NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = R.Sartor Found 36 matches. 2006SA08 Phys.Rev. C 73, 034307 (2006) Solution to the Bethe-Faddeev equation within the continuous version of the hole-line expansion
doi: 10.1103/PhysRevC.73.034307
2003SA55 Phys.Rev. C 68, 057301 (2003) Solution of the Bethe-Faddeev equation by direct matrix inversion
doi: 10.1103/PhysRevC.68.057301
2001SA62 Phys.Rev. C64, 054303 (2001) Diagrammatic Analysis of the Hellmann-Feynman Theorem: Numerical applications
doi: 10.1103/PhysRevC.64.054303
2000SA43 Phys.Rev. C62, 044318 (2000) Diagrammatic Analysis of the Hellmann-Feynman Theorem
doi: 10.1103/PhysRevC.62.044318
1997SA31 Phys.Rev. C56, 942 (1997) Enumeration Method for the Hole Line Expansion Diagrams
doi: 10.1103/PhysRevC.56.942
1996SA17 Phys.Rev. C54, 809 (1996) Solution of the Bethe-Goldstone Equation with an Exact Propagator
doi: 10.1103/PhysRevC.54.809
1994MA07 Nucl.Phys. A568, 1 (1994) Critical Study of the Dispersive n-90Zr Mean Field by Means of a New Variational Method NUCLEAR REACTIONS 90Zr(n, n), E=8-24 MeV; calculated σ(θ). Mean field, optical model approaches.
doi: 10.1016/0375-9474(94)90002-7
1992MA43 Nucl.Phys. A546, 65c (1992) Embedding of Correlations in the Nuclear Mean Field NUCLEAR REACTIONS 208Pb(e, e'p), E not given; calculated spectral function. Complex mean field.
doi: 10.1016/0375-9474(92)90502-B
1991JE02 Phys.Rev. C43, 2211 (1991) J.-P.Jeukenne, C.Mahaux, R.Sartor Dependence of the Fermi Energy Upon Neutron Excess NUCLEAR STRUCTURE A=40-208; calculated symmetry potential strength near Fermi energy. Dispersion relation related analysis input.
doi: 10.1103/PhysRevC.43.2211
1991MA15 Nucl.Phys. A528, 253 (1991) Dispersion Relation Approach to the Mean Field and Spectral Functions of Nucleons in 40Ca NUCLEAR REACTIONS 40Ca(n, n), (p, p), E=30-50 MeV; calculated potential radius parameters vs E. 40Ca(polarized p, p), E=19.6-48 MeV; 40Ca(polarized n, n), E=5-40 MeV; calculated σ(θ), analyzing power vs θ. Dispersion relation approach to mean field.
doi: 10.1016/0375-9474(91)90090-S
1990MA60 Nucl.Phys. A516, 285 (1990) Dispersive Versus Constant-Geometry Models of the Neutron-208Pb Mean Field NUCLEAR REACTIONS 208Pb(n, n), E ≈ 0-16 MeV; calculated σ(E). Mean field approach.
doi: 10.1016/0375-9474(90)90310-I
1989MA20 Nucl.Phys. A493, 157 (1989) From Scattering to Very Deeply Bound Neutrons in 208Pb: Extended and improved moment approaches NUCLEAR REACTIONS 208Pb(n, n), E=10-40 MeV; calculated σ(θ). Complex mean field.
doi: 10.1016/0375-9474(89)90395-3
1989MA48 Nucl.Phys. A503, 525 (1989) Variational Moment Approach to the Single-Particle Properties of Protons in 208Pb NUCLEAR STRUCTURE 208Pb; calculated proton single particle state properties, transfer reaction spectroscopic strengths. Variational moment approach.
doi: 10.1016/0375-9474(89)90248-0
1988MA21 Nucl.Phys. A481, 381 (1988) Single-Particle Potential and Quasiparticle Properties of Protons in 208Pb NUCLEAR REACTIONS 208Pb(p, p), E=-20-40 MeV; calculated potential features, proton quasiparticle strength. Mean field approach.
doi: 10.1016/0375-9474(88)90335-1
1988MA22 Nucl.Phys. A481, 407 (1988) Isovector, Isoscalar and Coulomb Contributions to the Mean Field in 208Pb NUCLEAR REACTIONS 208Pb(p, p), (n, n), E=-20-40 MeV; calculated potential features, differences; deduced isovector, isoscalar and Coulomb contributions. Mean field methods.
doi: 10.1016/0375-9474(88)90336-3
1988MA40 Nucl.Phys. A484, 205 (1988) The p-40Ca and n-40Ca Mean Fields from the Iterative Moment Approach NUCLEAR REACTIONS 40Ca(p, p), (n, n), E=-25-75 MeV; calculated mean field parameters. Iterative moment technique.
doi: 10.1016/0375-9474(88)90071-1
1987MA28 Nucl.Phys. A468, 193 (1987) Extrapolation from Positive to Negative Energy of the Woods-Saxon Parametrization of the n-208Pb Mean Field NUCLEAR STRUCTURE 209Pb; calculated neutron single particle energies. Mean field techniques. NUCLEAR REACTIONS 208Pb(n, X), E=20-40 MeV; calculated optical model parameters, radial moment, moment ratios. Mean field techniques.
doi: 10.1016/0375-9474(87)90515-X
1987MA53 Phys.Rev. C36, 1777 (1987) Fermi-Surface Anomaly for Neutrons in Yttrium NUCLEAR REACTIONS 89Y(n, n), E not given; calculated n-nucleus interaction potential features. Dispersion relation approach.
doi: 10.1103/PhysRevC.36.1777
1987MA60 Nucl.Phys. A475, 247 (1987) Properties of the Quasiparticle Excitations in 207Pb and 209Pb from an Extrapolation of the Optical-Model Potential NUCLEAR STRUCTURE 209,207Pb; calculated quasiparticle excitation characteristics. 208Pb; calculated neutron density distribution.
doi: 10.1016/0375-9474(87)90165-5
1986MA11 Nucl.Phys. A451, 441 (1986) Energy Dependence of the Global Properties of the Empirical Nucleon-Nucleus Potential for 40Ca, 132Sn and 208Pb NUCLEAR REACTIONS 40Ca, 208Pb(p, p), (n, n), E not given; calculated nucleon-nucleus potential global properties energy dependence. NUCLEAR STRUCTURE 40Ca, 132Sn, 208Pb; calculated proton rms radii.
doi: 10.1016/0375-9474(86)90069-2
1986MA53 Nucl.Phys. A458, 25 (1986) Empirical and Theoretical Investigation of the Average Potential of Nucleons in 40Ca and 208Pb NUCLEAR REACTIONS 40Ca, 208Pb(p, p), (n, n), E not given; calculated complex mean field radial moments; deduced average potential. Optical model, dispersion relation approach.
doi: 10.1016/0375-9474(86)90281-2
1986MA60 Phys.Rev.Lett. 57, 3015 (1986) Calculation of the Shell-Model Potential from the Optical-Model Potential NUCLEAR REACTIONS 208Pb(n, n), E=20-40 MeV; calculated shell model potential parameters energy dependence. Dispersion relation approach, optical model base.
doi: 10.1103/PhysRevLett.57.3015
1986MA61 Phys.Rev. C34, 2119 (1986) Empirical Evidence of an Energy Dependence of the Radial Shape of the Real Part of the Optical Potential NUCLEAR REACTIONS 40Ca(p, p), 208Pb(p, p), (p, n), E ≈ 10-40 MeV; analyzed potential parameter fits to data; deduced potential shape radial dependence.
doi: 10.1103/PhysRevC.34.2119
1986MA69 Nucl.Phys. A460, 466 (1986); Erratum Nucl.Phys. A472, 769 (1987) Dispersion Relation Approach to the Extrapolation towards Negative Energy of the Optical Potential in 40Ca and 208Pb NUCLEAR REACTIONS 40Ca(p, p), E=9-20 MeV; 40Ca(n, n), E=9-14 MeV; 208Pb(n, n), E=4-40 MeV; 208Pb(p, p), E=15-30 MeV; calculated optical model real part radial moments. Dispersion relation approach.
doi: 10.1016/0375-9474(86)90425-2
1984LA04 Nucl.Phys. A414, 309 (1984) G.La Rana, C.Ngo, A.Faessler, L.Rikus, R.Sartor, M.Barranco, X.Vinas Heavy-Ion Optical Potentials at Finite Temperature Calculated using a Complex Effective Interaction Derived from a Realistic Force NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E=400, 800 MeV; 208Pb(40Ca, 40Ca), E=1 GeV; calculated optical potential parameters vs separation distance, temperature. Double folding method.
doi: 10.1016/0375-9474(84)90647-X
1984SA08 Phys.Rev. C29, 1756 (1984) Density Matrix Approach to the Complex Heavy Ion Optical Potential: Exchange part NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated optical potential parameter dependence. Density matrix approach.
doi: 10.1103/PhysRevC.29.1756
1983SA14 Nucl.Phys. A404, 392 (1983) Unified Skyrme Approach to the Real and Imaginary Parts of the Heavy-Ion Optical Potential NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 208Pb; calculated binding energies, charge radii. Hartree-Fock method, Skyrme interaction. NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated optical potential real, imaginary parts vs separation distance. Skyrme approach.
doi: 10.1016/0375-9474(83)90555-9
1983SA36 Phys.Rev. C28, 2533 (1983) Complex Heavy Ion Optical Potential and the Proximity Concept NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated optical potential components vs ion-ion separation distance. Proximity approximation.
doi: 10.1103/PhysRevC.28.2533
1982SA20 Phys.Rev. C26, 1025 (1982) Density Matrix Approach to the Complex Heavy Ion Optical Potential NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated optical potential characteristics. Density matrix expansion, complex effective interaction.
doi: 10.1103/PhysRevC.26.1025
1981KH03 Nucl.Phys. A369, 495 (1981) S.B.Khadkikar, L.Rikus, A.Faessler, R.Sartor Surface and Volume Contributions to Real and Imaginary Parts of the Heavy-Ion Optical Potential NUCLEAR REACTIONS 16O(16O, 16O), E=80, 332 MeV; calculated σ(θ). Feshbach projection technique, heavy-ion optical potential.
doi: 10.1016/0375-9474(81)90034-8
1981SA12 Nucl.Phys. A359, 467 (1981) R.Sartor, A.Faessler, S.B.Khadkikar, S.Krewald Folding Computation of the 16O + 16O Optical Potential with a Complex Effective Force NUCLEAR REACTIONS 16O(16O, 16O), E=0, 83, 332 MeV; calculated real, imaginary optical potential terms. Folding method, complex effective force.
doi: 10.1016/0375-9474(81)90250-5
1981SA33 Phys.Rev. C24, 2347 (1981) The Nucleus-Nucleus Optical Potential Derived from a Complex Skyrme-Type Interaction NUCLEAR REACTIONS 16O(16O, 16O), E=83, 322 MeV; calculated nucleus-nucleus optical potential. Complex energy function, Skyrme-type interaction.
doi: 10.1103/PhysRevC.24.2347
1980CU07 Phys.Rev. C21, 2342 (1980) Factorization in High-Energy Nucleus-Nucleus Fragmentation Cross Sections NUCLEAR REACTIONS 63Cu(27Al, X), (107Ag, X), E=relativistic; calculated fragmentation probability function. Abrasion-ablation model.
doi: 10.1103/PhysRevC.21.2342
1978SA19 Phys.Rev. C18, 1035 (1978) Energy of the First 3/2- Excited State of 7Li NUCLEAR REACTIONS 6Li(n, t), E ≤ 3.9 MeV; analyzed σ, integral σ. 7Li deduced levels.
doi: 10.1103/PhysRevC.18.1035
1976SA16 Nucl.Phys. A267, 29 (1976) A Computation of the Optical Potential in Nuclear Matter from a Separable Nucleon-Nucleon Interaction NUCLEAR STRUCTURE 8Be, 12C, 16O, 27Al; calculated 1s hole state widths.
doi: 10.1016/0375-9474(76)90641-2
1974LE30 J.Phys.(Paris) 35, 895 (1974) Analysis of the 6Li(n, t)α Reaction over the Energy Range 14 to 3900 keV NUCLEAR REACTIONS 6Li(n, t), E=14-3900 keV; analyzed data, calculated σ(E, Et). 7Li deduced resonances, level-width.
doi: 10.1051/jphys:019740035012089500
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