- and Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 31P(t, p), E=12.1 MeV; 40,48Ca, 50,52,54Cr(d, p), E=10 MeV; 70Ge(p, d), 96Zr, 116,118Sn, 206Pb(t, p), 210Pb(p, t), E=20 MeV; measured nothing, calculated σ(θ). 33P, 41,49Ca, 51,53,55Cr, 69Ge, 98Zr, 118,120Sn, 208Pb deduced L, S.
1971OS02 Phys.Lett. 34B, 478 (1971) Three-Body Model for 6Li Induced Reactions NUCLEAR REACTIONS 12C(6Li, 6Li), (6Li, d), E=13.33 MeV; calculated σ(θ). Three-body model.
doi: 10.1016/0370-2693(71)90658-7
1971OS04 Phys.Rev. C4, 302 (1971) Modified Faddeev Equations for Three Bound α Particles in 12C NUCLEAR STRUCTURE 12C; calculated binding energy. α-cluster model, modified Faddeev equations.
doi: 10.1103/PhysRevC.4.302
1971OS05 Phys.Lett. 37B, 135 (1971) Alpha-8Be Asymptotic Wave Function as Three-α Particle Scattering NUCLEAR REACTIONS 8Be(α, α); E not given; 9Be(3He, α); E=3 MeV; calculated αα(θ). Asymptotic wave functions.
doi: 10.1016/0370-2693(71)90034-7
1970EL17 Acta Phys. 29, 127 (1970) Finite Range Coulomb Stripping in (t, p) and (He3, n) Reactions NUCLEAR REACTIONS 9Be(3He, n), E=2.1 MeV; 14N(t, p), E=1.83 MeV; calculated σ(θ).
doi: 10.1007/BF03155829
1970EL18 Acta Phys. 29, 143 (1970) Cluster Transfer Reactions at Low Energies NUCLEAR REACTIONS 90Zr(d, p), E=3 MeV; 27Al(3He, p), E=5 MeV; calculated σ(θ).
doi: 10.1007/BF03155830
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