NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = E.Suraud Found 31 matches. 2009ME13 Phys.Rev. C 80, 054314 (2009) Density functional theory and Kohn-Sham scheme for self-bound systems
doi: 10.1103/PhysRevC.80.054314
2008DI08 Int.J.Mod.Phys. E17, 120 (2008) P.M.Dinh, P.G.Reinhard, E.Suraud Time-resolved fission of metal clusters and nuclei
doi: 10.1142/S0218301308009616
2006NA36 Eur.Phys.J. A 30, 333 (2006) J.Navarro, P.-G.Reinhard, E.Suraud Small fermionic systems: The common methods and challenges
doi: 10.1140/epja/i2006-10127-4
2006SU19 Int.J.Mod.Phys. E15, 1549 (2006) Metal clusters and nuclei
doi: 10.1142/S021830130600523X
2001ZH10 Nucl.Phys. A684, 655c (2001) F.-S.Zhang, F.Wang, E.Suraud, F.Spiegelmann Temperature Dependence of the Vibrational Properties of Sodium Microclusters
doi: 10.1016/S0375-9474(01)00514-0
1998GE10 Phys.Lett. 437B, 19 (1998) M.Germain, Ch.Hartnack, J.L.Laville, J.Aichelin, M.Belkacem, E.Suraud Beyond Mean Field Confrontation of Different Models with High Transverse Momentum Proton Spectra NUCLEAR REACTIONS Ta(Ar, X), E=92 MeV/nucleon; analyzed proton spectra; deduced no collective effects.
doi: 10.1016/S0370-2693(98)00943-5
1997CA64 Nuovo Cim. 110A, 1175 (1997) F.Calvayrac, S.El-Gammal, C.Kohl, P.-G.Reinhard, E.Suraud Nonlinear Dynamics of Nuclei and Metal Clusters
doi: 10.1007/BF03035961
1996AB40 Phys.Rep. 275, 49 (1996) Y.Abe, S.Ayik, P.-G.Reinhard, E.Suraud On Stochastic Approaches of Nuclear Dynamics
doi: 10.1016/0370-1573(96)00003-8
1996BE09 Phys.Rev. C53, 1440 (1996) G.F.Bertsch, P.-G.Reinhard, E.Suraud Particle Evaporation from Semiclassical Dynamics NUCLEAR STRUCTURE A=64; calculated particle evaporation related features. BUU equation.
doi: 10.1103/PhysRevC.53.1440
1996RE17 Z.Phys. A355, 339 (1996) Towards a Fermionic Vlasov Equation
doi: 10.1007/s002180050118
1996SU22 Ann.Phys.(Paris) 21, 461 (1996) On Kinetic Equations in Heavy-Ion Physics
1995RE22 Ann.Phys.(New York) 239, 216 (1995) On Dissipative Features of the Vlasov Equation. II. Analysis of a Dissipative Pattern
doi: 10.1006/aphy.1995.1033
1995ZH14 Phys.Rev. C51, 3201 (1995) Analysis of Multifragmentation in a Boltzmann-Langevin Approach NUCLEAR REACTIONS 40Ca(40Ca, X), E=20-90 MeV/nucleon; calculated intermediate mass fragments, multiplicity distributions; deduced dynamical fluctuations energy dependence. Boltzmann-Langevin equation coupled to the coalescence model.
doi: 10.1103/PhysRevC.51.3201
1994BO37 Z.Phys. A349, 119 (1994) D.Boilley, Y.Abe, S.Ayik, E.Suraud A Bohr-Mottelson Model of Nuclei at Finite Temperature
doi: 10.1007/BF01291169
1994SU26 Nucl.Phys. A580, 323 (1994) E.Suraud, S.Ayik, M.Belkacem, F.-S.Zhang On Transient Effects in Violent Nuclear Collisions NUCLEAR REACTIONS 12C(12C, X), E=60 MeV/nucleon; calculated ensemble averaged quadrupole moment time evolution, other properties; deduced transient behavior role in particle production σ below threshold. Boltzmann-Langevin model.
doi: 10.1016/0375-9474(94)90777-3
1993BE01 Phys.Rev. C47, R16 (1993) K+ Production Far Below the Free Nucleon-Nucleon Threshold in Heavy-Ion Collisions NUCLEAR REACTIONS 12C(12C, K+X), E > 200 MeV/nucleon; 42Ca(42Ca, K+X), E=90 MeV/nucleon; calculated inclusive K+ production σ. Boltzmann and Boltzmann-Langevin equations simulations.
doi: 10.1103/PhysRevC.47.R16
1993BO19 Nucl.Phys. A556, 67 (1993) D.Boilley, E.Suraud, Y.Abe, S.Ayik Nuclear Fission with a Langevin Equation NUCLEAR REACTIONS 205At, 248Cf(n, F), E=thermal; calculated fission rate vs temperature, time. Langevin equation.
doi: 10.1016/0375-9474(93)90238-S
1993ZH29 Phys.Lett. 319B, 35 (1993) Boltzmann-Langevin Equation, Dynamical Instability, and Multifragmentation NUCLEAR REACTIONS 40Ca(40Ca, X), E=90 MeV/nucleon; calculated intermediate mass fragment, charged particle multiplicities. Boltzmann-Langevin equation, dynamical fluctuations.
doi: 10.1016/0370-2693(93)90777-F
1992AY03 Nucl.Phys. A545, 35c (1992) S.Ayik, E.Suraud, M.Belkacem, D.Boilley The Boltzmann-Langevin Model for Nuclear Collisions NUCLEAR REACTIONS 12C(12C, 12C), E=40-100 MeV/nucleon; calculated total quadrupole momentum distribution associated collision rate, diffusion coeffient, mean value, variance time evolutions. 12C(12C, K+X), E ≈ 400-1400 MeV/nucleon; calculated K+ production σ(E). Boltzmann-Langevin model.
doi: 10.1016/0375-9474(92)90444-O
1992SU10 Nucl.Phys. A542, 141 (1992) E.Suraud, S.Ayik, M.Belkacem, J.Stryjewski Applications of Boltzmann-Langevin Equation to Nuclear Collisions NUCLEAR REACTIONS 12C(12C, X), E=40 MeV/nucleon; calculated quadrupole, octupole moments, momentum distribution mean value time evolution, dispersion. Approximate numerical solutions to Boltzmann-Langevin equations.
doi: 10.1016/0375-9474(92)90403-7
1991PI04 Nucl.Phys. A524, 537 (1991) Quasi-Fusion of 139La + 12C at Intermediate Energies ( Question ) A study within the Landau-Vlasov approach NUCLEAR REACTIONS 12C(139La, X), E=50-170 MeV/nucleon; analyzed data; deduced fusion threshold beam energy dependence.
doi: 10.1016/0375-9474(91)90284-D
1991TO01 Phys.Rev. C43, R1518 (1991) Weighted Particle Method for Solving the Boltzmann Equation NUCLEAR STRUCTURE 12C; calculated quadrupole moment time evolution. Weighted particle method, quadrupole motion.
doi: 10.1103/PhysRevC.43.R1518
1990GA25 Z.Phys. A337, 261 (1990) F.Garcias, M.Barranco, J.Navarro, E.Suraud High Temperature Giant Dipole and Isoscalar Resonances NUCLEAR STRUCTURE 63Cu, 90Zr, 114Sn, 140Ce, 160Er, 208Pb; calculated GDR energy vs temperature. Semi-classical approximation, RPA sum rules.
1989SU05 Nucl.Phys. A492, 294 (1989) Giant Dipole Modes in Heavy-Ion Reactions NUCLEAR REACTIONS 12C(12Be, 12Be'), 40Ca(16O, 16O'), E=5 MeV/nucleon; calculated dipole mode time evolution.
doi: 10.1016/0375-9474(89)90088-2
1989SU10 Nucl.Phys. A495, 73c (1989) E.Suraud, D.Cussol, Ch.Gregoire, D.Boilley, M.Pi, P.Schuck, B.Remaud, F.Sebille Explosions in Landau Vlasov Dynamics NUCLEAR REACTIONS 40Ca(40Ca, X), E=20-100 MeV/nucleon; 50Ti(40Ar, X), E=20, 44 MeV/nucleon; 197Au(40Ar, X), E=60 MeV/nucleon; calculated average density time evolution. Landau-Vlasov simulations.
doi: 10.1016/0375-9474(89)90309-6
1988SU03 Nucl.Phys. A480, 29 (1988) E.Suraud, M.Barranco, J.Treiner A Semi-Classical Model for Isoscalar Giant Resonances at Finite Temperatures NUCLEAR STRUCTURE 56Fe, 208Pb; calculated neutron, proton rms radii. 90Zr, 40Ca, 120Sn, 208Pb; calculated isoscalar giant resonances. Semi-classical model, finite temperatures.
doi: 10.1016/0375-9474(88)90382-X
1988SU05 Nucl.Phys. A482, 187c (1988) Excitation of Giant Dipole Modes in Heavy-Ion Reactions NUCLEAR REACTIONS 12C(12Be, X), E=5 MeV/nucleon; calculated GDR excitation strength function. Nonlinearized Vlasov equation.
doi: 10.1016/0375-9474(88)90584-2
1987SU02 Nucl.Phys. A462, 109 (1987) Semi-Classical Calculations of Hot Nuclei NUCLEAR STRUCTURE 56Fe, 208Pb; calculated neutron, proton density profiles, mean square radii, chemical potentials, total energies; 90Rh; calculated neutron, proton density profiles. 56Fe, 208Pb, Sb, Xe, Ba, Cs, Ce, Nd, Pr, Sm, Gd, Eu, Dy, Er; calculated excitation energies per particle. Bonche-Levit-Vautherin formalism.
doi: 10.1016/0375-9474(87)90382-4
1987SU19 J.Phys.(Paris), Colloq.C-2, 11 (1987) E.Suraud, M.Barranco, J.Treiner A Semi-Classical Description of Giant Resonances at Finite Temperature NUCLEAR STRUCTURE 90Zr, 120Sn, 208Pb; calculated giant resonance energies vs temperature. Semi-classical model.
1985SU14 Phys.Lett. 164B, 212 (1985) On the Temperature Dependence of the Level Density Parameter NUCLEAR STRUCTURE 208Pb, 90Zr, 40Ca; calculated level density parameter vs temperature; deduced Bethe formula validity. Self-consistent, semi-classical model.
doi: 10.1016/0370-2693(85)90311-9
1984SU04 Phys.Lett. 138B, 325 (1984) Thomas-Fermi Calculations of Hot Dense Matter NUCLEAR STRUCTURE 208Pb; calculated proton distribution. Thomas-Fermi calculation, finite temperature.
doi: 10.1016/0370-2693(84)91908-7
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