NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = A.M.Kobos Found 24 matches. 1989RA03 Phys.Lett. 218B, 403 (1989) J.Raynal, H.S.Sherif, A.M.Kobos, E.D.Cooper, J.I.Johansson Dirac Coupled Channel Calculations and Nucleon Scattering at Large Momentum Transfer NUCLEAR REACTIONS 40Ca(polarized p, p), E=800 MeV; calculated σ(θ), analyzing power vs θ. Dirac coupled-channels method.
doi: 10.1016/0370-2693(89)91435-4
1988HA11 Nucl.Phys. A480, 1 (1988); Adendum Nucl.Phys. A486, 687 (1988) The Use of Off-Shell Potentials in Brueckner Theory Calculations of the Nucleon Optical Potential NUCLEAR REACTIONS 40Ca(p, p), (polarized p, p), E=30.3 MeV; 208Pb(p, p), (polarized p, p), E=160, 182, 200 MeV; calculated σ(θ), polarization vs θ; deduced potential parameters. Brueckner theory, off-shell potentials.
doi: 10.1016/0375-9474(88)90380-6
1988KO27 Nucl.Phys. A487, 457 (1988) A.M.Kobos, M.E.Brandan, G.R.Satchler Further Optical Model Studies of 16O Scattering at E/A = 94 MeV NUCLEAR REACTIONS 12C(16O, 16O), E=94 MeV/nucleon; 28Si(16O, 16O), E=1.47 GeV; analyzed data; deduced model parameters. Optical model.
doi: 10.1016/0375-9474(88)90624-0
1985HO03 Nucl.Sci.Eng. 89, 111 (1985) The Inelastic Scattering of Neutrons by 238U NUCLEAR REACTIONS 238U(n, n'), E=0.2-5 MeV; analyzed σ(E); deduced direct, compound nuclear contributions. Distorted wave approach, approximate treatment of channel coupling.
doi: 10.13182/NSE85-A18185
1985KO05 Nucl.Phys. A435, 677 (1985) A.M.Kobos, E.D.Cooper, J.R.Rook, W.Haider Proton Scattering from 4He at 500 MeV NUCLEAR REACTIONS 4He(polarized p, p), E=500 MeV; calculated σ(θ), analyzing power, Wolfenstein parameter, spin rotation function vs θ. First-order Brueckner, Dirac equation analyses.
doi: 10.1016/0375-9474(85)90181-2
1985KO37 Nucl.Phys. A445, 605 (1985) A.M.Kobos, E.D.Cooper, J.I.Johansson, H.S.Sherif Phenomenological Study of Relativistic Optical Model Potentials in Proton Elastic Scattering NUCLEAR REACTIONS 4He, 16O, 40Ca, 90Zr, 208Pb(polarized p, p), E=160-800 MeV; calculated σ(θ), analyzing power vs θ. Relativistic optical model.
doi: 10.1016/0375-9474(85)90562-7
1984KO07 Nucl.Phys. A417, 256 (1984) Validity of Brueckner Theory for the Nucleon Optical Potential near 200 MeV NUCLEAR REACTIONS 40Ca(p, p), E=182 MeV; 208Pb(p, p), E=185 MeV; 12C(p, p), E=200 MeV; calculated σ(θ). Brueckner theory optical potentials.
doi: 10.1016/0375-9474(84)90507-4
1984KO15 Phys.Rev. C30, 403 (1984) Potential Models and Resonances in the 16O + 28Si System NUCLEAR REACTIONS 28Si(16O, 16O), E=29.4-45 MeV; analyzed σ(E, θ); deduced optical model potential, phase shifts, no resonances.
doi: 10.1103/PhysRevC.30.403
1984KO20 Nucl.Phys. A425, 205 (1984) A.M.Kobos, B.A.Brown, R.Lindsay, G.R.Satchler Folding-Model Analysis of Elastic and Inelastic α-Particle Scattering using a Density-Dependent Force NUCLEAR REACTIONS 40Ca(α, α), E=29, 100 MeV; 90Zr(α, α), E=40, 59.1, 79.5, 99.5, 118 MeV; 208Pb(α, α'), E=25, 139 MeV; 58Ni(α, α'), E=139 MeV; 46,48,50Ti(α, α'), E=140 MeV; calculated σ(θ). Folding model analysis.
doi: 10.1016/0375-9474(84)90073-3
1984KO23 Nucl.Phys. A426, 92 (1984) Explicit Treatment of Internucleon P- and D-States in the Calculation of the Nucleon Optical Potential NUCLEAR REACTIONS 40Ca(p, p), E=30.3, 182 MeV; calculated σ(θ), potential parameters. Brueckner t-matrix, internucleon P-, D-states inclusion.
doi: 10.1016/0375-9474(84)90066-6
1984KO30 Nucl.Phys. A427, 589 (1984) A Global Optical Potential Analysis of 16O + 28Si Elastic Scattering NUCLEAR REACTIONS 28Si(16O, 16O), E(cm)=18-35 MeV; calculated σ(θ), σ(E); deduced potential parameters, scattering amplitude components. Global optical model.
doi: 10.1016/0375-9474(84)90232-X
1983KO06 Nucl.Phys. A395, 248 (1983) A.M.Kobos, G.R.Satchler, R.S.Mackintosh An Optical Potential Description of 16O + 28Si Elastic Scattering NUCLEAR REACTIONS 28Si(16O, 16O), E(cm)=21.1-34.8 MeV; analyzed σ(θ); deduced optical model, potential parameters. Double folded potential, model independent correction term.
doi: 10.1016/0375-9474(83)90099-4
1982KO19 Nucl.Phys. A384, 65 (1982) A.M.Kobos, B.A.Brown, P.E.Hodgson, G.R.Satchler, A.Budzanowski Folding Model Analysis of α-Particle Elastic Scattering with a Semirealistic Density-Dependent Effective Interaction NUCLEAR REACTIONS 40Ca, 46,48,50Ti, 58Ni, 90Zr, 208Pb(α, α), E=140 MeV; 58,60,62,64Ni(α, α), E=172 MeV: analyzed σ(θ). Folding model, density-dependent effective interaction.
doi: 10.1016/0375-9474(82)90305-0
1982KO23 Nucl.Phys. A389, 205 (1982) A.M.Kobos, R.S.Mackintosh, J.R.Rook Uncertainty in the Nucleon-Nucleus Optical Potential NUCLEAR REACTIONS 16O(p, p), (polarized p, p), E=30 MeV; calculated S-matrix element vs (L), Wolfenstein R-parameter; deduced nucleon-nucleus optical potential features. Phase shift analysis.
doi: 10.1016/0375-9474(82)90516-4
1982KO25 Phys.Rev. C26, 1766 (1982) Evaluation of Model-Independent Optical Potentials for the 16O + 40Ca System NUCLEAR REACTIONS 40Ca(16O, 16O), E(cm)=35.7 MeV; analyzed data; deduced potentials. Optical, full, restricted spline model analyses.
doi: 10.1103/PhysRevC.26.1766
1982MA35 Phys.Lett. 116B, 95 (1982) Potential Model Representation of 6Li Break-Up through a Simple Inversion Procedure NUCLEAR REACTIONS 12C(6Li, 6Li), E=156 MeV; calculated projectile breakup effects; deduced adiabatic breakup local potential equivalent. Inversion method, iterative perturbation approach.
doi: 10.1016/0370-2693(82)90983-2
1980MA19 Phys.Lett. 92B, 59 (1980) Application of Model Independent Analyses to the Evaluation of M3Y Heavy Ion Folding Model NUCLEAR REACTIONS 40Ca, 24Mg(6Li, 6Li), E=88 MeV; 40Ca(6Li, 6Li), E=30 MeV; 28Si(16O, 16O), E=55 MeV; analyzed data. Model independent spline interpolation method.
doi: 10.1016/0370-2693(80)90303-2
1980PA17 Nucl.Phys. A348, 45 (1980) Adiabatic Approximation for Alpha-Nucleus Scattering NUCLEAR REACTIONS 90Zr(α, α), E=59.1, 79.5 MeV; calculated σ(θ); deduced real part of α-nucleus potential. Adiabatic approximation, Woods-Saxon form factors.
doi: 10.1016/0375-9474(80)90544-8
1979KO01 J.Phys.(London) G5, 97 (1979) The Phenomenology of Proton Elastic Scattering and Evidence for Angular-Momentum-Dependent Optical-Model Potentials NUCLEAR REACTIONS 16O(p, p), E=23-52 MeV; 40Ca(p, p), E=17-48 MeV; 58Ni(p, p), E=40, 100 MeV; 56Fe(p, p), E=30.3 MeV; calculated σ(θ), A(θ). L-dependent optical model.
doi: 10.1088/0305-4616/5/1/012
1978MA25 J.Phys.(London) G4, L135 (1978) Evidence for an Imaginary Spin-Orbit Term in the Proton Optical Potential NUCLEAR STRUCTURE 40Ca, 16O; calculated proton optical potential parameter.
doi: 10.1088/0305-4616/4/6/006
1978WA05 Phys.Rev. C17, 1315 (1978) N.S.Wall, A.A.Cowley, R.C.Johnson, A.M.Kobos Modified Optical Potential for the Elastic Scattering of Complex Particles NUCLEAR REACTIONS 40Ca, 58Ni, 90Zr(3He, 3He), (α, α); calculated modified optical potential.
doi: 10.1103/PhysRevC.17.1315
1977KO22 Acta Phys.Pol. B8, 887 (1977) The Contribution of Pickup Channels to the Helion Optical Potential NUCLEAR REACTIONS 58Ni(3He, 3He), (3He, α), E=37.7, 51.3 MeV; calculated σ(θ).
1976MA29 Phys.Lett. 62B, 127 (1976) The Real and Imaginary Proton Optical Potentials: The Importance of Deuteron Channels NUCLEAR REACTIONS 40Ca(p, p), E=30 MeV; calculated potential with deuteron channel, σ(θ).
doi: 10.1016/0370-2693(76)90484-6
1975PE03 Nucl.Phys. A245, 343 (1975) D.G.Perkin, A.M.Kobos, J.R.Rook Real Part of the Optical Potential for Composite Particles NUCLEAR REACTIONS 148Sm(α, α), E=30 MeV; 90Zr(α, α), E=40, 59.1, 79.5, 99.5 MeV; calculated potentials.
doi: 10.1016/0375-9474(75)90182-7
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