NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = B.Remaud Found 43 matches. 1996RE27 Ann.Phys.(Paris) 21, 503 (1996) Pseudo-Particle Models for Nuclear Reactions with Heavy Ions
1995RE05 Nucl.Phys. A583, 323c (1995) B.Remaud, B.Benhassine, M.Farine, D.Idier, F.Sebille Dynamics of Fluctuations in Heavy-Ion Reactions
doi: 10.1016/0375-9474(94)00679-H
1994HA10 Nucl.Phys. A572, 459 (1994) F.Haddad, G.Royer, F.Sebille, B.Remaud From Fission to Scattering in the 100Mo (18.7 MeV/u) + 100Mo Reaction within a Microscopic Dynamic Approach NUCLEAR REACTIONS 100Mo(100Mo, F), E=18.7 MeV/nucleon; calculated symmetric fission, fragmentation barriers. 100Mo(100Mo, X), E=18.7 MeV/nucleon; calculated per nucleon collective energy vs time from equilibration, other reaction dynamics. Landau-Vlasov transport equation.
doi: 10.1016/0375-9474(94)90184-8
1994ID03 Ann.Phys.(Paris) 19, 159 (1994) D.Idier, M.Farine, B.Remaud, F.Sebille Modelling an Infinite Nucleonic System. Static and Dynamical Properties. Study of Density Fluctuations
1993BO04 Phys.Lett. 302B, 15 (1993) B.Borderie, B.Remaud, M.F.Rivet, F.Sebille Coulomb Instability in Collisions between Very Heavy Nuclei Around 30 MeV per Nucleon NUCLEAR REACTIONS 155Gd(238U, X), E=35 MeV/nucleon; calculated Coulomb instability; deduced unstable bubbles formation.
doi: 10.1016/0370-2693(93)90628-U
1992DE25 Z.Phys. A343, 417 (1992) V.de la Mota, F.Sebille, B.Remaud, P.Schuck On the Competing Role of Mean-Field and Residual Interactions in Flow Observables NUCLEAR REACTIONS 93Nb(93Nb, X), E=150 MeV/nucleon; calculated flow observables; deduced mean field, residual interactions role. Semi-classical Landau-Vlasov approach.
doi: 10.1007/BF01289818
1992DE34 Phys.Rev. C46, 677 (1992) V.de la Mota, F.Sebille, M.Farine, B.Remaud, P.Schuck Analysis of the Transverse Momentum Collective Motion in Heavy-Ion Collisions below 100 MeV/Nucleon NUCLEAR REACTIONS 93Nb(93Nb, X), Ca(Ca, X), C(C, X), E=50-100 MeV/nucleon; calculated collective sideward flow vs E. 27Al(Ar, X), E=45, 65 MeV/nucleon; calculated mean transverse momentum vs longitudinal rapidity. Gogny type forces.
doi: 10.1103/PhysRevC.46.677
1991FA08 Z.Phys. A339, 363 (1991) M.Farine, T.Sami, B.Remaud, F.Sebille Isospin Effects on Dynamics of Heavy-Ion Collisions NUCLEAR REACTIONS 48Ca(48Ca, X), E=40 MeV/nucleon; calculated nucleon emission number vs model parameter; deduced isospin role on reaction dynamics. Landau-Valasov formalism, effective force.
doi: 10.1007/BF01560638
1991GA04 Phys.Lett. 255B, 311 (1991) F.Garcias, V.De La Mota, B.Remaud, G.Royer, F.Sebille Dynamics of Hot Rotating Nuclei NUCLEAR STRUCTURE 40Ca; calculated binding energy per nucleon, rms radius, deexcitation channels phase diagram; deduced fission disappearance at high excitation. Hot rotating nuclei, microscopic semi-classical transport formalism.
doi: 10.1016/0370-2693(91)90771-H
1991JO12 Z.Phys. A340, 63 (1991) D.Jouan, B.Borderie, M.F.Rivet, C.Cabot, H.Fuchs, H.Gauvin, C.Gregoire, F.Hanappe, D.Gardes, M.Montoya, B.Remaud, F.Sebille Dynamics and Thermalization in Violent Collisions between 40Ar and Ag at 27 MeV/nucleon NUCLEAR REACTIONS Ag(40Ar, X), E=27 MeV/nucleon; measured (fragment)(fragment)-coin; deduced reaction mechanism.
doi: 10.1007/BF01284482
1991RO06 Phys.Rev. C44, 2226 (1991) G.Royer, B.Remaud, F.Sebille, V.de la Mota Semiclassical Simulation of Sudden Nucleus Scission with Two-Body Collisions NUCLEAR STRUCTURE 40Ca; calculated fission barrier heights. Semi-classical simulation, two-body collision effects.
doi: 10.1103/PhysRevC.44.2226
1990AR12 Nucl.Phys. A514, 564 (1990) D.Ardouin, Z.Basrak, P.Schuck, A.Peghaire, F.Saint-Laurent, H.Delagrange, H.Doubre, C.Gregoire, A.Kyanowski, W.Mittig, J.Peter, Y.P.Viyogi, J.Quebert, C.K.Gelbke, W.G.Lynch, M.Maier, J.Pochodzalla, G.Bizard, F.Lefebvres, B.Tamain, B.Remaud, F.Sebille Preequilibrium Particles and Mean-Field Effects from Particle-Particle Correlations in Heavy-Ion Collisions NUCLEAR REACTIONS 197Au, Ti(40Ar, X), E=60 MeV/nucleon; measured (particle)(particle) correlations for X=p, d, α; deduced mean-field, two-body collisions effects. Landau-Vlasov equation analysis.
doi: 10.1016/0375-9474(90)90156-G
1990DA16 Phys.Lett. 247B, 223 (1990) H.Dabrowski, D.Goujdami, F.Guilbault, C.Lebrun, D.Ardouin, P.Lautridou, R.Boisgard, J.Quebert, A.Peghaire, P.Eudes, F.Sebille, B.Remaud Temperature Measurements at Backward Angles in 40Ar Induced Reactions on Ag at E/A = 44 MeV NUCLEAR REACTIONS Ag(40Ar, X), E=44 MeV/nucleon; measured pt-, dα-correlation; deduced target-like fragment emission temperature.
doi: 10.1016/0370-2693(90)90886-B
1989LE15 Nucl.Phys. A495, 283c (1989) S.Leray, C.Ngo, M.E.Spina, B.Remaud, F.Sebille Multifragmentation in the Framework of a Restructured Aggregation Model NUCLEAR REACTIONS 197Au(197Au, X), E=200 MeV/nucleon; calculated fragment yield vs mass, multiplicity distribution. Restructured aggregation model.
doi: 10.1016/0375-9474(89)90326-6
1989RO05 Nucl.Phys. A494, 267 (1989) G.Royer, C.Piller, J.Mignen, B.Remaud Prolate Deformations Induced by the Proximity Forces in the Scission Region NUCLEAR STRUCTURE 149Eu, 160Dy, 191Ir, 209Bi, 225Ra, 238Np, 242Am, 253Cf; calculated fission barrier heights. 40Ar, 258Fm; calculated deformation energy vs mass centers distance. 109Cd, 198Hg; calculated deformation energy vs mass center distance, fission barrier heights. Liquid drop model, nuclear proximity energy.
doi: 10.1016/0375-9474(89)90023-7
1989SE10 Nucl.Phys. A501, 137 (1989) F.Sebille, G.Royer, C.Gregoire, B.Remaud, P.Schuck Nuclear Dynamics with the (Finite-Range) Gogny Force: Flow effects NUCLEAR REACTIONS 93Nb(93Nb, X), E=150 MeV/nucleon; calculated average density time evolution. Landau-Vlasov equation, Gogny force.
doi: 10.1016/0375-9474(89)90569-1
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
1987GR04 Phys.Lett. 186B, 14 (1987) C.Gregoire, B.Remaud, F.Sebille, L.Vinet Peripheral Reactions at Intermediate Energies in Landau-Vlasov Dynamics NUCLEAR REACTIONS 27Al(40Ar, X), E=44 MeV/nucleon; calculated target fragment average recoil vs projectile-like mass, projectile-like fragment mean energy vs mass, bombarding energy per nucleon vs abraded nucleon number; 40Ca(16O, X), E=25 MeV/nucleon; calculated time evolution; 108Ag(40Ar, X), E=35 MeV/nucleon; calculated projectile-like fragment isospin vs time. Landau-Vlasov dynamics.
doi: 10.1016/0370-2693(87)90504-1
1987GR09 Nucl.Phys. A465, 317 (1987) C.Gregoire, B.Remaud, F.Sebille, L.Vinet, Y.Raffray Semi-Classical Dynamics of Heavy-Ion Reactions NUCLEAR REACTIONS 27Al(40Ar, X), E=27, 35 MeV/nucleon; calculated collision dynamics characteristics. Extended Vlasov equation.
doi: 10.1016/0375-9474(87)90437-4
1987GR29 J.Phys.(Paris), Colloq.C-2, 203 (1987) C.Gregoire, B.Remaud, F.Sebille, L.Vinet, D.Jacquet Low and Intermediate Energy Heavy Ion Collisions in the Semi-Classical Microscopic Description NUCLEAR REACTIONS 27Al(40Ar, X), E=27, 35, 44 MeV/nucleon; 28Si(28Si, X), E=12 MeV/nucleon; 238U(40Ar, X), E=27 MeV/nucleon; 40Ca(16O, X), E=5.5 MeV/nucleon; calculated fragment mass-mass correlations, ejectile energies, σ(θ). Landau-Vlasov dynamics.
1987RO10 Nucl.Phys. A466, 139 (1987) G.Royer, Y.Raffray, A.Oubahadou, B.Remaud On the Projectile Fragmentation in Heavy-ion Reactions at Intermediate Energies NUCLEAR REACTIONS 197Au(20Ne, X), E=7.5-20 MeV/nucleon; 109Ag(40Ar, X), E=27 MeV/nucleon; 27Al(40Ar, X), E=40 MeV/nucleon; 197Au(40Ar, X), E=35 MeV/nucleon; calculated projectile-like fragment energy spectra. NUCLEAR STRUCTURE 20Ne; calculated fission fragmentation potential barriers for 10B to d final products. 40Ar; calculated fission fragmentation potential barriers for 20F to α final products.
doi: 10.1016/0375-9474(87)90350-2
1987VI03 Nucl.Phys. A468, 321 (1987) L.Vinet, C.Gregoire, P.Schuck, B.Remaud, F.Sebille A Study of the Disintegration of Highly Excited Nuclei with the Vlasov-Uehling-Uhlenbeck Equation NUCLEAR STRUCTURE 40Ca; calculated fragmentation density profile time evolution, anisotropy, monopole Landau parameters, energy per nucleon, density distributions. 40Ar; calculated energy, excitation energy per nucleon, mean kinetic energy time evolution in fragmentation.
doi: 10.1016/0375-9474(87)90520-3
1986VI03 Phys.Lett. 172B, 17 (1986) L.Vinet, F.Sebille, C.Gregoire, B.Remaud, P.Schuck Solution of the Vlasov Equation for Compressed and Heated Spherical Nuclei NUCLEAR STRUCTURE 40Ca, 16O; calculated rms radius, density time evolutions.
doi: 10.1016/0370-2693(86)90208-X
1985GR07 Nucl.Phys. A436, 365 (1985) C.Gregoire, B.Remaud, F.Scheuter, F.Sebille Semiclassical Approaches to Proton Emission in Intermediate-Energy Heavy-Ion Reactions NUCLEAR REACTIONS 12C(12C, pX), E=1032 MeV; calculated σ(Ep, θp); deduced one- to two-body process transition. Semi-classical approach.
doi: 10.1016/0375-9474(85)90203-9
1985RO20 Nucl.Phys. A444, 477 (1985) Static and Dynamic Fusion Barriers in Heavy-Ion Reactions NUCLEAR REACTIONS 209Bi, 165Ho(84Kr, X), 208Pb(64Ni, X), (58Fe, X), (50Ti, X), 110Pd(136Xe, X), 238U, 165Ho(56Fe, X), 160Gd, 123Sb(86Kr, X), 197Au(63Cu, X), 170Er(76Ge, X), 209Bi, 208Pb(58Fe, X), 110Pd(110Pd, X), 94Zr(124Sn, X), 209Bi(54Cr, X), 208Pb(52Cr, X), 249Cm(48Ca, X), 209Bi, 208Pb(50Ti, X), 238U, 206Pb, 197Au, 165Ho(40Ar, X), 208Pb(48Ca, X), 90Zr(90Zr, X), 197Au(35Cl, X), 208Pb(32S, X), E not given; calculated fusion barrier heights, σ(E), potential energy. Liquid drop model, nuclear proximity energy.
doi: 10.1016/0375-9474(85)90464-6
1984DA25 Ann.Phys.(New York) 156, 68 (1984) K.T.R.Davies, B.Remaud, M.Strayer, K.R.Sandhya Devi, Y.Raffray Geometry and Dynamics of a Zero-Temperature Fermi-Gas Model for Preequilibrium Emission of Nucleons with Application to 16O + 93Nb at E(Lab) = 204 MeV NUCLEAR REACTIONS 93Nb(16O, nX), E=204 MeV; measured inclusive σ(θn); deduced neutron multiplicity. Preequilibrium emission, Fermi gas model.
doi: 10.1016/0003-4916(84)90211-2
1984RO16 J.Phys.(London) G10, 1057 (1984) Fission Process through Compact and Creviced Shapes NUCLEAR STRUCTURE 109Cd, 160Dy, 166Os, 198Hg, 212Po, 228Ra, 232Th, 234U, 240Pu, 246Cm; calculated fission barrier heights. One-parameter compact, creviced shapes.
doi: 10.1088/0305-4616/10/8/011
1984RO23 J.Phys.(London) G10, 1541 (1984) On the Fission Barrier of Heavy and Superhheavy Nuclei NUCLEAR STRUCTURE 149Eu, 152Tb, 157Ho, 173Lu, 179Ta, 180W, 185Re, 191Ir, 195Au, 201Tl, 206Pb, 209Bi, 213At, 216Rn, 226Ac, 238U, 244Pu, 242Am, 250Bk, 253Cf; calculated fission barrier heights. 238U, 246Cm, 258Fm, 260Rf, 294Ds, 298Fl, 302Og, 306122; calculated deformation energy vs mass centers distance. Liquid drop model, proximity interaction effects.
doi: 10.1088/0305-4616/10/11/010
1984SE11 Nucl.Phys. A420, 141 (1984) Coherent Production of Fast Nucleons in Heavy-Ion Reactions NUCLEAR REACTIONS 40Ca(40Ca, pX), E ≈ 40 MeV/nucleon; calculated fast proton coherent production, transfer between ions, multiplicity; deduced reaction mechanism. Boltzmann transport equation.
doi: 10.1016/0375-9474(84)90662-6
1983GR19 Phys.Lett. 127B, 308 (1983) Cluster Jets as a Possible α Emission Mechanism in Intermediate Energy Heavy Ion Collisions NUCLEAR REACTIONS 164Dy(40Ar, α), E=1600 MeV; calculated σ(Eα); deduced reaction mechanism. Semi-classical α-clustering model.
doi: 10.1016/0370-2693(83)91006-7
1983RO16 J.Phys.(London) G9, 1103 (1983) Symmetrical Fusion of Heavy Ions around the Coulomb Barrier Energy NUCLEAR REACTIONS, ICPND 13C(13C, X), E(cm) ≈ 3-15 MeV; 40Ca(40Ca, X), E(cm) ≈ 55-75 MeV; 28Si(28Si, X), E(cm) ≈ 33-100 MeV; 16O(16O, X), E(cm) ≈ 12-25 MeV; 58Ni(58Ni, X), E(cm)=95-105 MeV; 64Ni(64Ni, X), E(cm)=90-105 MeV; 90Zr(90Zr, X), E(cm) ≈ 180-205 MeV; calculated fusion σ(E); deduced fusion mechanism, barrier characteristics. Liquid drop model, neck degree of freedom, tunnelling effects.
doi: 10.1088/0305-4616/9/9/014
1983SE05 Z.Phys. A310, 99 (1983) Cold Production of Fast Nucleons in Central Heavy-Ion Reactions NUCLEAR REACTIONS 40Ca(40Ca, X), E=10-60 MeV/nucleon; calculated fast nucleon intensities, tunneling multiplicities; deduced reaction mechanism. Semi-classical model.
doi: 10.1007/BF01433617
1982GR16 Nucl.Phys. A383, 392 (1982) Fast fission Phenomenon, Deep Inelastic Reactions and Compound Nucleus Formation Described within a Dynamical Macroscopic Model NUCLEAR REACTIONS 165Ho(40Ar, X), (40Ar, F), E=180-391 MeV; calculated mass asymmetry radial distance, σ(fusion) vs E, σ(fragment, mass), σ(fragment E, mass); deduced deep inelastic collision, fast fission, compound nucleus formation angular momentum range. Dynamical macroscopic model. NUCLEAR STRUCTURE 205At; calculated sudden, adiabatic potentials. Dynamical macroscopic model.
doi: 10.1016/0375-9474(82)90084-7
1982RO11 J.Phys.(London) G8, L159 (1982) A Geometrical Model for the Fusion of Identical Nuclei NUCLEAR REACTIONS 109Ag(109Ag, X), 58Ni(58Ni, X), E not given; calculated potential energy vs interfragment distance. Geometrical fusion model.
doi: 10.1088/0305-4616/8/10/002
1982TO04 J.Phys.(Paris), Lett. 43, L-115 (1982) E.Tomasi, C.Gregoire, C.Ngo, B.Remaud Macroscopic Dynamics of the Fusion Process NUCLEAR REACTIONS, ICPND 27Al(16O, X), E(cm) ≈ 16-100 MeV; 40Ca(40Ca, X), E(cm) ≈ 60-100 MeV; 63Cu(24Mg, X), E(cm) ≈ 7-200 MeV; 35Cl(58Ni, X), E(cm) ≈ 67-100 MeV; 109Ag(40Ar, X), E(cm) ≈ 100-200 MeV; 165Ho(40Ar, X), E(cm) ≈ 143-333 MeV; calculated fusion σ vs E; deduced reaction mechanism. Macroscopic dynamical model.
doi: 10.1051/jphyslet:01982004304011500
1981GR02 Phys.Lett. 99B, 17 (1981) Three Dissipative Regimes in Heavy Ion Reactions- A Macroscopic Dynamical Model NUCLEAR REACTIONS 165Ho(40Ar, X), E=340 MeV; 92Mo(86Kr, X), E=430 MeV; calculated fragment mass vs excitation energy, fragment mass variance vs energy loss; deduced dissipation from compound nucleus formation, deep inelastic collision, fast fission. Macroscopic dynamical model.
doi: 10.1016/0370-2693(81)90795-4
1981HE12 Nucl.Phys. A361, 483 (1981) E.S.Hernandez, W.D.Myers, J.Randrup, B.Remaud Quantal Dynamics of Charge Equilibration in Damped Nuclear Collisions NUCLEAR REACTIONS 92Mo(86Kr, X), E=430 MeV; 197Au(132Xe, X), E=900 MeV; calculated projectile-like fragment mean charge, charge dispersion.
doi: 10.1016/0375-9474(81)90648-5
1978AR12 Phys.Rev. C18, 1201 (1978) D.Ardouin, C.Lebrun, F.Guilbault, B.Remaud, E.R.Flynn, D.L.Hanson, S.D.Orbesen, M.N.Vergnes, G.Rotbard, K.Kumar Structure of 78Ge from the 76Ge(t, p)78Ge Reaction NUCLEAR REACTIONS 76Ge(t, p), E=17 MeV; measured σ(Ep, θ); deduced Q. 78Ge deduced levels, J, π, mass excess. DWBA analysis, magnetic spectrograph.
doi: 10.1103/PhysRevC.18.1201
1978AR17 Phys.Rev. C18, 2739 (1978) D.Ardouin, B.Remaud, K.Kumar, F.Guilbault, P.Avignon, R.Seltz, M.Vergnes, G.Rotbard Nuclear Structure Investigations of the Ge Isotopes by Means of (p, t) Reactions and Microscopic Studies of Nuclear Deformations and Collective Spectra NUCLEAR STRUCTURE 68,70,72,74Ge; calculated deformation energy curves, collective spectra using microscopic theory. NUCLEAR REACTIONS 70,72,74,76Ge(p, t), E=26 MeV; reviewed data; deduced systematics about reaction mechanisms, structure.
doi: 10.1103/PhysRevC.18.2739
1978RE09 Nukleonika 23, 139 (1978) Semi-Microscopic Calculations of Even-Even Nucleus Collective Spectra. Results for the Germanium Isotopes NUCLEAR STRUCTURE 68,70,72,74,76,78Ge; calculated levels, potential energy surfaces. Deformed quasiparticle basis, collective schrodinger equation.
1977KU13 Phys.Rev. C16, 1235 (1977) K.Kumar, B.Remaud, P.Aguer, J.S.Vaagen, A.C.Rester, R.Foucher, J.H.Hamilton Deformed-Quasiparticle Basis for Calculating Potential Energy Surfaces And Nuclear Spectra NUCLEAR STRUCTURE 148,150,152,154Sm, 186,188,190,192,194Os, 184,186,188,190Hg; calculated deformation energy curves. 24Mg, 102Zr, 168Er; calculated deformation energy curves, collective spectra.
doi: 10.1103/PhysRevC.16.1235
1973LA26 J.Phys.(Paris) 34, 783 (1973) La Diffusion Elastique Nucleon-6Li NUCLEAR REACTIONS 6Li(n, n), (p, p); calculated phase shifts, binding energies.
doi: 10.1051/jphys:019730034010078300
1971RE07 C.R.Acad.Sci., Ser.B, 272, 390 (1971) Collision n-6Li par la Methode de Wheeler NUCLEAR REACTIONS 6Li(n, n), E=3.35, 7.5, 15 MeV; measured nothing; analyzed σ(θ).
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