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Search: Author = W.Norenberg

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2006RO07      Int.J.Mod.Phys. E15, 362 (2006)

P.Rozmej, W.Norenberg, G.Papp

Spinodal instabilities of hot and dilute nuclear droplet - isovector effects

doi: 10.1142/S0218301306004211
Citations: PlumX Metrics

2005IV03      Phys.Rev.Lett. 95, 082501 (2005)

F.A.Ivanyuk, W.Norenberg

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2002DE58      Eur.Phys.J. A 15, 375 (2002)

V.Yu.Denisov, W.Norenberg

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
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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
Citations: PlumX Metrics

2002NO06      Eur.Phys.J. A 14, 43 (2002)

W.Norenberg, G.Papp, P.Rozmej

Stability and Instability of a Hot and Dilute Nuclear Droplet II. Dissipative Isoscalar Modes

doi: 10.1007/s10050-002-8788-z
Citations: PlumX Metrics

2000NO09      Eur.Phys.J. A 9, 327 (2000)

W.Norenberg, G.Papp, P.Rozmej

Stability and Instability of a Hot and Dilute Nuclear Droplet I. Adiabatic Isoscalar Modes

doi: 10.1007/s100500070017
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1993KU01      Phys.Lett. 298B, 273 (1993)

S.Yu.Kun, W.Norenberg, M.Papa

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
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1992KU09      Z.Phys. A343, 215 (1992)

S.Yu.Kun, W.Norenberg

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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)

Z.He, J.Wu, W.Norenberg

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
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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
Citations: PlumX Metrics

1987LU01      Z.Phys. A326, 79 (1987)

A.Lukasiak, W.Norenberg

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)

L.X.Ge, W.Norenberg

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)

L.Ge, Y.Zhuo, W.Norenberg

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
Citations: PlumX Metrics

1986RO19      Phys.Lett. 177B, 278 (1986)

P.Rozmej, W.Norenberg

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
Citations: PlumX Metrics

1984CA37      Nucl.Phys. A431, 558 (1984)

W.Cassing, W.Norenberg

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
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

1982ME14      Z.Phys. A308, 315 (1982)

A.C.Merchant, W.Norenberg

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
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1981ME07      Phys.Lett. 104B, 15 (1981)

A.C.Merchant, W.Norenberg

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
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1979NO02      Z.Phys. A290, 335 (1979)

W.Norenberg, C.Riedel

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
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1979RI10      Z.Phys. A290, 385 (1979)

C.Riedel, W.Norenberg

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
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1978WO12      Phys.Rev.Lett. 41, 691 (1978)

G.Wolschin, W.Norenberg

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
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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
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1974BO13      Phys.Lett. 49B, 227 (1974)

H.G.Bohlen, W.Norenberg

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
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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
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1973VO04      Nucl.Phys. A207, 113 (1973)

W.von Oertzen, W.Norenberg

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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2428.

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
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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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