NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = W.Norenberg Found 46 matches. 2006RO07 Int.J.Mod.Phys. E15, 362 (2006) Spinodal instabilities of hot and dilute nuclear droplet - isovector effects
doi: 10.1142/S0218301306004211
2005IV03 Phys.Rev.Lett. 95, 082501 (2005) Diabatic States from Nodal Structure Conservation NUCLEAR STRUCTURE 224Th; calculated single-particle energies and spreading widths vs deformation. Diabatic states, Woods-Saxon potential.
doi: 10.1103/PhysRevLett.95.082501
2005TO16 Part. and Nucl., Lett. 128, 43 (2005) V.D.Toneev, Yu.B.Ivanov, E.G.Nikonov, W.Norenberg, V.N.Russkikh Three-fluid relativistic hydrodynamics for heavy-ion collisions NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; calculated time evolution of energy density. 197Au(197Au, X), E=6, 8, 10.5 GeV/nucleon; calculated proton rapidity spectra vs impact parameter. Three-fluid model, comparisons with data.
2004RU01 Yad.Fiz. 67, 195 (2004); Phys.Atomic Nuclei 67, 199 (2004) V.N.Russkikh, Yu.B.Ivanov, E.G.Nikonov, W.Norenberg, V.D.Toneev Evolution of Baryon-Free Matter Produced in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), E=158 GeV/nucleon; 197Au(197Au, X), E=10.5 GeV/nucleon; calculated time evolution of energy density. Three-fluid hydrodynamic model.
doi: 10.1134/1.1644024
2004TO02 Eur.Phys.J. C 32, 399 (2004) V.D.Toneev, E.G.Nikonov, B.Friman, W.Norenberg, K.Redlich Strangeness production in nuclear matter and expansion dynamics
doi: 10.1140/epjc/s2003-01374-2
2002DE58 Eur.Phys.J. A 15, 375 (2002) Entrance channel potentials in the synthesis of the heaviest nuclei NUCLEAR REACTIONS 64Ni, 198Pt, 208Pb, 238U, 252Cf(58Fe, X), 198Pt, 208Pb, 238U, 244Pu, 248Cm, 252Cf(48Ca, X), 198Pt, 208Pb, 238U, 252Cf(50Ti, X), (54Cr, X), (64Ni, X), (70Zn, X), (78Ge, X), 198Pt, 208Pb(86Kr, X), 130,136Xe(124Sn, X), (136Xe, X), 150Nd(136Xe, X), (144Ce, X), 238U(42Ca, X), 238U, 252Cf(58Ni, X), (68Ni, X), (74Se, X), 198Pt, 238U, 252Cf(82Se, X), 244Pu, 248Cm, 252Cf(40Ca, X), 198Pt(40Ar, X), (96Zr, X), (100Mo, X), E not given; calculated semi-microscopic potentials, dependence on deformation, orientation. Implications for superheavy element production discussed.
doi: 10.1140/epja/i2002-10039-3
2002IV05 Acta Phys.Hung.N.S. 15, 117 (2002) Yu.B.Ivanov, E.G.Nikonov, W.Norenberg, A.A.Shanenko, V.D.Toneev Directed Flow of Baryons from High-Energy Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated directed flow, slope parameters, related features. Relativistic two-fluid model.
doi: 10.1556/APH.15.2002.1-2.6
2002NO06 Eur.Phys.J. A 14, 43 (2002) Stability and Instability of a Hot and Dilute Nuclear Droplet II. Dissipative Isoscalar Modes
doi: 10.1007/s10050-002-8788-z
2000NO09 Eur.Phys.J. A 9, 327 (2000) Stability and Instability of a Hot and Dilute Nuclear Droplet I. Adiabatic Isoscalar Modes
doi: 10.1007/s100500070017
1998AV02 Eur.Phys.J. A 3, 75 (1998) S.P.Avdeyev, V.A.Karnaukhov, W.D.Kuznetsov, L.A.Petrov, V.K.Rodionov, A.S.Zubkevich, H.Oeschler, O.V.Bochkarev, L.V.Chulkov, E.A.Kuzmin, A.Budzanovski, W.Karcz, M.Janicki, E.Norbeck, A.S.Botvina, W.A.Friedman, W.Norenberg, G.Papp Thermal Multifragmentation in p + Au Interactions at 2.16, 3.6 and 8.1 GeV Incident Energies NUCLEAR REACTIONS 197Au(p, X), E=2.16, 3.6, 8.1 GeV; measured intermediate mass fragments spectra, multiplicity, charge, angular distributions; deduced thermal multifragmentation. Intranuclear cascade model.
doi: 10.1007/s100500050149
1998FR17 Eur.Phys.J. A 3, 165 (1998) B.Friman, W.Norenberg, V.D.Toneev The Quark Condensate in Relativistic Nucleus-Nucleus Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=2-50 GeV/nucleon; calculated central baryon density time evolution. 197Au(197Au, X), E=2-100 GeV/nucleon; calculated central quark condensate time evolution, invariant 4-volume.
doi: 10.1007/s100500050163
1998NO14 Acta Phys.Pol. B29, 3259 (1998) Restoration of Chiral Symmetry in Nucleus-Nucleus Collisions Around 10 GeV/u NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated central density time evolution, quark condensate features.
1998WE10 Phys.Lett. 433B, 236 (1998) W.Weinhold, B.Friman, W.Norenberg Thermodynamics of Δ Resonances NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; analyzed π0 spectrum; deduced Δ-decay contribution.
doi: 10.1016/S0370-2693(98)00639-X
1997DE41 Phys.Lett. 409B, 51 (1997) C.Deutsch-Sauermann, B.Friman, W.Norenberg η-Meson Photoproduction Off Protons and Deuterons NUCLEAR REACTIONS 1H(γ, X), E=700-1000 MeV; 2H(γ, X), E=600-1100 MeV; analyzed η production σ; deduced reaction mechanism related features. Unitary, gauge-invariant model with coupled channels.
doi: 10.1016/S0370-2693(97)00886-1
1995SA14 Phys.Lett. 341B, 261 (1995) Ch.Sauermann, B.L.Friman, W.Norenberg Resonance Model for πN Scattering and (Eta)-Meson Production in the S11 Channel NUCLEAR REACTIONS 1H(π-, X), E ≈ 0.65-1.05 GeV/c; calculated σ vs momentum for eta production. Resonance πN scattering model.
doi: 10.1016/0370-2693(94)01372-J
1994AY01 Nucl.Phys. A578, 640 (1994) S.Ayik, Y.B.Ivanov, V.N.Russkikh, W.Norenberg Stochastic Multi-Fluid Models for Intermediate-Energy Heavy-Ion Collisions
doi: 10.1016/0375-9474(94)90765-X
1994RH01 Phys.Rev. C49, 250 (1994) M.Rhein, R.Barth, E.Ditzel, H.Feldmeier, E.Kankeleit, V.Lips, C.Muntz, W.Norenberg, H.Oeschler, A.Piechaczek, W.Polai, I.Schall Elastoplasticity in Dissipative Heavy-Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), E=12 MeV/nucleon; measured δ-electron spectra in coincidence with elastic, dissipative collisions; deduced time evolution of nuclear reactions, deceleration and contact times. Elastoplastic properties of nuclear matter.
doi: 10.1103/PhysRevC.49.250
1994SC10 Nucl.Phys. A572, 112 (1994) M.Schonhofen, M.Cubero, B.L.Friman, W.Norenberg, Gy.Wolf Convariant Kinetic Equations and Relaxation Processes in Relativistic Heavy-Ion Collions
doi: 10.1016/0375-9474(94)90424-3
1993KU01 Phys.Lett. 298B, 273 (1993) Effect of Angular-Momentum Dissipation and Fluctuation on Energy Coherence Lengths and Time Evolution in the Dissipative Collision 28Si + 48Ti NUCLEAR REACTIONS 48Ti(28Si, X), E=130 MeV; analyzed average σ(fragment θ, E) for fragment Z=11, 12; deduced angular momentum dissipation, fluctuation role.
doi: 10.1016/0370-2693(93)91819-9
1992KU09 Z.Phys. A343, 215 (1992) The Effect of Angular-Momentum Dissipation on Fluctuations of Excitation Functions in Heavy-Ion Collisions NUCLEAR REACTIONS 48Ti(28Si, X), E=130 MeV; analyzed σ(fragment θ, E) for fragment Z=12, energy autocorrelation; deduced relative angular momentum dissipation, fluctuations role in rotating dinuclear system time-angle localization.
doi: 10.1007/BF01291826
1989BE24 Nucl.Phys. A499, 609 (1989) D.Berdichevsky, A.Lukasiak, W.Norenberg, P.Rozmej Diabatic Shifts and Fluctuations of Heavy-Ion Fusion Barriers NUCLEAR REACTIONS 124Sn(96Zr, 96Zr), E not given; calculated adiabatic, diabatic interaction potential parameter vs inter-ion distance. 90Zr(90Zr, X), 100Mo(100Mo, X), E(cm)=170-250 MeV; calculated fusion probability vs E. Collective motion, diabatic approach. Other reactions studied.
doi: 10.1016/0375-9474(89)90548-4
1989BE39 Nucl.Phys. A502, 395c (1989) D.Berdichevsky, A.Lukasiak, W.Norenberg, P.Rozmej Diabatic Hindrance of Heavy-Ion Fusion NUCLEAR REACTIONS 100Mo(100Mo, X), E(cm)=175-250 MeV; 90Zr(90Zr, X), E ≈ 170-250 MeV; calculated fusion probability vs E. Other reactions investigated. Collective nuclear motion, diabatic approach.
doi: 10.1016/0375-9474(89)90678-7
1989MI19 Z.Phys. A334, 233 (1989) B.Milek, W.Norenberg, P.Rozmej Quantum Chaos in the Two-Center Shell Model NUCLEAR REACTIONS 208Pb(208Pb, X), E not given; calculated composite system level spacing vs two-center distance. Two-center shell model.
1988HE18 Nucl.Phys. A489, 421 (1988) Evaporation of Particles from Hot Nuclei NUCLEAR STRUCTURE 133Cs; calculated neutron, proton evaporation spectra. Hot nucleus model.
doi: 10.1016/0375-9474(88)90004-8
1987HE17 Nucl.Phys. A473, 342 (1987) Z.He, P.Rozmej, J.Wu, W.Norenberg Sharing of Excitation Energy in Dissipative Nucleus-Nucleus Collisions NUCLEAR REACTIONS 147Sm, 238U(98Mo, X), E at 14.7 MeV/nucleon; calculated light, heavy fragment, total excitation energy. Dissipative collisions.
doi: 10.1016/0375-9474(87)90149-7
1987LU01 Z.Phys. A326, 79 (1987) Dissipative Diabatic Dynamics of Nucleus-Nucleus Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), 90Zr(90Zr, X), E=0.1-5 MeV/nucleon; calculated adiabatic potential, stiffness parameter, composite system deformation, quadrupole moment, collective kinetic energy, intrinsic excitation energy, total energy time evolutions. Dissipative diabatic approach.
1986GE02 Z.Phys. A323, 293 (1986) Diabatic Emission of Neutrons and Protons in Central Nucleus-Nucleus Collisions NUCLEAR REACTIONS 40Ca(40Ca, xn), (40Ca, xp), E=13.4 MeV/nucleon; 58Ni(58Ni, xn), (58Ni, xp), E=14.4 MeV/nucleon; 92Mo(92Mo, xn), (92Mo, xp), E=15.5 MeV/nucleon; calculated diabatically emitted nucleon σ(θ), multiplicities. Central collisions.
1986GE09 Nucl.Phys. A459, 77 (1986) Temperature-Dependent Optical Potential and Mean Free Path Based on Skyrme Interactions NUCLEAR REACTIONS 40Ca, 208Pb(n, n), E=10, 30, 50 MeV; calculated real, imaginary parts of optical potential, mean free path vs E, temperature, separation distance. Effective Skyrme interactions.
doi: 10.1016/0375-9474(86)90057-6
1986RO19 Phys.Lett. 177B, 278 (1986) Quasi-Elastic Recoil in Central Nucleus-Nucleus Collisions NUCLEAR REACTIONS 124Sn(208Pb, 208Pb), E=0.1-5 MeV/nucleon; calculated kinetic, potential, excitation energies, interaction times. Dissipative diabatic dynamics.
doi: 10.1016/0370-2693(86)90752-5
1984CA37 Nucl.Phys. A431, 558 (1984) Diabatic Emission of Neutrons: A Probe for the Energy-Dissipation Mechanism in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 92Mo(92Mo, xn), E=7.5-20 MeV/nucleon; calculated nucleus-nucleus potential, neutron multiplicity vs En. Dissipative diabatic dynamics.
doi: 10.1016/0375-9474(84)90123-4
1984LU08 Nucl.Phys. A426, 181 (1984) A.Lukasiak, W.Cassing, W.Norenberg The Diabatic Two-Center Shell Model NUCLEAR REACTIONS 92Mo(92Mo, X), 166Er(86Kr, X), E ≈ 15 MeV/nucleon; calculated diabatic potential parameters, associated mass tensor. Dissipative diabatic dynamics, two-center shell model.
doi: 10.1016/0375-9474(84)90072-1
1983CA26 Z.Phys. A314, 309 (1983) W.Cassing, A.K.Dhar, A.Lukasiak, W.Norenberg Diabatic Aspects of Single-Particle Motion within the Time-Dependent Hartree-Fock Theory NUCLEAR REACTIONS 166Er(86Kr, X), E=8.2-20 MeV/nucleon; calculated potential energy, diabatic neutron potential vs relative distance, mean field. TDHF, diabatic single particle motion.
doi: 10.1007/BF01412927
1982DA08 Nucl.Phys. A378, 189 (1982) M.Dakowski, A.Gobbi, W.Norenberg Influence of Single-Particle Shell Structure on the Energy Dissipation in Heavy-Ion Collisions NUCLEAR REACTIONS 144Sm(144Sm, X), E=1000 MeV; 154Sm(154Sm, X), E=970 MeV; 56Fe, 165Ho, 209Bi(56Fe, X), E=8.3 MeV/nucleon; calculated total kinetic energy loss, mass variance correlation; deduced shell effects. Statistical model, random transfers, excitations.
doi: 10.1016/0375-9474(82)90390-6
1982ME14 Z.Phys. A308, 315 (1982) Microscopic Transport Theory of Heavy-Ion Collisions. V. Transfer of Neutrons and Protons NUCLEAR REACTIONS 166Er(86Kr, X), E=515, 619, 703 MeV; 209Bi(136Xe, X), E=900, 1130 MeV; 209Bi(84Kr, X), E=712 MeV; 208Pb(208Pb, X), E=1456, 1560 MeV; 120Sn(136Xe, X), E=779 MeV; 238U(208Pb, X), E=1560 MeV; 238U(238U, X), E=1766 MeV; calculated nucleon transfer diffusion coefficients. 144Sm(144Sm, X), E=1000 MeV; 154Sm(154Sm, X), E=970 MeV; 238U, 165Ho, 56Fe(56Fe, X), E=464 MeV; calculated nucleon transfer diffusion coefficient moments vs total kinetic energy. Microscopic transport theory.
doi: 10.1007/BF01415880
1981ME07 Phys.Lett. 104B, 15 (1981) Neutron and Proton Diffusion in Heavy-Ion Collisions NUCLEAR REACTIONS 165Ho(56Fe, X), E=464 MeV; 56Fe(129Xe, X), E=775 MeV; calculated fragment mass distribution width vs total kinetic energy; 197Au(132Xe, X), E=900 MeV; calculated fragment charge distribution vs total kinetic energy. Statistical theory, neutron, proton exchange.
doi: 10.1016/0370-2693(81)90844-3
1979NO02 Z.Phys. A290, 335 (1979) Entrance-Channel Coherence in Dissipative Heavy-Ion Collisions and Compound-Nucleus Formation NUCLEAR REACTIONS Pb(Ar, X), E=400 MeV; calculated trajectories for different L in d-α plane, d is distance between fragments, α is mass asymmetry. Fokker-Planck equation, Moller-Nix adiabatic potential; deduced criteria for entrance-channel coherence, compound nucleus formation.
1979RI04 Z.Phys. A290, 47 (1979) C.Riedel, G.Wolschin, W.Norenberg Relaxation Times in Dissipative Heavy-Ion Collisions NUCLEAR REACTIONS 166Er(86Kr, X), E=5.99, 8.18 MeV/nucleon; 209Bi(136Xe, X), E=8.31, 6.62 MeV/nucleon; calculated relaxation times for dissipation of radial kinetic energy, relative angular momentum, development of deformations. Classical model for dissipative HI collisions; deduced empirical mass transport coefficients.
doi: 10.1007/BF01408479
1979RI10 Z.Phys. A290, 385 (1979) Theoretical Estimates for the Production of Transuranium Elements in Heavy-Ion Collisions NUCLEAR REACTIONS 238U(238U, X), E=75 MeV/amu; measured nothing; analyzed data; deduced production σ of superheavy elements, probability distributions of E, spins as function of fragment Z. Diffusion model for dissipative HI collisions.
doi: 10.1007/BF01408400
1978WO12 Phys.Rev.Lett. 41, 691 (1978) Angular-Momentum Dissipation in Heavy-Ion Collisions NUCLEAR REACTIONS 166Er(86Kr, X), E=5.99 MeV/nucleon; calculated γ-multiplicity.
doi: 10.1103/PhysRevLett.41.691
1976AY01 Z.Phys. A279, 145 (1976) S.Ayik, B.Schurmann, W.Norenberg Microscopic Transport Theory of Heavy-Ion Collisions. II. Transport Coefficients for Asymmetric Fragmentation and Generalized Einstein Relations NUCLEAR REACTIONS 58Ni(16O, X), E=92 MeV; 50Ti(32S, X), E=131, 161 MeV; 197Au(40Ar, X), E=288, 340 MeV; 165Ho(84Kr, X), E=714 MeV; 197Au(63Cu, X), E=365, 443 MeV; 232Th(40Ar, X), E=279, 388 MeV; calculated transport coefficients.
doi: 10.1007/BF01437870
1974BO13 Phys.Lett. 49B, 227 (1974) Molecular Orbitals and Multiple Transfer in the Elastic Collision of 16O on 17O NUCLEAR REACTIONS 17O(16O, 16O), E=32 MeV; measured nothing, calculated σ(θ).
doi: 10.1016/0370-2693(74)90419-5
1974NO11 Phys.Lett. 52B, 289 (1974) Transport Phenomena in Multi-Nucleon Transfer Reactions NUCLEAR REACTIONS 232Th(40Ar, X), E=297, 388 MeV; calculated σ.
doi: 10.1016/0370-2693(74)90043-4
1973VO04 Nucl.Phys. A207, 113 (1973) Theory of Particle and Hole Transfer in Elastic Nucleus-Nucleus Scattering NUCLEAR REACTIONS 12C(13C, 13C), (14C, 14C), 13C(14C, 14C); calculated σ(θ), particle, hole transfer.
doi: 10.1016/0375-9474(73)90026-2
1969KO28 Nucl.Phys. A139, 513 (1969) E.Konecny, W.Norenberg, H.W.Schmitt Fragment Energy Correlation Measurements for the Proton Induced Fission of 226Ra NUCLEAR REACTIONS, Fission 226Ra(p, F), E=9, 11, 13 MeV; measured mass yield, average kinetic energy, variance of total kinetic energy.
doi: 10.1016/0375-9474(69)90275-9
1969RA39 Nucl.Phys. A136, 465 (1969) J.O.Rasmussen, W.Norenberg, H.J.Mang A model for calculating the angular momentum distribution of fission fragments NUCLEAR REACTIONS 239Pu(n, F)108Ru, E thermal; calculated distribution of rotational angular momenta in primary fission fragments with A=108.
doi: 10.1016/0375-9474(69)90066-9
1964NO11 Z.Angew.Phys. 17, 452 (1964) Magnetfeldregelung Eines Betaspektrometers. Konversionsspektrum und Konversionsverhaltnisse des 79, 51 keV - und 88, 97 keV - Ubergangs von Gd 158 und Gd 156 NUCLEAR STRUCTURE 158Gd, 156Gd; measured not abstracted; deduced nuclear properties.
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