NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = C.Ngo Found 102 matches. Showing 1 to 100. [Next]2000IG01 Nucl.Phys. A662, 295 (2000) Surface Multifragmentation Investigated with a Finite Temperature Spherical TDHF Model NUCLEAR STRUCTURE 208Pb; calculated fragment yields vs temperature, compression. Time-dependent Hartree-Fock calculations, surface multifragmentation.
doi: 10.1016/S0375-9474(99)00418-2
1998BE51 Phys.Rev. C58, 1639 (1998) M.Begemann-Blaich, V.Lindenstruth, J.Pochodzalla, J.C.Adloff, P.Bouissou, J.Hubele, G.Imme, I.Iori, P.Kreutz, G.J.Kunde, S.Leray, Z.Liu, U.Lynen, R.J.Meijer, U.Milkau, A.Moroni, W.F.J.Muller, C.Ngo, C.A.Ogilvie, G.Raciti, G.Rudolf, H.Sann, M.Schnittker, A.Schuttauf, W.Seidel, L.Stuttge, W.Trautmann, A.Tucholski Breakup Conditions of Projectile Spectators from Dynamical Observables NUCLEAR REACTIONS C, 27Al, Cu, Pb(197Au, X), E=600 MeV/nucleon; measured fragments mass, charge, multiplicity distributions, kinematic correlations; deduced source parameters. Statistical model comparisons.
doi: 10.1103/PhysRevC.58.1639
1995SC11 Nucl.Phys. A584, 704 (1995) F.Schussler, H.Nifenecker, B.Jakobsson, V.Kopljar, K.Soderstrom, S.Leray, C.Ngo, S.Souza, J.P.Bondorf, K.Sneppen Fragment Emission Pattern in Central and Semi-Central Heavy-Ion Collisions NUCLEAR REACTIONS Ag, Br(C, X), (O, X), (Ar, X), (Kr, X), E=50-220 MeV/nucleon; measured momentum vectors for all charged fragments. Emulsions, central collisions.
doi: 10.1016/0375-9474(94)00771-E
1994SO05 Nucl.Phys. A571, 159 (1994) S.R.Souza, L.de Paula, S.Leray, J.Nemeth, C.Ngo, H.Ngo A Dynamical Model for Multifragmentation of Nuclei NUCLEAR REACTIONS 80Br(16O, X), E ≤ 200 MeV/nucleon; calculated fragment charge distribution, multi-fragmentation probability vs impact parameter. Molecular dynamics based schematic model.
doi: 10.1016/0375-9474(94)90346-8
1994SO08 Phys.Rev. C50, 257 (1994) S.R.Souza, F.Schussler, R.Donangelo, K.Sneppen, J.P.Bondorf, R.Elmer, B.Jakobsson, S.Leray, C.Ngo, H.Nifenecker Angular Patterns from Fragments Produced in Central Heavy-Ion Collisions NUCLEAR REACTIONS Ag, Br(16O, X), E=210 MeV/nucleon; Ag, Br(36Ar, X), E=65 MeV/nucleon; Ag, Br(84Kr, X), E=95 MeV/nucleon; analyzed fragment σ(θ), multipolarity coefficients; deduced multi-fragmenting system shape features. Molecular dynamical approach.
doi: 10.1103/PhysRevC.50.257
1994TR10 Acta Phys.Pol. B25, 425 (1994) W.Trautmann, J.C.Adloff, M.Begemann-Blaich, P.Bouissou, J.Hubele, G.Imme, I.Iori, P.Kreutz, G.J.Kunde, S.Leray, V.Lindenstruth, Z.Liu, U.Lynen, R.J.Meijer, U.Milkau, A.Moroni, W.F.J.Muller, C.Ngo, C.A.Ogilvie, J.Pochodzalla, G.Raciti, G.Rudolf, H.Sann, A.Schuttauf, W.Seidel, L.Stuttge, A.Tucholski Multifragmentation in Peripheral Nucleus-Nucleus Collisions NUCLEAR REACTIONS C, 27Al, Cu, Pb(197Au, X), E=600 MeV/nucleon; 197Au(197Au, X), E=100-400 MeV/nucleon; analyzed multi-fragmentation data. Statistical multi-fragmentation models.
1993KR13 Nucl.Phys. A561, 672 (1993) P.Kreutz, J.C.Adloff, M.Begemann-Blaich, P.Bouissou, J.Hubele, G.Imme, I.Iori, G.J.Kunde, S.Leray, V.Lindenstruth, Z.Liu, U.Lynen, R.J.Meijer, U.Milkau, A.Moroni, W.F.J.Muller, C.Ngo, C.A.Ogilvie, J.Pochodzalla, G.Raciti, G.Rudolf, H.Sann, A.Schuttauf, W.Seidel, L.Stuttge, W.Trautmann, A.Tucholski Charge Correlations as a Probe of Nuclear Disassembly NUCLEAR REACTIONS C, 27Al, Cu, Pb(197Au, X), E=600 MeV/nucleon; measured fragment production σ, charge asymmetries, event-by-event charge moments.
doi: 10.1016/0375-9474(93)90476-E
1993KU06 Phys.Rev.Lett. 70, 2545 (1993) G.J.Kunde, J.Pochodzalla, E.Berdermann, B.Berthier, C.Cerruti, C.K.Gelbke, J.Hubele, P.Kreutz, S.Leray, R.Lucas, U.Lynen, U.Milkau, C.Ngo, C.H.Pinkenburg, G.Raciti, H.Sann, W.Trautmann Proton-Proton Correlations in 40Ar + 197Au Reactions and the Role of the Two-Particle Phase Space NUCLEAR REACTIONS 197Au(40Ar, X), E=200 MeV/nucleon; measured pp-correlation vs momentum; deduced two-particle density role. Boltzmann-Uehling-Uhlenbeck, quantum molecular dynamics models.
doi: 10.1103/PhysRevLett.70.2545
1993MI17 Z.Phys. A346, 227 (1993) U.Milkau, M.L.Begemann-Blaich, E.-M.Eckert, G.Imme, P.Kreutz, A.Kuhmichel, M.Lattuada, U.Lynen, C.Mazur, W.F.J.Muller, J.B.Natowitz, C.Ngo, J.Pochodzalla, G.Raciti, M.Ribrag, H.Sann, W.Trautmann, R.Trockel Inclusive Fragment Production in 84Kr + 197Au at E/A = 35 MeV NUCLEAR REACTIONS 197Au(84Kr, X), E=35 MeV/nucleon; measured σ(fragment θ, E) for X=Li-Ar; deduced moving source parameters, multi-fragment processes evidence.
doi: 10.1007/BF01306083
1993SO15 Phys.Rev. C48, R2555 (1993) Exotic Density Shapes in Asymmetric Heavy Ion Collisions at Intermediate Bombarding Energies NUCLEAR REACTIONS 197Au(Kr, X), Ag(Ar, X), E=65 MeV/nucleon; calculated nuclear density time evolution. Asymmetric systems, Boltzmann-Uehling-Unlenbeck approach.
doi: 10.1103/PhysRevC.48.R2555
1992HU06 Phys.Rev. C46, R1577 (1992) J.Hubele, P.Kreutz, V.Lindenstruth, J.C.Adloff, M.Begemann-Blaich, P.Bouissou, G.Imme, I.Iori, G.J.Kunde, S.Leray, Z.Liu, U.Lynen, R.J.Meijer, U.Milkau, A.Moroni, W.F.J.Muller, C.Ngo, C.A.Ogilvie, J.Pochodzalla, G.Raciti, G.Rudolf, H.Sann, A.Schuttauf, W.Seidel, L.Stuttge, W.Trautmann, A.Tucholski, R.Heck, A.R.DeAngelis, D.H.E.Gross, H.R.Jaqaman, H.W.Barz, H.Schulz, W.A.Friedman, R.J.Charity Statistical Fragmentation of Au Projectiles at E/A = 600 MeV NUCLEAR REACTIONS C, 27Al, Cu, Pb(197Au, X), E=600 MeV/nucleon; measured intermediate mass fragments mean multiplicity.
doi: 10.1103/PhysRevC.46.R1577
1992WA05 Nucl.Phys. A539, 316 (1992) R.Wada, M.Gonin, M.Gui, K.Hagel, Y.Lou, D.Utley, J.B.Natowitz, G.Nebbia, D.Fabris, R.Billerey, B.Cheynis, A.Demeyer, D.Drain, D.Guinet, C.Pastor, L.Vagneron, K.Zaid, J.Alarja, A.Giorni, D.Heuer, C.Morand, B.Viano, C.Mazur, C.Ngo, S.Leray, R.Lucas, M.Ribrag, E.Tomasi Mechanisms of Non-Equilibrium Light-Particle Emission in 32S + Ag Reactions at 30 A.MeV NUCLEAR REACTIONS Ag(32S, X), E=30 MeV/nucleon; measured (fragment)(fragment)-coin, left-right asymmetries. Moving source fit, recoil effect, classical dynamical model. Solid state detector telescope, CSI(Tl) single crystal detectors.
doi: 10.1016/0375-9474(92)90273-M
1991DE16 Phys.Lett. 258B, 251 (1991) L.De Paula, J.Nemeth, B.-H.Sa, S.Leray, C.Ngo, H.Ngo, S.R.Souza, Y.-M.Zheng Stability of Excited Nuclei in a Dynamical Simulation NUCLEAR STRUCTURE 197Au; calculated stability against multifragmentation. Heat, compression, rotation type excitations, dynamical simulation.
doi: 10.1016/0370-2693(91)91079-B
1991HU04 Z.Phys. A340, 263 (1991) J.Hubele, P.Kreutz, J.C.Adloff, M.Begemann-Blaich, P.Bouissou, G.Imme, I.Iori, G.J.Kunde, S.Leray, V.Lindenstruth, Z.Liu, U.Lynen, R.J.Meijer, U.Milkau, A.Moroni, W.F.J.Muller, C.Ngo, C.A.Ogilvie, J.Pochodzalla, G.Raciti, G.Rudolf, H.Sann, A.Schuttauf, W.Seidel, L.Stuttge, W.Trautmann, A.Tucholski Fragmentation of Gold Projectiles: From evaporation to total disassembly NUCLEAR REACTIONS C, 27Al, Cu(197Au, X), E=600 MeV/nucleon; measured fragment spectra, particle multiplicity; deduced projectile fragmentation features.
doi: 10.1007/BF01294674
1991KU21 Phys.Lett. 272B, 202 (1991) G.J.Kunde, J.Pochodzalla, J.Aichelin, E.Berdermann, B.Berthier, C.Cerruti, C.K.Gelbke, J.Hubele, P.Kreutz, S.Leray, R.Lucas, U.Lynen, U.Milkau, W.F.J.Muller, C.Ngo, C.H.Pinkenburg, G.Raciti, H.Sann, W.Trautmann Emission Temperatures in 40Ar + 197Au Reactions in the Limiting Fragmentation Regime NUCLEAR REACTIONS 197Au(40Ar, X), E=200 MeV/nucleon; measured fragment emission temperatures for X=4He, 5Li; deduced fragment formation dynamics role.
doi: 10.1016/0370-2693(91)91820-L
1991MI11 Phys.Rev. C44, R1242 (1991) U.Milkau, E.Berdermann, B.Berthier, P.Bouissou, C.Cerruti, A.Demeyer, E.-M.Eckert, D.Guinet, K.D.Hildenbrand, J.Hubele, G.Imme, P.Kreutz, A.Kuhmichel, G.J.Kunde, S.Leray, P.Lhenoret, R.Lucas, U.Lynen, C.Mazur, W.F.J.Muller, C.Ngo, C.H.Pinkenburg, J.Pochodzalla, H.J.Rabe, G.Raciti, M.Ribrag, H.Sann, H.Stelzer, E.Tomasi, W.Trautmann, R.Trockel, R.Wada Intermediate Mass Fragments from 40Ar + 197Au: Transition from the incomplete fusion to the participant spectator regime NUCLEAR REACTIONS 197Au(40Ar, X), E=30, 220 MeV/nucleon; measured σ(fragment E, θ, Z) for Z=3-20; deduced σ vs Z, moving source parameters. Moving source analysis.
doi: 10.1103/PhysRevC.44.R1242
1990EC02 Phys.Rev.Lett. 64, 2483 (1990) E.-M.Eckert, A.Kuhmichel, J.Pochodzalla, K.D.Hildenbrand, U.Lynen, W.F.J.Muller, H.J.Rabe, H.Sann, H.Stelzer, W.Trautmann, R.Trockel, R.Wada, C.Cerruti, P.Lhenoret, R.Lucas, C.Mazur, C.Ngo, M.Ribrag, E.Tomasi, A.Demeyer, D.Guinet Transient Times of Fission in 40Ar + 232Th Peripheral Collisions NUCLEAR REACTIONS 232Th(40Ar, XF), E=30 MeV/nucleon; measured fission (fragment)(projectile fragment)-coin; deduced transient time, probability, other features.
doi: 10.1103/PhysRevLett.64.2483
1989GA10 Nucl.Phys. A495, 169c (1989) F.Garcias, M.Barranco, J.Nemeth, C.Ngo, X.Vinas The Fission of Hot Rotating Nuclei: A selfconsistent Thomas-Fermi calculation NUCLEAR STRUCTURE 109Cd, 118Sn, 164Ho, 186Os, 207Bi, 240Pu; calculated fission barrier thermal evolution. Axially deformed Thomas-Fermi model.
doi: 10.1016/0375-9474(89)90316-3
1989GA13 Phys.Rev. C40, 1522 (1989) F.Garcias, M.Barranco, H.S.Wio, C.Ngo, J.Nemeth Fission Stability Diagram of 240Pu NUCLEAR STRUCTURE 240Pu; calculated fission barrier vs quadrupole moment. Axially symmetric deformed Thomas-Fermi model.
doi: 10.1103/PhysRevC.40.1522
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
1989NG01 Nucl.Phys. A499, 148 (1989) C.Ngo, H.Ngo, S.Leray, M.E.Spina Dynamical Instability of Hot and Compressed Nuclei NUCLEAR STRUCTURE 208Pb, 40Ca; calculated density, temperature time evolution, fragmentation, cluster yield vs mass. Hot, compressed nuclei, dynamical instabilities.
doi: 10.1016/0375-9474(89)90275-3
1989WA04 Phys.Rev. C39, 497 (1989) R.Wada, D.Fabris, K.Hagel, G.Nebbia, Y.Lou, M.Gonin, J.B.Natowitz, R.Billerey, B.Cheynis, A.Demeyer, D.Drain, D.Guinet, C.Pastor, L.Vagneron, K.Zaid, J.Alarja, A.Giorni, D.Heuer, C.Morand, B.Viano, C.Mazur, C.Ngo, S.Leray, R.Lucas, M.Ribrag, E.Tomasi Temperatures and Excitation Energies of Hot Nuclei in the Reactions of 32S + Ag and 16O + Ag at 30 MeV/Nucleon NUCLEAR REACTIONS Ag(32S, X), (16O, X), E=30 MeV/nucleon; measured light charged particle energy spectra, (light fragment)(heavy fragment)-coin; deduced hot nuclei excitation energies, temperatures.
doi: 10.1103/PhysRevC.39.497
1988CE01 Nucl.Phys. A476, 74 (1988) C.Cerruti, J.Desbois, R.Boisgard, C.Ngo, J.Natowitz, J.Nemeth Multifragmentation and Incomplete Fusion in Central Heavy Ion Collisions within a Schematic Phenomenological Model NUCLEAR REACTIONS 197Au(12C, X), (20Ne, X), (40Ar, X), E=10-80 MeV/nucleon; calculated emitted nucleon number per projectile nucleon characteristics. Schematic phenomenological model.
doi: 10.1016/0375-9474(88)90374-0
1988GA07 Phys.Lett. 206B, 177 (1988) F.Garcias, M.Barranco, J.Nemeth, C.Ngo Thomas-Fermi Calculations of the Level Density Parameter of Deformed Nuclei NUCLEAR STRUCTURE 164Ho, 63Cu; calculated fission barrier vs quadrupole moment. 63Cu, 164Ho, 205At, 240Pu; calculated level density parameter vs quadrupole moment. Constrained Thomas-Fermi model.
doi: 10.1016/0370-2693(88)91487-6
1988GR04 Nucl.Phys. A481, 109 (1988) O.Granier, C.Cerruti, S.Leray, P.Lhenoret, R.Lucas, C.Mazur, J.Natowitz, C.Ngo, M.Ribrag, E.Tomasi, G.Imme, G.Raciti, G.Spinella, L.Albinski, A.Gobbi, N.Hermann, K.D.Hildenbrand, A.Olmi Study of the 129Xe + (nat)Ag, 197Au Systems at 23.7 and 27 MeV/u NUCLEAR REACTIONS 129Xe, Ag, 197Au(Xe, X), E=3057, 3483 MeV; measured fragments Z, mass distributions. Partial coincidences.
doi: 10.1016/0375-9474(88)90476-9
1987BA08 Nucl.Phys. A464, 29 (1987) M.Barranco, M.Pi, J.Nemeth, C.Ngo, E.Tomasi Spurious Continuum Effects on Excited Giant Resonances NUCLEAR STRUCTURE 40Ca; calculated giant monopole isoscalar strength function. 208Pb; calculated sum rules, average energies; deduced spurious continuum effects role. Time-dependent Thomas-Fermi model.
doi: 10.1016/0375-9474(87)90420-9
1987BE58 Phys.Lett. 193B, 417 (1987) B.Berthier, R.Boisgard, J.Julien, J.M.Hisleur, R.Lucas, C.Mazur, C.Ngo, M.Ribrag, C.Cerruti Target Fragmentation at Ultrarelativistic Energies NUCLEAR REACTIONS 197Au(16O, X), E=60, 200 GeV/nucleon; measured light nuclei inclusive mass distributions. Target fragmentation.
doi: 10.1016/0370-2693(87)91689-3
1987DE30 Z.Phys. A328, 101 (1987) J.Desbois, R.Boisgard, C.Ngo, J.Nemeth Multifragmentation of Excited Nuclei within a Schematic Hydrodynamical and Percolation Picture NUCLEAR STRUCTURE 16O, 40,48Ca, 60Ni, 90Zr, 116Sn, 140Ce, 208Pb, 238U; calculated binding energy. 208Pb; calculated nucleon density time evolution. Hydrodynamical model, hot compressed nuclei.
1987FA12 Phys.Lett. 196B, 429 (1987) D.Fabris, K.Hagel, J.B.Natowitz, G.Nebbia, R.Wada, R.Billerey, B.Cheynis, A.Demeyer, D.Drain, D.Guinet, C.Pastor, L.Vagneron, K.Zaid, J.Alarja, A.Giorni, D.Heuer, C.Morand, B.Viano, C.Mazur, C.Ngo, S.Leray, R.Lucas, M.Ribrag, E.Tomasi α-Emission Temperatures, Coulomb Instabilities and Nuclear Cracking NUCLEAR REACTIONS 107,109Ag(32S, αX), E=960 MeV; 107,109Ag(16O, αX), E=480 MeV; measured σ(Eα, θα); deduced α-emission temperatures.
doi: 10.1016/0370-2693(87)90795-7
1987LU03 Nucl.Phys. A464, 172 (1987) R.Lucas, C.Ngo, T.Suomijarvi, M.Berlanger, C.Cerruti, S.Chiodelli, D.Dalili, A.Demeyer, D.Guinet, S.Leray, C.Mazur, M.Ribrag Peripheral Collisions in the 84Kr + 92,98Mo, (nat)Au Reactions at 22 MeV/u NUCLEAR REACTIONS 92,98Mo, Ag, 197Au(84Kr, X), E=22 MeV/nucleon; measured σ(fragment θ) vs mass, fragment velocity spectra, charge variances with energy loss, isobaric width distributions. Peripheral collisions.
doi: 10.1016/0375-9474(87)90429-5
1987NG04 J.Phys.(Paris), Colloq.C-2, 157 (1987) C.Ngo, R.Boisgard, J.Desbois, J.Nemeth, M.Barranco Multifragmentation of Nuclei NUCLEAR STRUCTURE 208Pb; calculated multi-fragmentation instability, per nucleon excitation energy/binding energy, density vs radius. Irrotational hydrodynamical model.
1986CE02 Nucl.Phys. A453, 175 (1986) C.Cerruti, D.Guinet, S.Chiodelli, A.Demeyer, K.Zaid, S.Leray, P.Lhenoret, C.Mazur, C.Ngo, M.Ribrag, A.Lleres Investigation of the Fusion Process in the Ar-Induced Reaction on Ag(nat) at 19.6 MeV/Nucleon NUCLEAR REACTIONS Ag(40Ar, X), (40Ar, F), E=19.6 MeV/nucleon; measured evaporation residue σ(θ), fission fragment mass distribution, (fragment)(fragment)(θ), (fragment)(fragment)(φ); deduced evaporation residue, fission, fussion σ(E).
doi: 10.1016/0375-9474(86)90036-9
1986DA10 Nucl.Phys. A454, 163 (1986) D.Dalili, R.Lucas, C.Ngo, C.Cerruti, S.Leray, C.Mazur, M.Ribrag, T.Suomijarvi, M.Berlanger, S.Chiodelli, A.Demeyer, D.Guinet Investigation of the 84Kr + 92,98Mo, (nat)Ag and 197Au Systems at 22 MeV/u NUCLEAR REACTIONS 92,98Mo, Ag, 197Au(84Kr, X), E=1836 MeV; measured fragment Z, mass distribution. Simple kinematical model.
doi: 10.1016/0375-9474(86)90153-3
1986NA16 Z.Phys. A325, 467 (1986) J.B.Natowitz, S.Leray, R.Lucas, C.Ngo, E.Tomasi, C.Volant A Simple Leading Particle Explanation for Linear Momentum Transfer Systematics NUCLEAR REACTIONS 58Ni, 238U(12C, X), 232Th, 238U(14N, X), (n, X), (p, X), (d, X), E=20-150 MeV/nucleon; calculated most probable, average momentum transfers, excitation energy per projectile. Leading particle models.
1986NE02 Z.Phys. A323, 419 (1986) J.Nemeth, M.Barranco, C.Ngo, E.Tomasi Model for the Evolution of Hot and Compressed Spherical Nuclei NUCLEAR STRUCTURE 40Ca; calculated rms radius time evolution. 208Pb, 16O calculated density profile vs radius evolution. Hydrodynamical approach.
1986NE04 Z.Phys. A325, 347 (1986) J.Nemeth, M.Barranco, J.Desbois, C.Ngo Multifragmentation of Hot and Compressed Nuclei within a Time Dependent Thomas Fermi and Percolation Model NUCLEAR STRUCTURE 208Pb; calculated dynamical evolution, density profile, primary, secondary mass distribution, multifragmentation, normal de-excitation regions, maximum thermal excitation energy per nucleon; deduced hot compressed nuclei multifragmentation. Time dependent Thomas-Fermi, percolation models.
1986PA13 Nucl.Phys. A457, 146 (1986) Y.Patin, S.Leray, E.Tomasi, O.Granier, C.Cerruti, J.L.Charvet, S.Chiodelli, A.Demeyer, D.Guinet, C.Humeau, P.Lhenoret, J.P.Lochard, R.Lucas, C.Mazur, M.Morjean, C.Ngo, A.Peghaire, M.Ribrag, L.Sinopoli, T.Suomijarvi, J.Uzureau, L.Vagneron Fission Fragment-Light Particle Coincidences and Linear Momentum Transfer NUCLEAR REACTIONS 197Au(40Ar, F), E=19.6 MeV/nucleon; 238U(40Ar, F), E=35 MeV/nucleon; measured fission(fragment)(fragment)(θ); deduced linear momentum transfer, reaction mechanisms.
doi: 10.1016/0375-9474(86)90524-5
1986PI02 Phys.Lett. 166B, 1 (1986) M.Pi, M.Barranco, J.Nemeth, C.Ngo, E.Tomasi Time-Dependent Thomas-Fermi Approach to Nuclear Monopole Oscillations NUCLEAR STRUCTURE 16O, 40Ca; calculated isoscalar strength function. Time-dependent Thomas-Fermi approach.
doi: 10.1016/0370-2693(86)91143-3
1986RU08 Phys.Rev.Lett. 57, 2905 (1986); Erratum Phys.Rev. 58, 2003 (1987) G.Rudolf, J.C.Adloff, A.Kamili, F.Scheibling, B.Boishu, A.Genoux-Lubain, C.Le Brun, J.F.Lecolley, F.Lefebvres, M.Louvel, R.Regimbart, O.Granier, S.Leray, R.Lucas, C.Mazur, C.Ngo, M.Ribrag, E.Tomasi Correlated Sources of Heavy Fragments in the Kr + Au Reaction at 35 and 44 MeV/u NUCLEAR REACTIONS 197Au(84Kr, X), E=35 MeV/nucleon; 197Au(86Kr, X), E=44 MeV/nucleon; measured (fragment)(fragment)-coin, yields, fragment, projectile velocity ratios, Z distributions; deduced two different mechanisms. Parallel plate avalanche detectors.
doi: 10.1103/PhysRevLett.57.2905
1985DA01 Z.Phys. A320, 349 (1985) D.Dalili, M.Berlanger, S.Leray, R.Lucas, C.Mazur, C.Ngo, M.Ribrag, T.Suomijarvi, C.Cerruti, S.Chiodelli, A.Demeyer, D.Guinet, A.Genoux-Lubain, C.Lebrun, J.F.Lecolley, F.Lefebvres, M.Louvel Investigation of the Kr + Au System at 22 MeV/u NUCLEAR REACTIONS 197Au(84Kr, X), E=22 MeV/nucleon; measured σ(fragment θ) vs mass, Z, kinetic energy.
doi: 10.1007/BF01881287
1985DA05 Z.Phys. A321, 335 (1985) A Self Consistent Thomas Fermi Calculation of Fission Barriers at Finite Temperature and Angular Momentum as Applied to the 205At NUCLEAR STRUCTURE 205At; calculated fission barrier vs temperature, free, binding energies vs quadrupole moment. Self-consistent Thomas-Fermi calculation.
doi: 10.1007/BF01493455
1985LE02 Z.Phys. A320, 383 (1985) S.Leray, G.La Rana, C.Ngo, M.Barranco, M.Pi, X.Vinas Emission of Prompt Nucleons in Heavy Ion Collisions NUCLEAR REACTIONS 165Ho(20Ne, xn), E=220, 402, 700 MeV; calculated prompt neutron multiplicity. Incomplete fusion, dynamical model.
doi: 10.1007/BF01415714
1985LE03 Z.Phys. A320, 533 (1985) S.Leray, O.Granier, C.Ngo, E.Tomasi, C.Cerruti, P.L'Henoret, R.Lucas, C.Mazur, M.Ribrag, J.L.Charvet, C.Humeau, J.P.Lochard, M.Morjean, Y.Patin, L.Sinopoli, J.Uzureau, D.Guinet, L.Vagneron, A.Peghaire Investigation of Linear Momentum Transfer on the 35 MeV/u Ar + U System NUCLEAR REACTIONS 238U(40Ar, F), E=35 MeV/nucleon; measured fission(fragment)(fragment)(θ); deduced reaction mechanism.
doi: 10.1007/BF01415733
1985MO08 Nucl.Phys. A438, 547 (1985) M.Morjean, J.L.Charvet, J.L.Uzureau, Y.Patin, A.Peghaire, Y.Pranal, L.Sinopoli, A.Billerey, A.Chevarier, N.Chevarier, A.Demeyer, M.Stern, G.La Rana, S.Leray, R.Lucas, C.Mazur, G.Nebbia, C.Ngo, M.Ribrag Nuclear Fragmentation Process in the 20Ne + 27Al System at 30 MeV/A NUCLEAR REACTIONS 27Al(20Ne, X), E=600 MeV; measured inclusive σ(fragment θ), σ(fragment E); deduced reaction mechanism. Natural target.
doi: 10.1016/0375-9474(85)90393-8
1985NE02 Phys.Lett. 154B, 11 (1985) Hartree-Fock and Thomas-Fermi Self-Consistent Calculations of the 144Nd Nucleus at Finite Temperature and Angular Momentum NUCLEAR STRUCTURE 144Nd; calculated fission barrier; deduced temperature, angular momentum dependences. Constrained Hartree-Fock, Thomas-Fermi approximations.
doi: 10.1016/0370-2693(85)91557-6
1985NE03 Z.Phys. A320, 691 (1985) J.Nemeth, M.Barranco, C.Ngo, E.Tomasi Spherical Time Dependent Thomas-Fermi Calculation of the Dynamical Evolution of Hot and Compressed Nuclei NUCLEAR STRUCTURE 40Ca; calculated density profile vs temperature. Self consistent time-dependent Thomas-Fermi model.
doi: 10.1007/BF01411873
1985NG03 Z.Phys. A322, 419 (1985) Linear Momentum Transfer Estimations in Heavy Ion Collisions at Intermediate Bombarding Energies NUCLEAR REACTIONS 197Au(20Ne, X), (40Ar, X), (12C, X), E ≈ 10-100 MeV/nucleon; calculated linear momentum transfer to fusing system. Schematic static model.
1984BA66 Nucl.Phys. A428, 239c (1984) M.Barranco, M.Pi, X.Vinas, G.La Rana, S.Leray, C.Ngo, E.Tomasi Friction, Imaginary Potential and Nucleon Jetting Calculated from Nucleon Currents in Semi-Infinite Nuclear Matter NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=64.8-120 MeV; calculated reaction σ. 165Ho(20Ne, X), E=402 MeV; calculated promptly emitted σ(θn), σ(En). Heavy ion collisions, nucleon jetting model.
doi: 10.1016/0375-9474(84)90254-9
1984DA09 Z.Phys. A316, 371 (1984) D.Dalili, P.Lhenoret, R.Lucas, C.Mazur, C.Ngo, M.Ribrag, T.Suomijarvi, E.Tomasi, B.Boishu, A.Genoux-Lubain, C.Lebrun, J.F.Lecolley, F.Lefebvres, M.Louvel, R.Regimbart, J.C.Adloff, A.Kamili, G.Rudolf, F.Scheibling Experimental Evidence of Highly Energy Relaxed Products in the 35 MeV/u 84Kr + 197Au Reaction NUCLEAR REACTIONS 197Au(84Kr, X), E=35 MeV/nucleon; measured fragment mass, charge distributions; deduced preponderance of Z=20-28 fragments, production mechanism.
doi: 10.1007/BF01439911
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
1984LE13 Nucl.Phys. A423, 175 (1984) S.Leray, X.S.Chen, G.Y.Fan, C.Gregoire, H.Ho, C.Mazur, C.Ngo, A.Pfoh, M.Ribrag, L.Schad, E.Tomasi, J.P.Wurm Investigation of Fast Fission in the 35Cl + 238U System NUCLEAR REACTIONS 238U(35Cl, F), E=250-350 MeV; measured fission fragment mass distribution characteristics; deduced fast fission evidence.
doi: 10.1016/0375-9474(84)90304-X
1984LE16 Nucl.Phys. A425, 345 (1984) S.Leray, G.Nebbia, C.Gregoire, G.La Rana, P.Lhenoret, C.Mazur, C.Ngo, M.Ribrag, E.Tomasi, S.Chiodelli, J.L.Charvet, C.Lebrun Investigation of the 40Ar + 197Au, 238U Systems at 44 MeV/u NUCLEAR REACTIONS 238U, 197Au(40Ar, F), E=44 MeV/nucleon; measured fission(fragment)(fragment)(θ); deduced linear momentum transfer role in fission.
doi: 10.1016/0375-9474(84)90079-4
1984LU01 Nucl.Phys. A413, 516 (1984) R.Lucas, C.Gregoire, C.Ngo, J.Poitou, E.Tomasi, A.Gobbi, A.Olmi, H.Sann, G.Wirth, J.V.Kratz, U.Lynen Equilibration of the Neutron-to-Proton Ratio for Heavy Asymmetric Systems in Heavy-Ion Collisions NUCLEAR REACTIONS 74Ge(208Pb, X), E=1550 MeV; 197Au(86Kr, X), E=550 MeV; measured σ(fragment) vs mass, charge, variances; deduced neutron to proton ratio equilibration differences. Heavy asymmetric systems.
doi: 10.1016/0375-9474(84)90425-1
1984PI13 Nucl.Phys. A426, 163 (1984) M.Pi, X.Vinas, M.Barranco, G.La Rana, S.Leray, C.Ngo, E.Tomasi Nucleon Currents between Highly Excited Nuclei (II). Influence of the Relative Motion NUCLEAR REACTIONS 40Ca(16O, X), E=40-204.1 MeV; 88Sr(16O, X), E=48-59 MeV; 28Si(16O, X), E=81, 141 MeV; 208Pb(16O, X), E=129.5-312.6 MeV; 40Ca(20Ne, X), E=151 MeV; 32S(32S, X), E=90.9 MeV; 40Ca(40Ca, X), E=143.6-240 MeV; 58Ni(16O, X), E=142 MeV; 209Bi(136Xe, X), E=940, 1130 MeV; calculated optical potential imaginary part for nucleon transfer at strong absorption radius. Finite temperature Thomas-Fermi method.
doi: 10.1016/0375-9474(84)90071-X
1984SU08 Nuovo Cim. 82A, 51 (1984) T.Suomijarvi, R.Lucas, C.Ngo, E.Tomasi, D.Dalili, J.Matuszek The Role of Dynamics in the Fusion of Two Heavy Nuclei NUCLEAR REACTIONS 40Ca(32S, X), 152Sm(12C, X), E(cm) ≈ 50-59 MeV; 26,24Mg(16O, X), E(cm) ≈ 20-50 MeV; 27Al(16O, X), E(cm) ≈ 20-100 MeV; 28Si(16O, X), E(cm) ≈ 20-50 MeV; 63Cu(16O, X), E(cm) ≈ 40-66 MeV; 148,146Nd(16O, X), 148Nd(18O, X), E(cm) ≈ 59-71 MeV; 40Ca(20Ne, X), 24Mg(32S, X), 24Mg(24Mg, X), E(cm) ≈ 25-50 MeV; 63Cu(26Mg, X), E(cm) ≈ 120-250 MeV; 208Pb(26Mg, X), E(cm) ≈ 10-12 MeV; 28Si(28Si, X), E(cm) ≈ 33-40 MeV; 27Al(35Cl, X), E(cm) ≈ 33-100 MeV; 48Ti, 56Fe, 58,62,64Ni, 90Zr(35Cl, X), E(cm) ≈ 59-100 MeV; 90Zr(35Cl, X), E(cm) ≈ 90-110 MeV; 141Pr, 112,116,120,124Sn(35Cl, X), E(cm) ≈ 100-120 MeV; 109Ag, 123Sb, 165Ho(40Ar, X), E(cm) ≈ 120-250 MeV; 148,154,144Sm(40Ar, X), E(cm) ≈ 130-140 MeV; 208Pb(48Ca, X), (50Ti, X), (52Cr, X), (58Fe, X), 165Ho(56Fe, X), E(cm) ≈ 220-333 MeV; 65Cu(63Cu, X), 45Sc(84Kr, X), 132Xe(30Si, X), E(cm) ≈ 100-167 MeV; calculated fusion σ(E); deduced fusion mechanism. Phenomenological model.
1983CH16 Nucl.Phys. A401, 143 (1983) X.S.Chen, C.Ngo, E.Tomasi, M.Barranco, X.Vinas, H.Ngo Real Part of the Nuclear Interaction Potential between α or p and Excited Heavy Nuclei NUCLEAR REACTIONS 56Fe, 208Pb(p, p), (α, α), E not given; calculated interaction potentials. 40Ca, 51V, 56Fe, 59Co, 60,62Ni, 63Cu, 90Zr, 116Sn, 181Ta, 197Au, 208Pb, 233,238U(α, X), (p, p), E not given; calculated fusion barrier, proton potential barrier vs temperature. Double folding model.
doi: 10.1016/0375-9474(83)90341-X
1983LA22 Nucl.Phys. A407, 233 (1983) G.La Rana, G.Nebbia, E.Tomasi, C.Ngo, X.S.Chen, S.Leray, P.Lhenoret, R.Lucas, C.Mazur, M.Ribrag, C.Cerruti, S.Chiodelli, A.Demeyer, D.Guinet, J.L.Charvet, M.Morjean, A.Peghaire, Y.Pranal, L.Sinopoli, J.Uzureau, R.De Swiniarski Linear Momentum Transfer Investigated in the 20Ne + 197Au and 209Bi Systems at 30 MeV/u NUCLEAR REACTIONS 197Au, 209Bi(20Ne, F), E=30 MeV/nucleon; measured fission (fragment)(fragment)-correlation, σ(fragment A), σ(fragment E); deduced fission σ, most probable projectile to nucleus linear momentum transfer. Monte Carlo simulation.
doi: 10.1016/0375-9474(83)90317-2
1983NA08 Phys.Rev. C28, 460 (1983) M.N.Namboodiri, R.K.Choudhury, J.B.Natowitz, K.Hagel, L.Adler, P.L.Gonthier, H.Simon, S.Kniffen, R.Patton, E.Tomasi, C.Ngo, C.Mazur, M.Ribrag Momentum Widths in the Fragmentation of 32 MeV/u 10B NUCLEAR REACTIONS 181Ta(10B, p), (10B, t), (10B, 3He), (10B, α), (10B, 9Be), (10B, 7Li), (10B, 6Li), E=320 MeV; measured σ(light fragment θ, E); deduced fragment momentum widths. Projectile fragmentation model.
doi: 10.1103/PhysRevC.28.460
1983NE06 Z.Phys. A311, 247 (1983) G.Nebbia, E.Tomasi, C.Ngo, X.S.Chen, G.La Rana, S.Leray, P.Lhenoret, R.Lucas, C.Mazur, M.Ribrag, C.Cerruti, S.Chiodelli, A.Demeyer, D.Guinet, J.L.Charvet, M.Morjean, Y.Pranal, A.Peghaire, L.Sinopoli, J.Uzureau, R.de Swiniarski Investigation of Linear Momentum Transfer on the 20Ne + 197Au System at 30 MeV/A NUCLEAR REACTIONS 197Au(20Ne, F), E=30 MeV/nucleon; measured fission (fragment)(fragment)(θ), (fragment)(fragment)(φ); deduced projectile to fissioning nucleus momentum transfer. Tof telescope, solid state detectors.
doi: 10.1007/BF01415111
1982BE34 Nucl.Phys. A385, 319 (1982) V.Bernard, C.Gregoire, C.Mazur, C.Ngo, M.Ribrag, G.Y.Fan, P.Gonthier, H.Ho, W.Kuhn, J.P.Wurm Further Experimental Study of Fast Fission with the Cl + Au System NUCLEAR REACTIONS 197Au(35Cl, F), (35Cl, X), E=204-317 MeV; measured fission induced σ(fragment θ), σ(fusion) versus mass; deduced reaction mechanism. Semi-static model.
doi: 10.1016/0375-9474(82)90175-0
1982BE43 Nucl.Phys. A388, 187 (1982) M.Berlanger, B.Borderie, D.Chapoulard, C.Gerschel, F.Hanappe, J.Kuzminski, J.Natowitz, C.Ngo, N.Perrin, B.Tamain Gamma Ray Multiplicities in Deep Inelastic Collisions for the Cu + Au 400 MeV System NUCLEAR REACTIONS Au(Cu, X), E=400 MeV; measured γ-multiplicities; deduced angular momentum transfer, repartition, variances, collective mode excitations.
doi: 10.1016/0375-9474(82)90515-2
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
1982NO10 Phys.Rev. C26, 1114 (1982) L.Nowicki, M.Berlanger, B.Borderie, C.Cabot, P.del Marmol, Y.El Masri, C.Gregoire, F.Hanappe, C.Ngo, B.Tamain Collective Modes Associated with the Proton-Induced Fission of 209Bi NUCLEAR REACTIONS 209Bi(p, F), E=60 MeV; measured fission fragment mass distribution, γ-multiplicity first, second moments, < Eγ >; deduced scission point shell effects, fragment spin dependence on rotational modes. 210Po deduced fission mechanism. Moretto-Schmitt model.
doi: 10.1103/PhysRevC.26.1114
1982TO03 Nucl.Phys. A373, 341 (1982) E.Tomasi, D.Ardouin, J.Barreto, V.Bernard, B.Cauvin, C.Magnago, C.Mazur, C.Ngo, E.Piasecki, M.Ribrag Fusion Excitation Function of the 40Ca + 40Ca System Close to the Threshold NUCLEAR REACTIONS 40Ca(40Ca, X), E=112.5-165 MeV; measured σ(fusion, E), σ(evaporation residue θ).
doi: 10.1016/0375-9474(82)90155-5
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
1982TO13 Nucl.Phys. A389, 69 (1982) E.Tomasi, X.S.Chen, S.Leray, C.Ngo, M.Barranco, X.Vinas, H.Ngo Calculation of Interaction Potentials between Two Heavy Ions at Finite Temperature NUCLEAR REACTIONS 40Ca(40Ca, X), 63Cu(24Mg, X), 109Ag(40Ar, X), E(cm) ≈ 66-200 MeV; calculated σ(fusion) vs E. Thomas-Fermi model, finite temperature nuclear densities.
doi: 10.1016/0375-9474(82)90291-3
1981BO15 Z.Phys. A299, 263 (1981) B.Borderie, M.Berlanger, D.Gardes, F.Hanappe, L.Nowicki, J.Peter, B.Tamain, S.Agarwal, J.Girard, C.Gregoire, J.Matuszek, C.Ngo A Possible Mechanism in Heavy Ion Induced Reactions: 'Fast fission process' NUCLEAR REACTIONS, Fission 165Ho(40Ar, F), E=180, 200, 230, 243, 280, 315, 340, 391 MeV; 181Ta(24Mg, F), E=270, 335, 340 MeV; Re(20Ne, F), E=124, 206 MeV; measured σ(fusion), L(critical), fragment mass vs compound nucleus excitation, angular momentum; deduced fast fission process.
doi: 10.1007/BF01443944
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
1981TO18 Fizika(Zagreb) 13, Suppl.No.1, 6 (1981) E.Tomasi, D.Ardouin, J.Barreto, V.Bernard, H.Doubre, C.Ngo, C.Mazur, E.Piasecki, M.Ribrag Fusion Excitation Function of the 40Ca + 40Ca System near Threshold NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm) ≈ 60-80 MeV; measured σ(fusion, E). Two-dimensional position sensitive detector.
1980BO27 Z.Phys. A298, 235 (1980) B.Borderie, R.Bimbot, C.Cabot, D.Gardes, L.Nowicki, B.Tamain, C.Gregoire, C.Ngo, M.Berlanger, F.Hanappe Limitation to the Fusion Cross Section for the System Mg + Cu at High Energy NUCLEAR REACTIONS Cu(24Mg, X), E=161-341 MeV; measured σ(θ) for evaporation residue, σ(fusion, E); deduced critical angular momentum. Sharp cutoff model.
doi: 10.1007/BF01418662
1980GU09 Z.Phys. A295, 105 (1980) D.Guerreau, J.Galin, B.Gatty, X.Tarrago, J.Girard, R.Lucas, C.Ngo Seven New Neutron Rich Nuclides Observed in Deep Inelastic Collisions Of 340 MeV 40Ar on 238U NUCLEAR REACTIONS 238U(40Ar, X), E=340 MeV; measured σ for 54Ti, 56V, 58,59Cr, 61Mn, 63,64Fe. deep-inelastic collisions.
1980NG01 Nucl.Phys. A348, 140 (1980) Calculation of the Real Part of the Interacting Potential between Two Heavy Ions in the Sudden Approximation NUCLEAR STRUCTURE 16O, 40,48Ca, 60Ni, 90Zr, 116Sn, 140Ce, 208Pb, 238U; calculated binding energies. Energy density formalism, generalized Thomas-Fermi form, variational procedure. NUCLEAR REACTIONS 197Au(40Ar, 40Ar), (136Xe, 136Xe), 112,114,116,118,122,124Sn(40Ca, 40Ca), E not given; calculated real potential. Sudden approximation, energy density formalism.
doi: 10.1016/0375-9474(80)90550-3
1979BE23 Z.Phys. A291, 133 (1979) M.Berlanger, A.Gobbi, F.Hanappe, U.Lynen, C.Ngo, A.Olmi, H.Sann, H.Stelzer, H.Richel, M.F.Rivet Study of a Fast Collective Mode in Deep Inelastic Reactions: Quantal Fluctuations NUCLEAR REACTIONS 92,98Mo(86Kr, X), E=430 MeV; measured σ(E(X), A, Z); deduced reaction mechanism of fast collective mode.
doi: 10.1007/BF01437993
1979GE01 Nucl.Phys. A317, 473 (1979) C.Gerschel, M.A.Deleplanque, M.Ishihara, C.Ngo, N.Perrin, J.Peter, B.Tamain, L.Valentin, D.Paya, Y.Sugiyama, M.Berlanger, F.Hanappe Angular Momentum Transfer in Deep Inelastic Collisions for the Ar + Au and Cu + Au Systems NUCLEAR REACTIONS Au(Ar, X), E=227 MeV; Au(63Cu, X), E=365, 443 MeV; measured γ-ray multiplicities of the hot fragments; deduced L-transfer. Comparison with theory.
doi: 10.1016/0375-9474(79)90493-7
1979HO30 Z.Phys. A293, 229 (1979) H.Hofmann, C.Gregoire, R.Lucas, C.Ngo A Theoretical Model for the Charge Equilibration in Heavy Ion Collisions NUCLEAR REACTIONS 92Mo(86Kr, X), E=430 MeV; 197Au(136Xe, X), E=900 MeV; calculated fragment production σ. Quantal mass equation, dynamical treatment of charge equilibration.
doi: 10.1007/BF01435592
1979LE12 Nucl.Phys. A321, 207 (1979) C.Lebrun, F.Hanappe, J.F.Lecolley, F.Lefebvres, C.Ngo, J.Peter, B.Tamain Influence of Angular Momentum on the Mass Distribution Width of Heavy Ion Induced Fission: What Is the Frontier between Fission and Quasi-Fission (Question) NUCLEAR REACTIONS Re(20Ne, X), E=124, 206 MeV; 165Ho(40Ar, X), E=192, 197 MeV; measured mass distribution of fission fragments. 205At deduced temperature effect on width of mass distributions.
doi: 10.1016/0375-9474(79)90693-6
1979NG01 Nucl.Phys. A313, 15 (1979) C.Ngo-Trong, T.Suzuki, D.J.Rowe The Tensor Open-Shell Random Phase Approximation with Application to the Even Nickel Isotopes NUCLEAR STRUCTURE 58,60,62,64Ni; calculated energy levels, isoscalar, electromagnetic transition rates in tensor open-shell RPA.
doi: 10.1016/0375-9474(79)90566-9
1979TA15 Nucl.Phys. A330, 253 (1979) B.Tamain, R.Chechik, H.Fuchs, F.Hanappe, M.Morjean, C.Ngo, J.Peter, M.Dakowski, B.Lucas, C.Mazur, M.Ribrag, C.Signarbieux Neutron Multiplicity in Deep Inelastic Collisions: 400 MeV Cu + Au System NUCLEAR REACTIONS 197Au(63Cu, X), E=400 MeV; (fragment) n-coin, fragment mass; neutron multiplicity, equilibration relaxation time.
doi: 10.1016/0375-9474(79)90549-9
1978BE03 Z.Phys. A284, 61 (1978) M.Berlanger, C.Ngo, P.Grange, J.Richert, H.Hofmann Statistical Fluctuations and the Double Differential Cross Section for Energy and Angle in Deep Inelastic Reactions NUCLEAR REACTIONS 232Th(40Ar, 40Ar), E=388 MeV; calculated σ(θ).
doi: 10.1007/BF01433876
1978BE18 Phys.Rev. C17, 1495 (1978) M.Berlanger, P.Grange, H.Hofmann, C.Ngo, J.Richert Influence of Coulomb and Nuclear Forces on the Pattern of the Double Differential Cross Section d2σ/dθdE for Deep Inelastic Reactions NUCLEAR REACTIONS 120Sn(84Kr, X), E=514 MeV; 208Pb(208Pb, X), E=1560 MeV; 208Pb(136Xe, X), E=1000 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.17.1495
1978BE23 Z.Phys. A286, 207 (1978) M.Berlanger, P.Grange, H.Hofmann, C.Ngo, J.Richert Triple Differential Cross Section for Angle, Atomic Number and Energy (Or Angular Momentum Transfer) Calculated for the 280 MeV 40Ar + 58Ni (Or 365 MeV 63Cu + 197Au) System in a Simple Model NUCLEAR REACTIONS 58Ni(40Ar, X), E=280 MeV; 197Au(63Cu, X), E=365 MeV; calculated σ(E, Z, θ).
doi: 10.1007/BF01408977
1977BE07 Nucl.Phys. A276, 347 (1977) M.Berlanger, F.Hanappe, C.Ngo, J.Peter, F.Plasil, B.Tamain Deep Inelastic Collisions between 280 MeV 63Cu Ions and 93Nb Nuclei NUCLEAR REACTIONS 93Nb(63Cu, F), (63Cu, X), E=280 MeV; measured masses, kinetic energies, angular distributions; deduced cross sections.
doi: 10.1016/0375-9474(77)90388-8
1977NG01 Z.Phys. A282, 83 (1977) Mass Exchange and Angular Distribution in a Dynamical Treatment of Heavy Ion Collisions NUCLEAR REACTIONS 197Au(63Cu, X), E=365, 443 MeV; calculated quasi-fission σ(A).
1977NG02 Z.Phys. A283, 161 (1977) C.Ngo, J.Peter, B.Tamain, M.Berlanger, F.Hanappe Fusion and Deep Inelastic Collision Studied on the Ar + Au System I. Influence of the Bombarding Energy NUCLEAR REACTIONS 197Au(40Ar, X), E=201, 248 MeV; measured σ(E, A, θ). 197Au(40Ar, X), E=183, 189, 195, 201, 248 MeV; measured complete fusion σ.
1977PE16 Z.Phys. A283, 413 (1977) J.Peter, M.Berlanger, C.Ngo, B.Tamain, B.Lucas, C.Mazur, M.Ribrag, C.Signarbieux Neutron-Multiplicity in Deep Inelastic Collisions: 365 MeV Cu + Au System NUCLEAR REACTIONS 197Au(63Cu, X), E=365 MeV; measured neutron fragment coin.
1976BE52 J.Phys.(Paris), Lett. 37, L-323 (1976) M.Berlanger, M.A.Deleplanque, C.Gerschel, F.Hanappe, M.Leblanc, J.F.Mayault, C.Ngo, D.Paya, N.Perrin, J.Peter, B.Tamain, L.Valentin Gamma Ray Multiplicity in the Quasi-Fission of Cu + Au at 443 MeV NUCLEAR REACTIONS 197Au(63Cu, X), E=443 MeV; measured γ-ray multiplicity associated with quasi-fission, sequential fission.
doi: 10.1051/jphyslet:019760037012032300
1976HO22 Phys.Lett. 65B, 97 (1976) Influence of Statistical Fluctuations on the Angular Distribution of Deep Inelastic Reactions NUCLEAR REACTIONS 209Bi(Kr, X), E=525, 600 MeV; calculated σ.
doi: 10.1016/0370-2693(76)90001-0
1976NG02 Nucl.Phys. A267, 181 (1976) C.Ngo, J.Peter, B.Tamain, M.Berlanger, F.Hanappe Quasi-Fission Mass Distributions as a Random Walk Process: The 63Cu + 197Au System NUCLEAR REACTIONS 197Au(63Cu, X), E=365, 443 MeV; measured quasi-fission mass distributions. Interpretation as a nonequilibrium process.
doi: 10.1016/0375-9474(76)90652-7
1976TA01 Phys.Rev.Lett. 36, 18 (1976) B.Tamain, F.Plasil, C.Ngo, J.Peter, M.Berlanger, F.Hanappe Energy Dependence of Quasifission NUCLEAR REACTIONS 197Au(63Cu, F), E=443 MeV; measured σ(θ); compared with results at 365 MeV.
doi: 10.1103/PhysRevLett.36.18
1975NG01 Nucl.Phys. A240, 353 (1975) C.Ngo, B.Tamain, J.Galin, M.Beiner, R.J.Lombard Calculation of Interaction Barriers Using the Energy Density Formalism NUCLEAR REACTIONS 24Mg, 27Al, 40Ca, 58Ni(32S, X), 238U(12C, X), (14N, X), 121Sb, 162Dy, 238U, 80Se, 118Sn, 209Bi(40Ar, X), 74Ge, 114Cd, 40Ca, 186W(84Kr, X), 197Au, 238U(63Cu, X), 118Sn(118Sn, X), (114Cd, X); calculated interaction parameters.
doi: 10.1016/0375-9474(75)90335-8
1975NG02 Nucl.Phys. A252, 237 (1975) C.Ngo, B.Tamain, M.Beiner, R.J.Lombard, D.Mas, H.H.Deubler Properties of Heavy Ion Interaction Potentials Calculated in the Energy Density Formalism NUCLEAR REACTIONS 108Ag(14N, X), 63Cu, 108Ag(20Ne, X), 63Cu, 108Ag, 118Sn, 121Sb(40Ar, X), 197Au(63Cu, X), 63Cu, 74Ge, 84Kr, 108Ag, 197Au, 209Bi(84Kr, X), 63Cu, 108Ag(136Xe, X), 40Ca(40Ca, X); calculated interaction potential.
doi: 10.1016/0375-9474(75)90614-4
1975PE01 J.Phys.(Paris), Suppl.Lett. 36, L-23 (1975) Quasi-Fission Reactions Induced by 365 MeV 63Cu Ions on a 197Au Target NUCLEAR REACTIONS 197Au(63Cu, F), E=365 MeV; measured σ(E(fragment mass), θ).
1975PE08 Nucl.Phys. A250, 351 (1975) Complete Fusion and Quasi-Fission Reactions Induced by 84Kr Ions on Heavy Targets NUCLEAR REACTIONS 165Ho(84Kr, F), E=450, 492 MeV; 186W(84Kr, F), E=492 MeV; 238U(40Ar, F), E=300 MeV; 209Bi(84Kr, F), E=500, 525 MeV; 238U(84Kr, F), E=500 MeV; measured correlated kinetic energies; deduced complete fusion, quasi-fission σ.
doi: 10.1016/0375-9474(75)90265-1
1975TA15 Nucl.Phys. A252, 187 (1975) B.Tamain, C.Ngo, J.Peter, F.Hanappe Fission of Medium and Heavy Nuclei Induced by 40Ar from 160 to 300 Mev: Cross Sections NUCLEAR REACTIONS Mo(40Ar, F), E=200, 300 MeV; 165Ho(40Ar, F), E=226, 300 MeV; 209Bi, 238U(40Ar, F), E=250, 300 MeV; Sb(40Ar, F), E=162, 179, 199, 226, 300 MeV; measured σ(E(fragment mass), θ); deduced variation in critical angular momentum, reaction mechanism.
doi: 10.1016/0375-9474(75)90612-0
1974BO07 Nucl.Phys. A220, 93 (1974) B.Borderie, F.Hanappe, C.Ngo, J.Peter, B.Tamain Fission of Medium and Heavy Nuclei Induced by 40Ar from 160 to 300 MeV: Average Total Kinetic Energy NUCLEAR REACTIONS Mo, Sb, Pr, Ho, Au, Bi, Th, U(40Ar, F), E=160-300 MeV; measured total kinetic energy at symmetry; compared to theoretical predictions.
doi: 10.1016/0375-9474(74)90754-4
1974HA13 Phys.Rev.Lett. 32, 738 (1974) F.Hanappe, M.Lefort, C.Ngo, J.Peter, B.Tamain Cross Section and Angular Distribution of Products in 'Quasifission' Reactions Induced by 525-MeV 84Kr Ions on a 209Bi Target NUCLEAR REACTIONS 209Bi(84Kr, X), E=525 MeV; measured σ(E(reaction products), θ), deduced reaction mechanism.
doi: 10.1103/PhysRevLett.32.738
1974NA01 Nucl.Phys. A218, 495 (1974) O.Nalcioglu, D.J.Rowe, C.Ngo-Trong Excitation of the T > Components of the Giant Dipole States in N > Z Nuclei by Muon Capture NUCLEAR REACTIONS 58,60,62,64Ni(μ-, ν); measured nothing, calculated σ.
doi: 10.1016/0375-9474(74)90037-2
1974NG02 Nucl.Phys. A221, 37 (1974) Search for Coulomb Fission Induced by 84Kr Ions on 238U NUCLEAR REACTIONS 238U(84Kr, 84KrF), E=408-458 MeV; measured σ(E(84Kr), E(fragment)), compared to theoretical predictions.
doi: 10.1016/0375-9474(74)90097-9
1973LE21 Nucl.Phys. A216, 166 (1973) M.Lefort, C.Ngo, J.Peter, B.Tamain Recherche de Fission Provenant de l'Interaction 84Kr + 209Bi; La Fusion entre Ions Krypton et Noyaux Lourds Est-Elle Possible NUCLEAR REACTIONS 209Bi, 238U, 165Ho, 186W(Kr, F), E=500 MeV; measured σ(fission).
doi: 10.1016/0375-9474(73)90525-3
1972LE41 Nucl.Phys. A197, 485 (1972) M.Lefort, C.Ngo, J.Peter, B.Tamain Diffusion Elastique des Ions 84Kr sur 238U et Distance d'Approche pour Le Seuil de Reaction NUCLEAR REACTIONS 238U(84Kr, 84Kr), 400 < E < 500 MeV; measured σ.
doi: 10.1016/0375-9474(72)91023-8
Back to query form [Next] |