NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = R.Cusson Found 39 matches. 1988JU01 Nucl.Phys. A477, 256 (1988) Chr.Jung, W.Cassing, U.Mosel, R.Y.Cusson Microscopic Investigations on the Fragmentation of Heavy Nuclei NUCLEAR STRUCTURE 109Ag; calculated fission, fragmentation characteristics. TDHF.
doi: 10.1016/0375-9474(88)90321-1
1988PE02 Nucl.Phys. A477, 277 (1988) M.Petrovici, J.Albinski, R.Bock, R.Cusson, A.Gobbi, G.Guarino, S.Gralla, K.D.Hildenbrand, W.F.J.Muller, A.Olmi, H.Stelzer, J.Toke Fast Dissipative Collisions NUCLEAR REACTIONS 98Mo, 147,154Sm(98Mo, X), 92Mo, 154Sm, 238U(92Mo, X), E=14.7 MeV/nucleon; measured σ(fragment θ), mass, charge variances, excitation energy sharing; deduced charge equilibration, excitation energy sharing mechanisms. Large area position sensitive ionization chamber. Monte Carlo simulation.
doi: 10.1016/0375-9474(88)90322-3
1987BA10 Z.Phys. A326, 269 (1987) J.J.Bai, R.Y.Cusson, J.Wu, P.-G.Reinhard, H.Stocker, W.Greiner, M.R.Strayer Mean Field Model for Relativistic Heavy Ion Collisions NUCLEAR REACTIONS 16O(16O, 16O), E=300, 600, 1200 MeV/nucleon; calculated total, field energies, maximum density, transverse vs longitudinal momentum; deduced scalar potential. Mean field model.
1986BA30 Nucl.Phys. A456, 159 (1986) W.Bauer, W.Cassing, U.Mosel, M.Tohyama, R.Y.Cusson High Energy γ-Ray Emission in Heavy-Ion Collisions NUCLEAR REACTIONS 12C(12C, γ), E=84 MeV/nucleon; 16O(16O, γ), E=80 MeV/nucleon; calculated σ(Eγ, θγ). TDHF.
doi: 10.1016/0375-9474(86)90371-4
1985CU01 Z.Phys. A320, 475 (1985) R.Y.Cusson, P.-G.Reinhard, M.R.Strayer, J.A.Maruhn, W.Greiner Density as a Constraint and the Separation of Internal Excitation Energy in TDHF NUCLEAR REACTIONS 16O(16O, 16O), E=1.56, 8 MeV/nucleon; calculated ion-ion distance, adiabatic potential, collective kinetic, internal energies vs initialization time. Time-dependent Hartree-Fock, density constraint.
doi: 10.1007/BF01415725
1985UM01 Phys.Rev. C32, 172 (1985) A.S.Umar, M.R.Strayer, R.Y.Cusson, P.-G.Reinhard, D.A.Bromley Time-Dependent Hartree-Fock Calculations of 4He + 14C, 12C + 12C(0+), and 4He + 20Ne Molecular Formations NUCLEAR REACTIONS 14C, 20Ne(α, α), 12C(12C, 12C), E ≈ Coulomb barrier; calculated composite system density contours, isoscalar quadrupole, octupole, isovector dipole moment frequency dependence; deduced dynamical degrees of freedom, associated classical frequencies. TDHF.
doi: 10.1103/PhysRevC.32.172
1984ST02 Phys.Lett. 135B, 261 (1984) M.R.Strayer, R.Y.Cusson, A.S.Umar, P.-G.Reinhard, D.A.Bromley, W.Greiner Time-Dependent Hartree-Fock Picture of Nuclear Molecular Resonances NUCLEAR STRUCTURE 18O; calculated isovector dipole, isocalar quadrupole, octupole molecular resonances. TDHF method.
doi: 10.1016/0370-2693(84)90387-3
1983SA04 Lett.Nuovo Cim. 36, 321 (1983) A.Sandulescu, R.Y.Cusson, W.Greiner Time-Dependent Hartree-Fock Study of Alpha Decay NUCLEAR REACTIONS 208Pb(α, α), E not given; calculated compound nuclear shapes during, after α-capture. TDHF.
1982RE05 Nucl.Phys. A378, 418 (1982) A Comparative Study of Hartree-Fock Iteration Techniques NUCLEAR STRUCTURE 16O; calculated total energy. Hartree-Fock iteration techniques.
doi: 10.1016/0375-9474(82)90458-4
1982ST06 Phys.Rev. C25, 1873 (1982) H.Stocker, L.P.Csernai, G.Graebner, G.Buchwald, H.Kruse, R.Y.Cusson, J.A.Maruhn, W.Greiner Jets of Nuclear Matter from High Energy Heavy Ion Collisions NUCLEAR REACTIONS 40Ca(40Ar, p), 238U(20Ne, p), E=393 MeV/nucleon; calculated σ(θ, E); deduced nuclear matter jet thrust angle vs impact parameter. Fluid dynamical model.
doi: 10.1103/PhysRevC.25.1873
1982ST10 Z.Phys. A306, 235 (1982) H.Stocker, R.Y.Cusson, H.J.Lustig, A.Gobbi, J.Hahn, J.A.Maruhn, W.Greiner Fusion-Fission, Superheavy Molecular-Capture and Symmetric Fragmentation in 3D-TDHF Calculations of Reactions 238U, 208Pb(4.6-8.0 MeV/u)64Ni, 48Ca NUCLEAR REACTIONS 238U, 208Pb(48Ca, X), (64Ni, X), E=4.6-8 MeV/nucleon; calculated σ(capture) vs E. 286Cn, 256No deduced formation impact parameters dependence. Three dimensional TDHF, heavy-ion asymmetric collisions.
1981CU04 Phys.Rev. C23, 1279 (1981) Isopin Mixing in 16O by use of Pion and Deuteron Probes NUCLEAR REACTIONS 16O(π+, π+'), E=164 MeV; calculated σ. 16O(d, t), E not given; calculated C2S. 16O levels deduced isopin matrix element. Euler angle representation.
doi: 10.1103/PhysRevC.23.1279
1981CU06 Phys.Rev. C23, 2524 (1981) R.Y.Cusson, J.Gomez del Campo, J.A.Maruhn, V.Maruhn-Rezwani Analysis of the 14N + 12C Heavy-Ion Reaction NUCLEAR REACTIONS 12C(14N, X), E=106, 167 MeV; calculated σ(fragment θ, E, Z), deflection, energy loss functions. TDHF, semiclassical scattering model, evaporation effects.
doi: 10.1103/PhysRevC.23.2524
1981ST06 Phys.Lett. 101B, 379 (1981) H.Stocker, R.Y.Cusson, J.A.Maruhn, W.Greiner Preequilibrium Nucleon Jets in TDHF Calculations of Medium-Energy, Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(12C, X), (197Au, X), E=30-85 MeV/nucleon; calculated constant density contours, fragment velocity, density vs Z. Three-dimensional TDHF.
doi: 10.1016/0370-2693(81)90156-8
1980CA15 Nucl.Phys. A341, 93 (1980) B.Castel, R.Y.Cusson, L.Zamick Isospin Mixing in 16O: A Three-Level Model NUCLEAR STRUCTURE 16O; calculated isospin mixing effects for 2- states. Three-level model.
doi: 10.1016/0375-9474(80)90363-2
1980CU04 Z.Phys. A294, 257 (1980) R.Y.Cusson, J.A.Maruhn, H.Stocker Collision of 238U + 238U Using a Three-Dimensional TDHF-BCS Model NUCLEAR REACTIONS 238U(238U, X), E=7.5 MeV/nucleon; calculated energy loss, deflection angle; deduced reaction mechanism properties. Three-dimensional time-dependent Hartree-Fock, BCS model.
doi: 10.1007/BF01438163
1980ST02 Z.Phys. A294, 125 (1980) H.Stocker, R.Y.Cusson, J.A.Maruhn, W.Greiner Medium Energy Collisions of Heavy Nuclei in the Three-Dimensional Nuclear Fluid Dynamical-(NFD) and Time-Dependent Hartree-Fock (TDHF) Models NUCLEAR REACTIONS Kr(Kr, X), E=20-200 MeV/nucleon; calculated σ for density isomers. time-dependent Hartree-Fock, three-dimensional nuclear fluid dynamic model.
1979CU01 Phys.Rev.Lett. 42, 694 (1979) Time-Dependent Hartree-Fock-Bogoliubov Calculations of Heavy-Element Fusion and Fission Phenomena NUCLEAR REACTIONS 118Pd(118Pd, X), E=637 MeV; calculated transition time from fusion to fission, fragment elongation parameter, distance of closest approach. Time-dependent Hartree-Fock-Bogoliubov method.
doi: 10.1103/PhysRevLett.42.694
1978CU06 Phys.Rev. C18, 2589 (1978) R.Y.Cusson, J.A.Maruhn, H.W.Meldner Direct Inelastic Scattering of 14N + 12C in a Three-Dimensional Time-Dependent Hartree-Fock Scheme NUCLEAR REACTIONS 12C(14N, X), E=112 MeV; 16O(16O, X), E=128 MeV; calculated deflection functions using time-dependent Hartree-Fock in 3-dimensional scheme, Skyrme interaction.
doi: 10.1103/PhysRevC.18.2589
1976CU01 Phys.Rev.Lett. 36, 1166 (1976) R.Y.Cusson, R.K.Smith, J.A.Maruhn Time-Dependent Hartree-Fock Calculation of the Reaction 16O + 16O in Three Dimensions NUCLEAR REACTIONS 16O(16O, X); calculated reaction parameters. Time-dependent Hartree-Fock.
doi: 10.1103/PhysRevLett.36.1166
1976CU03 Phys.Lett. 62B, 134 (1976) Dynamics of 12C + 12C in a Realistic Time-Dependent, Hartree-Fock Model NUCLEAR REACTIONS 12C(12C, X), E=1.6-12.8 MeV/A; calculated collision dynamics.
doi: 10.1016/0370-2693(76)90486-X
1976CU06 Phys.Rev. C14, 1615 (1976) R.Y.Cusson, H.P.Trivedi, H.W.Meldner, M.W.Weiss, R.E.Wright Self-Consistent K-Matrix-Model Calculation for Finite and Superheavy Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb, 298Fl; calculated total binding energies, rms radii, electron scattering form factors.
doi: 10.1103/PhysRevC.14.1615
1976CU07 Nucl.Phys. A270, 437 (1976) Realistic Heavy-Ion Adiabatic Potentials NUCLEAR STRUCTURE 8Be, 16O, 20Ne, 24Mg, 32S; calculated static adiabatic heavy-ion cluster potentials.
doi: 10.1016/0375-9474(76)90456-5
1976MA45 Nucl.Phys. A270, 471 (1976) Time-Dependent Hartree-Fock Calculation of 12C + 12C with a Realistic Potential NUCLEAR REACTIONS 12C(12C, X); calculated head-on scattering.
doi: 10.1016/0375-9474(76)90457-7
1974KO17 Phys.Rev. C10, 1529 (1974) D.Kolb, R.Y.Cusson, H.W.Schmitt Asymmetric Fission of 236U in a Self-Consistent K-Matrix Model NUCLEAR STRUCTURE, Fission 236U; calculated fission path, shape asymmetry, static total energy, single particle energies. Self-consistent Brueckner-Hartree-Fock method.
doi: 10.1103/PhysRevC.10.1529
1973CU03 Nucl.Phys. A211, 429 (1973) Nuclear Structure Studies of 20Ne and 24Mg in the Variation-after-Projection Hartree-Fock Method NUCLEAR REACTIONS 20Ne, 24Mg(e, e), (e, e'); calculated form factors. 20Ne, 24Mg calculated levels, J, π, quadrupole moment, B(E2), charge radii, γ-branching.
doi: 10.1016/0375-9474(73)90435-1
1973KO26 Nucl.Phys. A215, 1 (1973) Realistic Single-Particle K-Matrix for Deformed and Fissioning Nuclei NUCLEAR STRUCTURE 4He, 8Be, 12C, 16O, 20Ne, 28Si, 32S, 40,48Ca; calculated binding energies, single particle energies, quadrupole moment, rms radii.
doi: 10.1016/0375-9474(73)90096-1
1972CU03 Phys.Rev. C5, 2120 (1972) Fast and Accurate Solutions for Meldner's Realistic Single-Particle Hamiltonian NUCLEAR STRUCTURE 16O, 40Ca; calculated Coulomb energy, binding energy, rms proton radii. Meldner'S realistic single-particle Hamiltonian.
doi: 10.1103/PhysRevC.5.2120
1972KO28 Z.Phys. 253, 282 (1972) Gaussian Approximations for the Nuclear Coulomb Interaction
doi: 10.1007/BF01386162
1972LE10 Phys.Lett. 39B, 453 (1972) Practical Angular Momentum Projection Method in Multi-Shell Hartree-Fock Calculations; 22Na as an Example NUCLEAR STRUCTURE 22Na; calculated levels, B(E2), B(M1), T1/2, γ-mixing, γ-branching. Angular momentum projection from multi-shell Hartree-Fock model.
doi: 10.1016/0370-2693(72)90316-4
1972LE38 Phys.Rev.Lett. 29, 1525 (1972); Erratum Phys.Rev.Lett. 30, 153 (1973) Anticentrifugal Stretching in 20Ne NUCLEAR STRUCTURE 20Ne; calculated B(E2), ground-band energies vs mass quadrupole coupling parameter; analyzed rms radius vs state J. Variation-after-projection Hartree-Fock theory.
doi: 10.1103/PhysRevLett.29.1525
1971BI07 Phys.Lett. 35B, 303 (1971) E.G.Bilpuch, N.H.Prochnow, R.Y.Cusson, H.W.Newson, G.E.Mitchell Statistical Properties of 49V via Proton Resonance Reactions NUCLEAR REACTIONS 48Ti(p, p), (p, p'), E=1.8-3.1 MeV; measured σ(E). 49V deduced resonances, level spacing.
doi: 10.1016/0370-2693(71)90264-4
1971LE22 Nucl.Phys. A170, 439 (1971) The Nuclear Neutron-Proton rms Radius Difference NUCLEAR STRUCTURE 48Ca, 56Fe, 58Ni, 59Co, 60,62Ni, 90Zr, 120Sn; calculated binding energies, rms charge radii.
doi: 10.1016/0375-9474(71)90645-2
1970HA67 Can.J.Phys. 48, 240 (1970) Mutual Excitation and Reorientation of Target and Projectile in Coulomb Excitation NUCLEAR REACTIONS 24Mg(35Cl, 35Cl'), E=61 MeV; 62Ni(28Si, 28Si), E=68.5 MeV; calculated mutual excitation, reorientation effects on σ. Coulomb excitation.
1969CU04 Phys.Rev.Letters 23, 871 (1969) Istopic-Shift Parameters in the Nilsson Model NUCLEAR STRUCTURE Sm, Gd, Yb, U; calculated isotope shift.
doi: 10.1103/PhysRevLett.23.871
1969CU07 Can.J.Phys. 47, 2835 (1969) Octupole Transitions in 19F and Other s-d Shell Nuclei NUCLEAR STRUCTURE 16O, 19F, 20Ne; calculated E3 transition strengths.
doi: 10.1139/p69-347
1968CU01 Z.Physik 209, 428 (1968) Coupling of a Quasi-Particle to the Pairing Vibrations
doi: 10.1007/BF01380548
1966CU02 Nucl.Phys. 86, 481(1966) Levels in 11B from 7Li(α, α)7Li and 7Li(α, α')7Li*(0.48) NUCLEAR REACTIONS 7Li(α, α'), E = 1.6-12.0 MeV; measured σ(E; Eα', θ). 11B deduced levels, J, π. Enriched target.
doi: 10.1016/0029-5582(66)90492-5
1964CU03 Bull. Am. Phys. Soc. 9, No. 7, 703, B3 (1964) Elastic and Inelastic Scattering of α Particles by Li7 NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
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