NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = F.Brieva Found 22 matches. 1996AR13 Phys.Rev. C54, 2570 (1996) H.F.Arellano, F.A.Brieva, M.Sander, H.V.von Geramb Sensitivity of Nucleon-Nucleus Scattering to the Off-Shell Behavior of On-Shell Equivalent NN Potentials NUCLEAR REACTIONS 40Ca(p, p), (polarized p, p), E=40-500 MeV; 208Pb(polarized p, p), (p, p), E=400 MeV; analyzed σ(θ), analyzing power vs θ; deduced sensitivity to off-shell behavior of on-shell equivalent. NN-potentials.
doi: 10.1103/PhysRevC.54.2570
1995AR13 Phys.Rev. C52, 301 (1995) H.F.Arellano, F.A.Brieva, W.G.Love In-Medium Full-Folding Optical Model for Nucleon-Nucleus Elastic Scattering NUCLEAR REACTIONS 208Pb, 40Ca(polarized p, p), E=30.3-400 MeV; analyzed σ(θ), analyzing power, spin-rotation function vs θ. 40Ca, 90Zr, 208Pb(n, n), E=4-500 MeV; calculated σ(E). In-medium, full-folding optical model.
doi: 10.1103/PhysRevC.52.301
1994AR17 Phys.Rev. C50, 2480 (1994) H.F.Arellano, F.A.Brieva, W.G.Love Deuteron Effects in Nucleon-Nucleus Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=160-400 MeV; 208Pb(polarized p, p), E=98-400 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ; deduced medium effects, higher order corrections role. Full folding model.
doi: 10.1103/PhysRevC.50.2480
1993HI01 Phys.Rev. C47, 260 (1993) K.H.Hicks, W.P.Alford, A.Celler, R.S.Henderson, K.P.Jackson, C.A.Miller, M.C.Vetterli, S.Yen, F.Brieva, C.J.Horowitz, J.Piekarewicz Comparison of the Quasifree Charge-Exchange Reaction for 12C and 54Fe NUCLEAR REACTIONS 12C, 54Fe(polarized p, n), E=290, 420 MeV; measured σ(θ), analyzing power A(y)(θ); deduced medium modification of the nucleon-nucleon isovector force.
doi: 10.1103/PhysRevC.47.260
1991AR03 Phys.Rev. C43, 1875 (1991) H.F.Arellano, F.A.Brieva, W.G.Love, K.Nakayama Comparison of Nucleon-Nucleon Potential Models in a Full-Folding Description of Elastic Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 300, 400 MeV; analyzed σ(θ), polarization observables data; deduced effective nucleon-nucleon potential dependence. Nonrelativistic full-folding model analysis.
doi: 10.1103/PhysRevC.43.1875
1991AR11 Phys.Rev. C43, 2734 (1991) H.F.Arellano, W.G.Love, F.A.Brieva Starting Energy Dependence of Elastic Scattering Observables in a Full-Folding Model NUCLEAR REACTIONS 16O(polarized p, p), E=135 MeV; 40Ca(polarized p, p), E=200, 300 MeV; calculated σ(θ), polarization observables; deduced starting energy dependence.
doi: 10.1103/PhysRevC.43.2734
1990AR03 Phys.Rev. C41, 2188 (1990); Erratum Phys.Rev. C42, 1782 (1990) H.F.Arellano, F.A.Brieva, W.G.Love Nonrelativistic Full-Folding Model of Nucleon Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=400, 200 MeV; calculated σ(θ), analyzing power, spin-rotation parameter vs momentum transfer. Nonrelativistic full-folding optical potentials.
doi: 10.1103/PhysRevC.41.2188
1990AR11 Phys.Rev. C42, 652 (1990) H.F.Arellano, F.A.Brieva, W.G.Love Role of Nuclear Densities in Nucleon Elastic Scattering NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 400 MeV; 16O(polarized p, p), E=200 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ; deduced scattering observables sensitivity to density. Full-folding model.
doi: 10.1103/PhysRevC.42.652
1990AR31 J.Phys.(Paris), Colloq.C-6, 603 (1990) H.F.Arellano, W.E.Love, K.Nakayama, F.A.Brieva Off-Shell Effects of Nucleon-Nucleon Potential Models on Proton-Nucleus Elastic Scattering Observables NUCLEAR REACTIONS 40Ca(polarized p, p), E=200 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ.
1990BR22 Phys.Rev. C42, 2573 (1990) Nonlocal Couplings, Off-Shell Effects, and the Nuclear Response NUCLEAR REACTIONS 40Ca(polarized p, p'), E=100, 300 MeV; calculated inclusive σ, spin-flip probabilities, analyzing powers, σ(θp, Ep'); deduced nonlocal couplings, off-shell effects role. Interacting Fermi gas model.
doi: 10.1103/PhysRevC.42.2573
1989AR05 Phys.Rev.Lett. 63, 605 (1989) H.F.Arellano, F.A.Brieva, W.G.Love Full-Folding-Model Description of Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 40Ca(polarized p, p), E=200, 300 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ. Full folding model analysis.
doi: 10.1103/PhysRevLett.63.605
1988AM01 Phys.Rev. C37, 934 (1988) K.Amos, L.Berge, F.A.Brieva, A.Katsogiannis, L.Petris, L.Rikus Off-Shell Properties of the Two-Nucleon t Matrix NUCLEAR STRUCTURE 2H; calculated binding energy.
doi: 10.1103/PhysRevC.37.934
1987BR21 Phys.Rev. C36, 899 (1987) Random Phase Approximation Effects in the Longitudinal Response Function of 12C NUCLEAR REACTIONS 12C(e, e'), E not given; calculated longitudinal response function. 12C(γ, X), E ≤ 40 MeV; calculated photoabsorption σ(E). RPA.
doi: 10.1103/PhysRevC.36.899
1985DE20 Phys.Rev. C31, 1088 (1985) A.Dellafiore, F.Lenz, F.A.Brieva Particle-Hole Calculation of the Longitudinal Response Function of 12C NUCLEAR REACTIONS 40Ca, 12C(e, e'), E not given; calculated longitunal response functions, form factors. 4He(e, e'), E not given; calculated intrinsic response function; deduced quasielastic region many-body effects.
doi: 10.1103/PhysRevC.31.1088
1980BR12 Nucl.Phys. A341, 377 (1980) Lane Model on Microscopic Grounds NUCLEAR REACTIONS 48Ca, 90Zr, 208Pb(p, n), E=25, 35, 45 MeV; calculated σ(θ); deduced microscopic Lane potential. Energy, density dependent complex effective interactions.
doi: 10.1016/0375-9474(80)90371-1
1978BR06 Nucl.Phys. A297, 206 (1978) Nucleon-Nucleus Optical Model Potential (III). The Spin-Orbit Component NUCLEAR REACTIONS 40Ca(p, p), E=30.3 MeV; calculated potential, polarization.
doi: 10.1016/0375-9474(78)90272-5
1978BR22 Phys.Lett. 76B, 533 (1978) Exchange Term and Effect of Odd Forces in the Nucleon-Nucleus Optical Potential NUCLEAR REACTIONS 208Pb(p, p); calculated optical potential parameters.
doi: 10.1016/0370-2693(78)90847-X
1978BR28 Nucl.Phys. A307, 493 (1978) Microscopic Description of Nucleon-Nucleus Elastic Scattering NUCLEAR REACTIONS 40Ca(n, n), E=7.91, 11, 20, 26 MeV; 16O(p, p), E=23-53 MeV; 40Ca(p, p), E=15-76 MeV; 208Pb(p, p), E=16-100 MeV; calculated σ(E, θ).
doi: 10.1016/0375-9474(78)90461-X
1978BR29 Nucl.Phys. A308, 27 (1978) Inelastic Nucleon Scattering from Deformed Nuclei NUCLEAR REACTIONS 152,154Sm(n, n'), E=7 MeV; 154Sm(p, p'), E=50.8 MeV; 152Sm(p, p'), E=35, 50.8 MeV; 238U(p, p'), E=35 MeV; 20Ne(p, p'), E=24.5 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(78)90438-4
1978BR30 Phys.Lett. 79B, 177 (1978) F.A.Brieva, H.V.Geramb, J.R.Rook A Realistic Complex Interaction for Elastic and Inelastic Nucleon Scattering NUCLEAR REACTIONS 27Al(p, n), E=40 MeV; calculated σ(θ) for 27Si ground state; 40Ca(p, p'), E=30, 35.8, 40 MeV; calculated σ(θ) for 3.74-MeV (3-) state in 40Ca. Complex nuclear t-matrix interaction.
doi: 10.1016/0370-2693(78)90216-2
1977BR36 Nucl.Phys. A291, 317 (1977) Nucleon-Nucleus Optical Model Potential (II). Finite Nuclei NUCLEAR REACTIONS 40Ca(p, p), E=30.3, 40 MeV; 40Ca(n, n), E=7.91 MeV; 208Pb(p, p), E=30.3, 40, 100.4 MeV; calculated σ.
doi: 10.1016/0375-9474(77)90323-2
1977BR37 Nucl.Phys. A292, 445 (1977) Quasielastic Electron Scattering from Nuclei NUCLEAR REACTIONS 6Li, 12C, 24Mg, 40Ca, 59Ni, 89Y, 119Sn, 181Ta, 208Pb(e, e'), E=500 MeV; calculated σ, quasielastic σ.
doi: 10.1016/0375-9474(77)90629-7
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