NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = R.W.Hasse Found 19 matches. 1988JA13 Phys.Lett. 214B, 1 (1988) J.Jaenicke, P.Schuck, R.W.Hasse The Missing Charge Problem in the Longitudinal Response and the Importance of Two-Particle-Two-Hole States NUCLEAR STRUCTURE 12C, 40Ca, 56Fe, 238U; calculated longitudinal response function. RPA, 2p-2h states.
doi: 10.1016/0370-2693(88)90441-8
1987JA14 J.Phys.(Paris), Colloq.C-2, 71 (1987) J.Jaenicke, P.Schuck, U.Stroth, R.W.Hasse On the Longitudinal Charge Response in the Quasi Elastic Peak Region NUCLEAR REACTIONS 12C, 56Fe, 238U(e, e'), E not given; analyzed longitudinal charge response data; deduced 2p2h level densities vs mass number, missing charge persistence.
1987ST02 Nucl.Phys. A462, 45 (1987) On the Nuclear Longitudinal Charge Response in the Quasi-Elastic Peak Region NUCLEAR REACTIONS 12C, 40Ca, 56Fe(e, e'), E not given; calculated charge responses. 40Ca, 56Fe deduced missing charge problem, isovector channel role. Semi-classical RPA approach.
doi: 10.1016/0375-9474(87)90378-2
1986HA40 Phys.Lett. 179B, 313 (1986) Correlation Effects on the Level Density of a Hot Nucleus NUCLEAR STRUCTURE A=160; calculated effective mass, level density parameter vs temperature.
doi: 10.1016/0370-2693(86)90483-1
1986HA43 Phys.Lett. 181B, 5 (1986) R.W.Hasse, B.L.Friman, D.Berdichevsky The Influence of Ground State Correlations on Nuclear Densities NUCLEAR STRUCTURE 208Pb, 200Hg, 116,124Sn, 90Zr, 58Ni, 58Fe; calculated occupation numbers, charge, neutron densities, proton, charge rms radii. Semi-classical approximation.
doi: 10.1016/0370-2693(86)91243-8
1986MO23 Z.Phys. A325, 357 (1986) M.Montoya, R.W.Hasse, P.Koczon Coulomb Effects in Low Energy Fission NUCLEAR REACTIONS 234,236U(n, F), E=low; analyzed cold fission fragment charge, total kinetic energy distributions, yield data; deduced Coulomb effects role in fission. Static scission model.
1985HA09 Nucl.Phys. A438, 157 (1985) The Imaginary Part of the Nucleon-Nucleus Optical Potential in Semiclassical Approximation NUCLEAR REACTIONS 40Ca, 208Pb(n, n), E not given; calculated nucleon-nucleus imaginary potential parameter characteristics. Semi-classical approximation.
doi: 10.1016/0375-9474(85)90123-X
1985ST09 Phys.Lett. 156B, 291 (1985) U.Stroth, R.W.Hasse, P.Schuck, W.M.Alberico, A.Molinari, M.Ericson On the Nuclear Isovector Spin Response in the Quasielastic Peak Region NUCLEAR REACTIONS 208Pb(p, p'), E not given; calculated longitudinal, transverse nuclear response. Nonlocal mean field plus particle-hole interactions. NUCLEAR STRUCTURE 40Ca; calculated structure function. 48Ca, 12C; calculated transverse nuclear response function.
doi: 10.1016/0370-2693(85)91611-9
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
1984HA15 Nucl.Phys. A417, 351 (1984) Wave Packet Scattering Model with Quantum Friction for Heavy-Ion Collisions NUCLEAR REACTIONS 159Tb(11B, X), E=51 MeV; calculated fusion, deep-inelastic scattering probabilities vs (L), classical, quantum mechanical deflection functions. Wave packet scattering model.
doi: 10.1016/0375-9474(84)90512-8
1983TR15 J.Phys.(Paris), Lett. 44, L-733 (1983) J.Treiner, R.W.Hasse, P.Schuck Fission from Saddle to Exit: Influence of curvature and compression energies NUCLEAR STRUCTURE 240Pu; calculated potential energy surfaces, fission saddle, scission energies vs curvature energy coefficients. Energy density formalism, comparison with liquid drop model.
doi: 10.1051/jphyslet:019830044017073300
1982HA23 Phys.Rev. C25, 2771 (1982) R.W.Hasse, G.Ghosh, J.Winter, A.Lumbroso Isoscalar Giant-Resonance Energies and Long-Mean-Free Path Nuclear Fluid Dynamics NUCLEAR STRUCTURE A ≈ 60-220; calculated giant monopole resonance energies. Fluid dynamic approach.
doi: 10.1103/PhysRevC.25.2771
1982HA48 Phys.Rev. C26, 1667 (1982) Nuclear Fluid Dynamics with Long-Mean-Free Path Dissipation: Multipole vibrations and isoscalar giant resonance widths NUCLEAR STRUCTURE A ≈ 50-200; calculated T=0 giant resonance widths. Fluid dynamics approach.
doi: 10.1103/PhysRevC.26.1667
1981DI03 Nucl.Phys. A355, 66 (1981) M.Diebel, K.Albrecht, R.W.Hasse Microscopic Calculations of Fission Barriers and Critical Angular Momenta for Excited Heavy Nuclear Systems NUCLEAR STRUCTURE 270Ds, 278Ds, 298Fl, 292Og, 322128; calculated fission barriers, critical angular momenta. Extended Strutinsky macro-microscopic method, BCS pairing.
doi: 10.1016/0375-9474(81)90132-9
1974HA46 Nucl.Phys. A229, 141 (1974) A Two-Nucleus Shell Model with Pairing for the Calculation of Molecular Heavy-Ion or Fission Potentials NUCLEAR STRUCTURE 118Pd; calculated normalized density distribution of paired nuclei.
doi: 10.1016/0375-9474(74)90681-2
1973HA19 Phys.Lett. 44B, 26 (1973) Temperature Effects in the Liquid Drop Description of Nuclear Fission NUCLEAR STRUCTURE 238U calculated deformation energy, fission barrier.
doi: 10.1016/0370-2693(73)90290-6
1972HA65 Phys.Lett. 41B, 264 (1972) Talmi Integrals and Effective Interaction
doi: 10.1016/0370-2693(72)90574-6
1971HA33 Phys.Rev. C4, 572 (1971) Fission of Heavy Nuclei at Higher Excitation Energies in a Dynamic Model NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; calculated fragment mass, energy distributions. Dynamic model.
doi: 10.1103/PhysRevC.4.572
1971HA65 Ann.Phys.(New York) 68, 377 (1971) Studies in the Shape Dependence of the Droplet Model of Nuclei (Curvature and Compressibility Effects)
doi: 10.1016/0003-4916(71)90129-1
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