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NSR database version of April 11, 2024.

Search: Author = F.A.Brieva

Found 21 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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)

F.A.Brieva, W.G.Love

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
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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
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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
Citations: PlumX Metrics


1987BR21      Phys.Rev. C36, 899 (1987)

F.A.Brieva, A.Dellafiore

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
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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
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1980BR12      Nucl.Phys. A341, 377 (1980)

F.A.Brieva, R.G.Lovas

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
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1978BR06      Nucl.Phys. A297, 206 (1978)

F.A.Brieva, J.R.Rook

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
Citations: PlumX Metrics


1978BR22      Phys.Lett. 76B, 533 (1978)

F.A.Brieva

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
Citations: PlumX Metrics


1978BR28      Nucl.Phys. A307, 493 (1978)

F.A.Brieva, J.R.Rook

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
Citations: PlumX Metrics


1978BR29      Nucl.Phys. A308, 27 (1978)

F.A.Brieva, B.Z.Georgiev

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
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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
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1977BR36      Nucl.Phys. A291, 317 (1977)

F.A.Brieva, J.R.Rook

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
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1977BR37      Nucl.Phys. A292, 445 (1977)

F.A.Brieva, A.Dellafiore

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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