NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = A.Lejeune Found 24 matches. 2002ZU02 Nucl.Phys. A706, 418 (2002) W.Zuo, A.Lejeune, U.Lombardo, J.F.Mathiot Interplay of Three-Body Interactions in the EOS of Nuclear Matter
doi: 10.1016/S0375-9474(02)00750-9
2002ZU03 Eur.Phys.J. A 14, 469 (2002) W.Zuo, A.Lejeune, U.Lombardo, J.F.Mathiot Microscopic three-body force for asymmetric nuclear matter
doi: 10.1140/epja/i2002-10031-y
2002ZU06 Prog.Theor.Phys.(Kyoto), Suppl. 146, 478 (2002) W.Zuo, A.Lejeune, U.Lombardo, J.F.Mathiot EOS of Neutron-Rich Matter with a Microscopic Three-Body Force
doi: 10.1143/PTPS.146.478
2000CU05 Phys.Rev. C62, 064308 (2000) J.Cugnon, A.Lejeune, H.-J.Schulze Hypernuclei in the Skyrme-Hartree-Fock Formalism with a Microscopic Hyperon-Nucleon Force NUCLEAR STRUCTURE 13C, 17O, 29Si, 41Ca, 91Zr, 141Ce, 209Pb; calculated Λ hypernucleus single-particle levels. 40Ca, 90Zr, 208Pb; calculated multi-Λ hypernuclei density profiles, radii, binding energies. Skyrme-Hartree-Fock model.
doi: 10.1103/PhysRevC.62.064308
2000LE12 Phys.Lett. 477B, 45 (2000) Nuclear Matter EOS with a Three-Body Force
doi: 10.1016/S0370-2693(00)00211-2
1998SC01 Phys.Rev. C57, 704 (1998) H.-J.Schulze, M.Baldo, U.Lombardo, J.Cugnon, A.Lejeune Hyperonic Nuclear Matter in Brueckner Theory
doi: 10.1103/PhysRevC.57.704
1997RI03 Nucl.Phys. A615, 1 (1997) J.Richert, D.Boose, A.Lejeune, P.Wagner Phase-Space Characteristics of Fragmenting Nuclei Described as Excited Disordered Systems
doi: 10.1016/S0375-9474(96)00468-X
1996SC10 Phys.Lett. 375B, 1 (1996) H.-J.Schulze, J.Cugnon, A.Lejeune, M.Baldo, U.Lombardo Medium Polarization Effects on Neutron Matter Superfluidity
doi: 10.1016/0370-2693(96)00213-4
1995SC41 Phys.Rev. C52, 2785 (1995) H.-J.Schulze, J.Cugnon, A.Lejeune, M.Baldo, U.Lombardo Status of the Brueckner-Hartree-Fock Approximation to the Nuclear Matter Binding Energy with the Paris Potential
doi: 10.1103/PhysRevC.52.2785
1995SC43 Phys.Lett. 355B, 21 (1995) H.-J.Schulze, A.Lejeune, J.Cugnon, M.Baldo, U.Lombardo Hypernuclear Matter in the Brueckner-Hartree-Fock Approximation
doi: 10.1016/0370-2693(95)00665-8
1988CU05 Nucl.Phys. A485, 271 (1988) Spin and Spin-Isospin Polarized Nuclear Matter NUCLEAR REACTIONS 59Co(n, n), E ≈ 0.3-31 MeV; 27Al(p, p), E=18 MeV; 59Co(p, p), E=47.5 MeV; 89Y, 87Rb(p, p), E=5 MeV; calculated model parameters. Optical model.
doi: 10.1016/0375-9474(88)90102-9
1982LA10 Phys.Rev. C25, 2278 (1982) Phenomenological and Microscopic Optical Model Analyses of the Interaction of Low-Energy Nucleons with 93Nb NUCLEAR REACTIONS 93Nb(n, n), E=7, 8.05, 11 MeV; 93Nb(p, p), E=22.2 MeV; 93Nb(p, n), E=18.7, 49.4 MeV; analyzed σ(total), σ(θ); deduced neutron, proton optical potential differences, Coulomb absorption term role. Phenomenological, microscopic optical model analyses.
doi: 10.1103/PhysRevC.25.2278
1982LE20 Nucl.Phys. A389, 141 (1982) A.Lejeune, C.Barbagallo, J.Richert Influence of Inertia Effects on the Transfer of Nucleons in Heavy Ion Collisions NUCLEAR REACTIONS 74Ge(32S, xnypzα), E=170 MeV; calculated nucleon transfer characteristics. Transport model.
doi: 10.1016/0375-9474(82)90295-0
1981LE08 Z.Phys. A299, 273 (1981) Exact Calculation of the Mass Distribution in the Collision Process of 32S on Medium-Weight Nuclei NUCLEAR REACTIONS 59Co, 65Cu(32S, X), E=160 MeV; 74Ge(32S, X), E=170 MeV; 89Y(32S, X), E=155 MeV; calculated fragment mass distribution functions. Fokker-Planck equation, exact integration.
doi: 10.1007/BF01443945
1980LE13 Z.Phys. A296, 359 (1980) Mass Transport Mechanism in the Collision of Sulphur on Medium-Weight Nuclei NUCLEAR REACTIONS 59Co, 65Cu(32S, X), E=160 MeV; 74Ge, 79Br, 85Rb(32S, X), E=170 MeV; 89Y(32S, X), E=153 MeV; calculated σ(θ, mass asymmetry); deduced reaction mechanism. Transport model.
doi: 10.1007/BF01438530
1978LE06 Nucl.Phys. A295, 301 (1978) Microscopic Optical Model Analyses of Proton and Neutron Elastic Scattering Cross Sections NUCLEAR REACTIONS 12C, 16O, 27Al, 40Ca, 56Fe, 58,60,62,64Ni, 63,65Cu, 68Zn, 90Zr, 116,120Sn, 208Pb, 209Bi(n, n), E=1-15 MeV; 12C, 16O, 27Al, 40Ca, 56Fe, 58,60,62,64Ni, 63,65Cu, 68Zn, 90Zr, 116,120Sn, 208Pb, 209Bi(p, p), E=10-70 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(78)90118-5
1977JE04 Phys.Rev. C16, 80 (1977) J.-P.Jeukenne, A.Lejeune, C.Mahaux Optical-Model Potential in Finite Nuclei from Reid's Hard Core Interaction NUCLEAR REACTIONS 12C, 16O, 27Al, 40Ca, 58Ni, 120Sn, 208Pb(p, p); calculated optical-model potentials.
doi: 10.1103/PhysRevC.16.80
1976JE01 Phys.Lett. 62B, 256 (1976) J.-P.Jeukenne, A.Lejeune, C.Mahaux Coulomb Correlation Due to the True Nonlocality of the Optical-Model Potential NUCLEAR REACTIONS 208Pb(n, n'), (p, p'); calculated Coulomb correction.
doi: 10.1016/0370-2693(76)90068-X
1975BE06 Can.J.Phys. 53, 203 (1975) M.Betz, J.P.Jeukenne, A.Lejeune Low Energy n-16O Elastic Scattering Phase Shifts Derived from the Sussex Interaction NUCLEAR REACTIONS 16O(n, n), E=low; calculated phase shifts.
doi: 10.1139/p75-030
1974JE03 Phys.Rev. C10, 1391 (1974) J.-P.Jeukenne, A.Lejeune, C.Mahaux Optical-Model Potential in Nuclear Matter from Reid's Hard Core Interaction NUCLEAR REACTIONS 40Ca, 58Ni(p, p); calculated scattering potential.
doi: 10.1103/PhysRevC.10.1391
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
1972JE01 Nucl.Phys. A183, 666 (1972) Truncation Effects in Elastic Scattering by a Nuclear Hartree-Fock Field NUCLEAR STRUCTURE 16O; calculated single-particle binding energies. Hartree-Fock theory. NUCLEAR REACTIONS 16O(n, n), E not given; calculated phase shifts. Hartree-Fock theory.
doi: 10.1016/0375-9474(72)90364-8
1972LE43 Phys.Lett. 42B, 171 (1972) Truncation Dependence of the 40Ca Hartree-Fock Field in the Continuum NUCLEAR REACTIONS 40Ca(n, n), E < 10 MeV; calculated phase shifts. Hartree-Fock field; finite harmonic oscillator basis, truncation effects.
doi: 10.1016/0370-2693(72)90052-4
1970LE02 Nucl.Phys. A141, 123 (1970) Comparison between Various Approximations of the Collision Matrix for the Reaction 6Li(p, p)6Li NUCLEAR REACTIONS 6Li(p, p), E=0.4-2.5 MeV; calculated σ(E). 7Be deduced resonance, level-width.
doi: 10.1016/0375-9474(70)90298-8
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