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NSR database version of March 21, 2024.

Search: Author = J.A.Maruhn

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2017IS16      Phys.Rev. C 96, 064616 (2017)

C.Ishizuka, M.D.Usang, F.A.Ivanyuk, J.A.Maruhn, K.Nishio, S.Chiba

Four-dimensional Langevin approach to low-energy nuclear fission of 236U

NUCLEAR REACTIONS 235U(n, F), E=14 MeV; 257Fm(n, F), E=thermal; calculated mass distribution of fission fragments, fission events on the mass-TKE plane, TKE distributions. 235U(n, F), E=0.5, 3.5, 5.5, 8.5, 13.5 MeV; calculated TKE of fission fragments, contour map of prescission kinetic energy as a function of mass number of fission fragments, distribution of deformation parameter in its dependence on the mass number. Four-dimensional (4D) Langevin model with infinite-depth two-center shell-model (TCSM) potential and the finite-depth two-center Woods-Saxon (TCWS) potential. Comparison with experimental data in JENDL/FPY-2011 data library.

doi: 10.1103/PhysRevC.96.064616
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2016RE07      Phys.Rev. C 93, 044618 (2016)

P.-G.Reinhard, A.S.Umar, P.D.Stevenson, J.Piekarewicz, V.E.Oberacker, J.A.Maruhn

Sensitivity of the fusion cross section to the density dependence of the symmetry energy

NUCLEAR REACTIONS 48Ca(48Ca, X)96Zr*, E(cm)=45-65 MeV; calculated folding model ion-ion interaction potentials, fusion σ(E). Impact of nuclear fusion on the nuclear equation of state (EOS). 48Ca; calculated Neutron root-mean-square radius (rms), neutron diffraction radius, and neutron halo. Dynamic microscopic method based on density-constrained time-dependent Hartree-Fock (DC-TDHF) approach, and direct TDHF study of barrier cross sections using a family of Skyrme parametrization.

doi: 10.1103/PhysRevC.93.044618
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2015IW01      Phys.Rev. C 92, 011303 (2015)

Y.Iwata, T.Ichikawa, N.Itagaki, J.A.Maruhn, T.Otsuka

Examination of the stability of a rod-shaped structure in 24Mg

NUCLEAR STRUCTURE 24Mg; calculated density profiles of the initial states of six-α clusters, contours of final states of compact shape, rod shape, and fragmentation, comparison of energies with and without the spin-orbit interaction as a function of rotational frequency; deduced rod-shaped structure of 24Mg with large angular momentum as a metastable stationary state. Cranked Hartree-Fock calculation with several different Skyrme-type interactions.

doi: 10.1103/PhysRevC.92.011303
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2015SC04      Phys.Rev. C 91, 025801 (2015)

B.Schuetrumpf, M.A.Klatt, K.Iida, G.E.Schroder-Turk, J.A.Maruhn, K.Mecke, P.-G.Reinhard

Appearance of the single gyroid network phase in "nuclear pasta" matter

doi: 10.1103/PhysRevC.91.025801
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2015UM03      Phys.Rev. C 92, 025808 (2015)

A.S.Umar, V.E.Oberacker, C.J.Horowitz, P.-G.Reinhard, J.A.Maruhn

Swelling of nuclei embedded in neutron-gas and consequences for fusion

NUCLEAR REACTIONS 28O(28O, X), E(cm)=2-14 MeV; 60Ca(60Ca, X), E(cm)=34-58 MeV; calculated pycnonuclear fusion cross sections and Astrophysical S factor as a function of external neutron-gas density, up to 500 neutrons for 28O and 1040 for 60Ca using Sao Paulo potential and incoming wave boundary condition (IWBC) method. Relevance to study of fusion of neutron rich nuclei at radioactive ion beam facilities, and to the study of composition and heating of the crust of accreting neutron stars.

doi: 10.1103/PhysRevC.92.025808
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2014IC01      Phys.Rev. C 89, 011305 (2014)

T.Ichikawa, K.Matsuyanagi, J.A.Maruhn, N.Itagaki

Pure collective precession motion of a high-spin torus isomer

NUCLEAR STRUCTURE 40Ca; calculated time-evolution of the density distribution, total angular momentum, tilting angle, and rotational angle of precession motion of the high-K torus isomer. Three-dimensional time-dependent Hartree-Fock (TDHF) method, and random-phase approximation (RPA) method for high-spin states.

doi: 10.1103/PhysRevC.89.011305
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2014IC02      Phys.Rev. C 90, 034314 (2014)

T.Ichikawa, K.Matsuyanagi, J.A.Maruhn, N.Itagaki

High-spin torus isomers and their precession motions

NUCLEAR STRUCTURE 36Ar, 40Ca, 44Ti, 48Cr, 52Fe; calculated density distributions, moments of inertia, single-particle energies, time evolution of the precession motion, Nilsson diagrams for high-spin torus isomers. Cranked three-dimensional Hartree-Fock (TDHF) method with Skyrme interactions and radially displaced harmonic-oscillator (RDHO) model.

doi: 10.1103/PhysRevC.90.034314
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2014JI17      Phys.Rev. C 90, 064618 (2014)

X.Jiang, J.A.Maruhn, S.Yan

Microscopic study of noncentral effects in heavy-ion fusion reactions with spherical nuclei

NUCLEAR REACTIONS 16O(16O, X), E(cm)=12, 20 MeV; 40Ca(40Ca, X), E(cm)=56, 58, 60, 70, 100, 48-75 MeV; 90Zr(40Ca, X), E(cm)=100, 110, 120, 180, 300 MeV; calculated time evolution of the moment of inertia for 16O+16O reaction, time evolution of the quadrupole moments, penetration probability as a function of impact parameter, and fusion σ(E) for 40Ca+40Ca reaction, N-N potentials and collective kinetic energies, effective mass parameters for head-on collisions and for various impact parameters. Three dimensional time-dependent Hartree-Fock approach (TDHF) with and without density constraint. Comparison with available experimental data.

doi: 10.1103/PhysRevC.90.064618
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2014SC25      Phys.Rev. C 90, 055802 (2014)

B.Schuetrumpf, K.Iida, J.A.Maruhn, P.-G.Reinhard

Nuclear ``pasta matter" for different proton fractions

doi: 10.1103/PhysRevC.90.055802
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2013JI17      Phys.Rev. C 88, 044611 (2013)

X.Jiang, S.Yan, J.A.Maruhn

Dynamics of energy dissipation in heavy-ion fusion reactions

NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=55, 100 MeV; 64Ni(64Ni, X), E(cm)=95, 190 MeV; 90Zr(90Zr, X), E(cm)=195, 300 MeV; 120Sn(120Sn, X), E(cm)=300, 500 MeV; calculated relative distance, quadrupole moment, nuclear stopping power as function of time, dynamic interaction potentials, dynamic reduced mass parameters, friction coefficients, relative distance dependence of the nucleons transferred, energies dissipated. Role of nucleon-nucleon two-body collisions in energy dissipation. Improved quantum molecular dynamics (ImQMD) model.

doi: 10.1103/PhysRevC.88.044611
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2013KL03      J.Phys.:Conf.Ser. 445, 012036 (2013)

M.A.Klatt, T.Ichikawa, K.Iida, N.Itagaki, J.A.Maruhn, K.Matsuyanagi, K.Mecke, S.Ohkubo, P.-G.Reinhard, B.Schuetrumpf

Exotic cluster structures in the mean-field theory

NUCLEAR STRUCTURE 16O, 40Ca; calculated deformation, exotic shapes using Skyrme Hartree-Fock, TDHF.

doi: 10.1088/1742-6596/445/1/012036
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2013SC09      Phys.Rev. C 87, 055805 (2013)

B.Schuetrumpf, M.A.Klatt, K.Iida, J.A.Maruhn, K.Mecke, P.-G.Reinhard

Time-dependent Hartree-Fock approach to nuclear "pasta" at finite temperature

doi: 10.1103/PhysRevC.87.055805
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2012IC04      Phys.Rev.Lett. 109, 232503 (2012)

T.Ichikawa, J.A.Maruhn, N.Itagaki, K.Matsuyanagi, P.-G.Reinhard, S.Ohkubo

Existence of an Exotic Torus Configuration in High-Spin Excited States of 40Ca

NUCLEAR STRUCTURE 40Ca; calculated high-spin states, J, π, neutron single-particle energies; deduced stable state with thorus configuration. Skyrme Hartree-Fock method, comparison with available data.

doi: 10.1103/PhysRevLett.109.232503
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2012LO10      Phys.Rev. C 86, 024608 (2012)

N.Loebl, A.S.Umar, J.A.Maruhn, P.-G.Reinhard, P.D.Stevenson, V.E.Oberacker

Single-particle dissipation in a time-dependent Hartree-Fock approach studied from a phase-space perspective

NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=160, 200, 240 MeV; calculated β and γ deformation parameter, quadrupole moment, and volume phase-space global observables in momentum and coordinate space using the time-dependent Hartree-Fock (TDHF) theory and the Wigner distribution function in the full six-dimensional phase space. Significance of extra time-odd terms.

doi: 10.1103/PhysRevC.86.024608
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2012OB02      Phys.Rev. C 85, 034609 (2012)

V.E.Oberacker, A.S.Umar, J.A.Maruhn, P.-G.Reinhard

Dynamic microscopic study of pre-equilibrium giant resonance excitation and fusion in the reactions 132Sn + 48Ca and 124Sn + 40Ca

NUCLEAR REACTIONS 132Sn(48Ca, X), 124Sn(40Ca, X), E(cm)=130 MeV; calculated time evolution of isoscalar quadrupole moment, deformation parameter and rms charge radius, isovector quadrupole moment, dipole amplitude, neutron leakage, pre-equilibrium dipole radiation spectrum, total fusion cross sections, heavy-ion potential, microscopic mass parameter. Pre-equilibrium Giant dipole resonance (GDR) excitation. Density-constrained time-dependent Hartree-Fock (TDHF) method. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.034609
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2012UM01      Phys.Rev. C 85, 017602 (2012)

A.S.Umar, V.E.Oberacker, J.A.Maruhn, P.-G.Reinhard

Microscopic composition of ion-ion interaction potentials

NUCLEAR REACTIONS 16O(16O, X), (24O, X), E(cm)=12 MeV; 40Ca(40Ca, X), E(cm)=55 MeV; 132Sn(48Ca, X), E(cm)=120 MeV; calculated ion-ion interaction potentials for head-on collisions using TDHF approach for the time evolution of the nuclear collision.

doi: 10.1103/PhysRevC.85.017602
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2011IC04      Phys.Rev.Lett. 107, 112501 (2011)

T.Ichikawa, J.A.Maruhn, N.Itagaki, S.Ohkubo

Linear Chain Structure of Four-α Clusters in 16O

NUCLEAR STRUCTURE 16O; calculated surface and total nucleon density, coefficient of the rotational energy, angular momentum; deduced existence of stable exotic nuclei with large angular momentum of inertia. Skyrme cranked Hartree-Fock method.

doi: 10.1103/PhysRevLett.107.112501
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2011IT05      Int.J.Mod.Phys. E20, 1012 (2011)

N.Itagaki, Tz.Kokalova, W.von Oertzen, J.A.Maruhn

Three-α cluster state around 40Ca core

NUCLEAR STRUCTURE 40Ca; calculated energy convergence of three α clusters around 40Ca. THSR wave function, time-dependent HF theory.

doi: 10.1142/S0218301311019167
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2011IW01      Phys.Rev. C 84, 014616 (2011)

Y.Iwata, J.A.Maruhn

Enhanced spin-current tensor contribution in collision dynamics

NUCLEAR REACTIONS 40Ca(40Ca, X), E(cm)=130 MeV; calculated spin-current tensor contribution and its dependence on mass of the colliding system. Time-dependent density functional calculations with explicit inclusion of tensor terms.

doi: 10.1103/PhysRevC.84.014616
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2011LO18      Phys.Rev. C 84, 034608 (2011)

N.Loebl, J.A.Maruhn, P.-G.Reinhard

Equilibration in the time-dependent Hartree-Fock approach probed with the Wigner distribution function

NUCLEAR REACTIONS 16O(16O, X), E(cm)=100 MeV; 96Zr(132Sn, X), E(cm)=250 MeV; calculated Wigner and Husimi distribution contours, 2-dimensional momentum distributions, global eccentricity for central and non-central collisions. Time-dependent Hartree-Fock (TDHF) model.

doi: 10.1103/PhysRevC.84.034608
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2011RE05      Phys.Rev. C 83, 034312 (2011)

P.-G.Reinhard, J.A.Maruhn, A.S.Umar, V.E.Oberacker

Localization in light nuclei

NUCLEAR STRUCTURE 4He, 8Be, 12,20C, 16O, 20Ne, 24Mg, 28Si; calculated contours of proton localization and total density. Spatial localization of light nuclei within the Hartree-Fock approximation.

doi: 10.1103/PhysRevC.83.034312
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2010IW01      Phys.Rev.Lett. 104, 252501 (2010)

Y.Iwata, T.Otsuka, J.A.Maruhn, N.Itagaki

Suppression of Charge Equilibration Leading to the Synthesis of Exotic Nuclei

NUCLEAR REACTIONS 208Pb(238U, X), (132Xe, X), (132Sn, X), (40Ca, X), (24Mg, X), (24O, X), (16O, X), (α, X), 24Mg(24O, X), E=2, 3, 4, 4.5, 5, 6, 7, 8 MeV/nucleon; calculated mass and N/Z yields, time evolution of charge distribution, charge equilibration. Skyrme time-dependent Hartee-Fock (TDHF) theory.

doi: 10.1103/PhysRevLett.104.252501
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2010IW02      Nucl.Phys. A836, 108 (2010)

Y.Iwata, T.Otsuka, J.A.Maruhn, N.Itagaki

Geometric classification of nucleon transfer at moderate low-energies

doi: 10.1016/j.nuclphysa.2010.01.242
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2010MA24      Nucl.Phys. A833, 1 (2010)

J.A.Maruhn, N.Loebl, N.Itagaki, M.Kimura

Linear-chain structure of three α-clusters in 16C and 20C

NUCLEAR STRUCTURE 16,20C; calculated ground-state binding energies, β2, configurations, related features for chain-like α clusters using Skyrme mean-field model.

doi: 10.1016/j.nuclphysa.2009.12.005
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2010OB01      Phys.Rev. C 82, 034603 (2010)

V.E.Oberacker, A.S.Umar, J.A.Maruhn, P.-G.Reinhard

Microscopic study of the 132, 124Sn+96Zr reactions: Dynamic excitation energy, energy-dependent heavy-ion potential, and capture cross section

NUCLEAR REACTIONS 96Zr(124Sn, X), (132Sn, X), (134Sn, X), E(cm)=195-260 MeV; calculated mass density contour plots, potential barriers, intrinsic mass quadrupole moment, heavy ion potential barriers, precompound excitation energy, capture and inelastic cross sections using time-dependent Hartree-Fock (TDHF) and density-constrained time-dependent Hartree-Fock methods (DC-TDHF).

doi: 10.1103/PhysRevC.82.034603
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2010UM01      Phys.Rev.Lett. 104, 212503 (2010)

A.S.Umar, J.A.Maruhn, N.Itagaki, V.E.Oberacker

Microscopic Study of the Triple-α Reaction

NUCLEAR REACTIONS 8Be(α, X)12C, E(cm)=2 MeV; calculated time evolution, potential energy curves for 4He + 8Be head-n collision, single-particle parities of the neutron states; deduced formation of a metastable linear chain state of three α-like clusters. Time-dependent Hartree-Fock theory.

doi: 10.1103/PhysRevLett.104.212503
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2010UM02      Phys.Rev. C 81, 064607 (2010)

A.S.Umar, V.E.Oberacker, J.A.Maruhn, P.-G.Reinhard

Entrance channel dynamics of hot and cold fusion reactions leading to superheavy elements

NUCLEAR REACTIONS 208Pb(70Zn, X), E(cm)=260-350 MeV; 238U(48Ca, X), E(cm)=180-250 MeV; calculated potential barriers, excitation energies, and capture σ using fully microscopic time-dependent Hartree-Fock theory coupled with a density constraint. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.064607
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2009IW06      Eur.Phys.J. A 42, 613 (2009); Erratum Eur.Phys.J. A 42, 625 (2009)

Y.Iwata, T.Otsuka, J.A.Maruhn, N.Itagaki

Synthesis of exotic nuclei in heavy-ion collisions at higher energies

NUCLEAR REACTIONS 208Pb(α, X), (16O, X), (24O, X), (24Mg, X), (40Ca, X), (132Sn, X), (132Xe, X), (238U, X), E(cm)=5, 8 MeV/nucleon; calculated Q-values, N/Z yields, time evolution of dipole moment, reaction mechanism features, charge equilibration. Three-dimensional time-dependent Hartee-Fock method.

doi: 10.1140/epja/i2009-10851-1
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2009KL01      Phys.Rev. C 79, 034310 (2009)

P.Klupfel, P.-G.Reinhard, T.J.Burvenich, J.A.Maruhn

Variations on a theme by Skyrme: A systematic study of adjustments of model parameters

NUCLEAR STRUCTURE Z=20, 28, 50, 82, N=20, 28, 50, 82, 126; calculated correlation shifts of charge rms radii, diffraction radii, surface thicknesses, and correlation energies. 16O; calculated mean resonance frequency for GDR. 132Sn; calculated neutron level sequence. 208Pb; calculated mean resonance frequencies for GMR, GDR and GQR, neutron skin. Z=50, N=86-104; calculated uncertainties in binding energies and S(2n). Z=82, N=126-132; calculated isotope shifts. 236U; calculated fission barriers. 264Hs; calculated binding energy, Q(α). A=10-264; calculated errors in binding energies, rms radii and proton deformations. 302120; calculated total binding energy, fission barrier, Q(α). Skyrme-Hartree-Fock model. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.034310
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2009SU06      Phys.Rev. C 79, 044306 (2009)

A.Sulaksono, T.J.Burvenich, P.-G.Reinhard, J.A.Maruhn

Criteria for nonlinear parameters of relativistic mean field models

doi: 10.1103/PhysRevC.79.044306
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2009UM04      Phys.Rev. C 80, 041601 (2009)

A.S.Umar, V.E.Oberacker, J.A.Maruhn, P.-G.Reinhard

Microscopic calculation of pre-compound excitation energies for heavy-ion collisions

NUCLEAR REACTIONS 16O(16O, X), E(cm)=11, 20, 34, 50 MeV; 34Ne(16O, X), E(cm)=11, 15, 30 MeV; 40Ca(40Ca, X), E(cm)=55, 60, 80, 100 MeV;calculated excitation energies, internuclear potentials, and ion-ion potentials for head-on collisions using time-dependent Hartree-Fock (TDHF) theory.

doi: 10.1103/PhysRevC.80.041601
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2008GU06      Phys.Rev. C 77, 041301 (2008)

L.Guo, J.A.Maruhn, P.-G.Reinhard, Y.Hashimoto

Conservation properties in the time-dependent Hartree Fock theory

NUCLEAR REACTIONS 16O(16O, X), E(cm)=25, 125 MeV; calculated angular momentum. Hartree-Fock calculations.

doi: 10.1103/PhysRevC.77.041301
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2008IW06      Int.J.Mod.Phys. E17, 1660 (2008)

Y.Iwata, N.Itagaki, J.A.Maruhn, T.Otsuka

The competitive reaction mechanism in exotic nuclear reactions

doi: 10.1142/S0218301308010672
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2008KL04      Eur.Phys.J. A 37, 343 (2008)

P.Klupfel, J.Erler, P.-G.Reinhard, J.A.Maruhn

Systematics of collective correlation energies from self-consistent mean-field calculations

NUCLEAR STRUCTURE Ca, Ni, Sn, Pb and for N=20, 28, 50, 82, 126 isotones; calculated 2+ state energies, B(E2), rms radii. Skyrme-Hartree-Fock approach with (density-dependent) delta interaction. Comparison with various models and data.

doi: 10.1140/epja/i2008-10633-3
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2008UM04      Eur.Phys.J. A 37, 245 (2008)

A.S.Umar, V.E.Oberacker, J.A.Maruhn

Neutron transfer dynamics and doorway to fusion in time-dependent Hartree-Fock theory

NUCLEAR REACTIONS 24O(16O, X), E(cm)=7, 8, 9 MeV; 96Zr(40Ca, X), E(cm)=91, 97 MeV; calculated neutron and single-particle probability densities, potential barrier using time-dependent Hartree-Fock model.

doi: 10.1140/epja/i2008-10614-6
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2007GU17      Phys.Rev. C 76, 014601 (2007)

L.Guo, J.A.Maruhn, P.-G.Reinhard

Boost-invariant mean field approximation and the nuclear Landau-Zener effect

doi: 10.1103/PhysRevC.76.014601
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2007GU22      Phys.Rev. C 76, 034317 (2007)

L.Guo, J.A.Maruhn, P.-G.Reinhard

Triaxiality and shape coexistence in germanium isotopes

NUCLEAR STRUCTURE Ge; calculated binding energies, quadrupole and triaxial deformation parameters for ground and coexistent isomeric states using Gogny-HFB and Skyrme-HF plus BCS approximation.

doi: 10.1103/PhysRevC.76.034317
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2007GU28      Phys.Rev. C 76, 065801 (2007)

L.Guo, M.Hempel, J.Schaffner-Bielich, J.A.Maruhn

Triaxial nuclear models and the outer crust of nonaccreting cold neutron stars

NUCLEAR STRUCTURE Z=20-48, N=24-110; calculated masses, binding energies, deformations. Comparison with experimental values.

doi: 10.1103/PhysRevC.76.065801
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2007RE23      Eur.Phys.J. A 32, 19 (2007)

P.-G.Reinhard, L.Guo, J.A.Maruhn

Nuclear giant resonances and linear response

NUCLEAR STRUCTURE 16O, 40Ca, 100,120,132Sn, 208Pb; calculated isovector dipole and isoscalar quadrupole GR strength distributions using time dependent HF dynamics using Skyrme forces.

doi: 10.1140/epja/i2007-10366-9
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2007ST27      Nucl.Phys. A788, 343c (2007)

P.D.Stevenson, D.Almehed, P.-G.Reinhard, J.A.Maruhn

Monopole Giant Resonances and TDHF boundary conditions

doi: 10.1016/j.nuclphysa.2007.01.091
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2007SU21      Phys.Rev. C 76, 041301 (2007)

A.Sulaksono, T.Mart, T.J.Burvenich, J.A.Maruhn

Instabilities of relativistic mean field models and the role of nonlinear terms

doi: 10.1103/PhysRevC.76.041301
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2006BR26      Int.J.Mod.Phys. E15, 1417 (2006)

M.P.Brine, P.D.Stevenson, J.A.Maruhn, P.-G.Reinhard

Dipole response in neutron-rich magnesium

NUCLEAR STRUCTURE 34Mg; calculated isovector dipole response.

doi: 10.1142/S0218301306005009
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2006GU16      Int.J.Mod.Phys. E15, 1141 (2006)

L.Guo, F.Sakata, E.-G.Zhao, J.A.Maruhn

To what extent does the self-consistent mean-field exist?

doi: 10.1142/S0218301306004739
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2006MA54      Phys.Rev. C 74, 027601 (2006)

J.A.Maruhn, P.-G.Reinhard, P.D.Stevenson, M.R.Strayer

Spin-excitation mechanisms in Skyrme-force time-dependent Hartree-Fock calculations

NUCLEAR REACTIONS 16O(16O, X), E(cm)=75-150 MeV; calculated energy loss, spin excitations, role of odd-odd couplings. Skyrme-force time-dependent Hartree-Fock calculations.

doi: 10.1103/PhysRevC.74.027601
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2006MA72      Phys.Rev. C 74, 044311 (2006)

J.A.Maruhn, M.Kimura, S.Schramm, P.-G.Reinhard, H.Horiuchi, A.Tohsaki

α-cluster structure and exotic states in a self-consistent model for light nuclei

NUCLEAR STRUCTURE 4He, 8Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar; calculated binding energies, deformation, cluster configurations. 28Si, 32S, 36Ar, 40Ca; calculated superdeformed states features.

doi: 10.1103/PhysRevC.74.044311
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2005LI30      Phys.Rev.Lett. 95, 042501 (2005)

Yu.A.Litvinov, T.J.Burvenich, H.Geissel, Yu.N.Novikov, Z.Patyk, C.Scheidenberger, F.Attallah, G.Audi, K.Beckert, F.Bosch, M.Falch, B.Franzke, M.Hausmann, Th.Kerscher, O.Klepper, H.-J.Kluge, C.Kozhuharov, K.E.G.Lobner, D.G.Madland, J.A.Maruhn, G.Munzenberg, F.Nolden, T.Radon, M.Steck, S.Typel, H.Wollnik

Isospin Dependence in the Odd-Even Staggering of Nuclear Binding Energies

NUCLEAR STRUCTURE Hf, W; compiled, analyzed neutron and proton pair-gap energies, odd-even staggering effect. Several models compared with data.

doi: 10.1103/PhysRevLett.95.042501
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2005MA41      Phys.Rev. C 71, 064328 (2005)

J.A.Maruhn, P.G.Reinhard, P.D.Stevenson, J.Rikovska Stone, M.R.Strayer

Dipole giant resonances in deformed heavy nuclei

NUCLEAR STRUCTURE 132Sn, 142,144,146,148,150Nd, 152Dy, 188Os, 238U; calculated dipole strength distributions, resonance features, deformation dependence. Time-dependent Skyrme-Hartree-Fock method.

doi: 10.1103/PhysRevC.71.064328
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2004BU03      Phys.Rev. C 69, 014307 (2004); Erratum Phys.Rev. C 69, 029901 (2004)

T.Burvenich, M.Bender, J.A.Maruhn, P.-G.Reinhard

Systematics of fission barriers in superheavy elements

NUCLEAR STRUCTURE Z=108-120; calculated fission barrier energies, related features. Relativistic mean-field and nonrelativistic Skyrme-Hartree-Fock approaches. Comparison with data.

doi: 10.1103/PhysRevC.69.014307
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2004BU18      Acta Phys.Hung.N.S. 19, 149 (2004)

T.Burvenich, T.Cornelius, A.Sulaksono, J.A.Maruhn, W.Greiner, D.G.Madland, P.-G.Reinhard, S.Schramm

Application and Extrapolation of Mean-Field Models in the Heavy and Superheavy Regions

NUCLEAR STRUCTURE 292120; calculated neutron and proton density distributions. Relativistic point-coupling models.

doi: 10.1556/APH.19.2004.1-2.23
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2004FL04      Phys.Rev. C 70, 054321 (2004)

P.Fleischer, P.Klupfel, P.-G.Reinhard, J.A.Maruhn

Skyrme energy functional and low lying 2+ states in Sn, Cd, and Te isotopes

NUCLEAR STRUCTURE Sn, Cd, Te; calculated level energies, B(E2), radii. Several Skyrme forces compared.

doi: 10.1103/PhysRevC.70.054321
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2004FL05      Eur.Phys.J. A 22, 363 (2004)

P.Fleischer, P.Klupfel, T.Cornelius, T.J.Burvenich, S.Schramm, J.A.Maruhn, P.-G.Reinhard

The two-proton shell gap in Sn isotopes

NUCLEAR STRUCTURE 108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated two-proton shell gap, deformation and correlation effects. Cd, Sn, Te; calculated deformation energies. Several models compared.

doi: 10.1140/epja/i2004-10054-4
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2004JO17      J.Phys.(London) G30, L43 (2004)

E.F.Jones, J.H.Hamilton, P.M.Gore, A.V.Ramayya, J.K.Hwang, A.P.deLima, S.J.Zhu, Y.X.Luo, C.J.Beyer, J.Kormicki, X.Q.Zhang, W.C.Ma, I.Y.Lee, J.O.Rasmussen, S.C.Wu, T.N.Ginter, P.Fallon, M.Stoyer, J.D.Cole, A.V.Daniel, G.M.Ter-Akopian, R.Donangelo, S.J.Asztalos, T.Cornelius, P.Fleischer, M.Bender, T.Burvenich, S.Schramm, J.A.Maruhn, P.-G.Reinhard

Identification of levels in 162, 164Gd and decrease in moment of inertia between N = 98-100

RADIOACTIVITY 252Cf(SF); measured Eγ, Iγ, γγ-coin. 162,164Gd deduced levels, J, π, rotational bands. Collective features in neighboring nuclides discussed.

doi: 10.1088/0954-3899/30/12/L02
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2004MA56      Nucl.Phys. A738, 245 (2004)

J.A.Maruhn, M.R.Strayer, P.-G.Reinhard, H.Horiuchi

Search for Highly-Deformed or Molecular States in a Static Hartree-Fock Method

NUCLEAR STRUCTURE 28Si, 32S, 36Ar, 40Ca; calculated cluster states energies, deformation. Static Hartree-Fock method.

doi: 10.1016/j.nuclphysa.2004.04.039
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2004MA60      Nucl.Phys. A741, 52 (2004)

D.G.Madland, T.J.Burvenich, J.A.Maruhn, P.-G.Reinhard

On the isovector channels in relativistic point coupling models within the Hartree and Hartree-Fock approximations

doi: 10.1016/j.nuclphysa.2004.06.003
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2004RE29      Nucl.Phys. A746, 76c (2004)

P.-G.Reinhard, T.Burvenich, T.Cornelius, P.Fleischer, P.Klupfel, J.A.Maruhn

Mean-field models and exotic nuclei

doi: 10.1016/j.nuclphysa.2004.09.072
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2002BE40      Eur.Phys.J. A 14, 23 (2002)

M.Bender, T.Cornelius, G.A.Lalazissis, J.A.Maruhn, W.Nazarewicz, P.-G.Reinhard

The Z = 82 Shell Closure in Neutron-Deficient Pb Isotopes

NUCLEAR STRUCTURE Hg, Pb, Po; calculated single-particle energies, deformation energy, two-proton gap parameters for A ≈ 180-210; deduced shell closure features. Self-consistent mean-field approach.

doi: 10.1007/s10050-002-8785-2
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2002BU07      Phys.Rev. C65, 044308 (2002)

T.Burvenich, D.G.Madland, J.A.Maruhn, P.-G.Reinhard

Nuclear Ground State Observables and QCD Scaling in a Refined Relativistic Point Coupling Model

NUCLEAR STRUCTURE Ca, Ni, Sn, Pb, Cf, Fm, No, Rf, Sg, Hs; calculated binding energies. 240Pu; calculated fission barrier. Sn, Pb; calculated radii, surface thickness. 48Ca, 100Sn; calculated total baryon densities. 48Ca; calculated charge form factor. Relativistic point-coupling model, comparison with other models.

doi: 10.1103/PhysRevC.65.044308
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2002BU20      Phys.Lett. 542B, 261 (2002)

T.Burvenich, I.N.Mishustin, L.M.Satarov, J.A.Maruhn, H.Stocker, W.Greiner

Enhanced Binding and Cold Compression of Nuclei due to Admixture of Antibaryons

NUCLEAR STRUCTURE 8Be, 16O; calculated density distributions, energy levels with and without antiproton admixture.

doi: 10.1016/S0370-2693(02)02351-1
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2002BU36      Acta Phys.Hung.N.S. 16, 275 (2002)

T.Burvenich, M.Bender, P.-G.Reinhard, J.A.Maruhn

Fission Barriers of Superheavy Nuclei from Self-Consistent Mean-Field Models

NUCLEAR STRUCTURE Z=108-120; calculated fission barrier features. Self-consistent mean-field approach.

doi: 10.1556/APH.16.2002.1-4.30
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2002BU37      J.Nucl.Radiochem.Sci. 3, No 1, 191 (2002)

T.Burvenich, D.G.Madland, J.A.Maruhn, P.-G.Reinhard

A Relativistic Point Coupling Model for Nuclear Structure Calculations


2000BE24      Eur.Phys.J. A 7, 467 (2000)

M.Bender, K.Rutz, P.-G.Reinhard, J.A.Maruhn

Consequences of the Center-of-Mass Correction in Nuclear Mean-Field Models

NUCLEAR STRUCTURE A=10-270; calculated center-of-mass energy corrections. 44S, 240Pu; calculated deformation energies. Several effective interactions compared.

doi: 10.1007/s100500050419
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2000BE32      Eur.Phys.J. A 8, 59 (2000)

M.Bender, K.Rutz, P.-G.Reinhard, J.A.Maruhn

Pairing Gaps from Nuclear Mean-Field Models

doi: 10.1007/s100530050009
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2000BR06      Phys.Rev. C61, 024909 (2000)

J.Brachmann, S.Soff, A.Dumitru, H.Stocker, J.A.Maruhn, W.Greiner, L.V.Bravina, D.H.Rischke

Antiflow of Nucleons at the Softest Point of the Equation of State

NUCLEAR REACTIONS 197Au(197Au, X), E=8 GeV/nucleon; calculated time evolution of nucleon flow, net-baryon number, rapidity distributions. 197Au(197Au, X), E=2.5-200 GeV/nucleon; calculated directed flow, transverse momentum distributions; deduced antiflow component, quark-gluon plasma phase transition features. Macroscopic and microscopic transport models.

doi: 10.1103/PhysRevC.61.024909
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2000RE21      Hyperfine Interactions 127, 13 (2000)

P.-G.Reinhard, C.Reiss, M.Bender, T.Burvenich, T.Cornelius, J.A.Maruhn

Exotic nuclei - a challenge for nuclear mean-field models

NUCLEAR STRUCTURE Hg; calculated radii, deformation. Sn; calculated two-neutron separation energies, skin thickness for neutron-rich isotopes.

doi: 10.1023/A:1012633904537
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1999BE38      Phys.Rev. C60, 034304 (1999)

M.Bender, K.Rutz, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Shell Structure of Superheavy Nuclei in Self-Consistent Mean-Field Models

NUCLEAR STRUCTURE 208Pb, 298Fl, 292120, 310126; calculated single-particle levels; deduced shell closure features. Z=120, A=270-380; calculated single-proton levels, two-proton shell gap. Shell closures at Z=120, N=172 predicted. Self-consistent mean-field model.

doi: 10.1103/PhysRevC.60.034304
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1999BE75      Acta Phys.Hung.N.S. 10, 185 (1999)

M.Bender, K.Rutz, T.Burvenich, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Superheavy Nuclei in Self-Consistent Mean-Field Models

NUCLEAR STRUCTURE Z=100-140; calculated shell gaps. 208Pb, 298Fl, 292120; calculated single-particle levels. 264Hs, 298Fl, 292120; calculated potential energy vs deformation. Self-consistent mean-field models, several parameterizations compared.


1999RE12      Phys.Rev. C60, 014316 (1999)

P.-G.Reinhard, D.J.Dean, W.Nazarewicz, J.Dobaczewski, J.A.Maruhn, M.R.Strayer

Shape Coexistence and the Effective Nucleon-Nucleon Interaction

NUCLEAR STRUCTURE 30,32,34Mg, 26,28,30,32Ne, 38,40,42,44S, 80,82,84,92,94,96,98,100Zr; calculated potential energy surfaces, neutron shell structure; deduced shape coexistence mechanisms. Self-consistent Hartree-Fock, shell model approaches.

doi: 10.1103/PhysRevC.60.014316
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1999RU09      Phys.Lett. 468B, 1 (1999)

K.Rutz, M.Bender, P.-G.Reinhard, J.A.Maruhn

Pairing Gap and Polarisation Effects

NUCLEAR STRUCTURE Sn; calculated neutron pair gaps, two-neutron separation energies, radii for N=49-83. 110Sn, 240Pu; calculated deformation features. Relativistic mean-field approach.

doi: 10.1016/S0370-2693(99)01190-9
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1999SC23      Prog.Part.Nucl.Phys. 42, 279 (1999)

S.Scherer, S.A.Bass, M.Bleicher, M.Belkacem, L.Bravina, J.Brachmann, A.Dumitru, C.Ernst, L.Gerland, M.Hofmann, L.Neise, M.Reiter, S.Soff, C.Spieles, H.Weber, E.Zabrodin, D.Zschiesche, J.A.Maruhn, H.Stocker, W.Greiner

Critical Review of Quark Gluon Plasma Signatures

doi: 10.1016/S0146-6410(99)00083-6
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1998BE65      Acta Phys.Hung.N.S. 7, 167 (1998)

M.Bender, K.Rutz, T.Burvenich, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Superheavy Nuclei in Self-Consistent Models

NUCLEAR STRUCTURE Z=98-108; calculated binding energies, two-neutron separation energies, other ground-state properties for even-even nuclei. 298Fl; calculated single-particle levels. Several models compared.


1998BE66      Phys.Rev. C58, 2126 (1998)

M.Bender, K.Rutz, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Potential Energy Surfaces of Superheavy Nuclei

NUCLEAR STRUCTURE 258Fm, 264Hs, 278Cn, 298Fl, 292120; calculated potential energy vs deformation; deduced fission barrier features. Relativistic mean-field model, Skyrme-Hartree-Fock approach.

doi: 10.1103/PhysRevC.58.2126
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1998BU26      Eur.Phys.J. A 3, 139 (1998)

T.Burvenich, K.Rutz, M.Bender, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Superheavy Nuclei in Deformed Mean-Field Calculations

NUCLEAR STRUCTURE Z=98-108; calculated even-even nuclei two-neutron, two-proton separation energies. Z=102-128; calculated proton, neutron shell gaps, α-decay Q-values; deduced shell closure features. Nonrelativistic Skyrme-Hartree-Fock scheme, relativistic mean-field model approaches.

doi: 10.1007/s100500050160
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1998RE21      Nucl.Phys. A643, 99 (1998)

M.Reiter, A.Dumitru, J.Brachmann, J.A.Maruhn, H.Stocker, W.Greiner

Entropy Production in Collisions of Relativistic Heavy Ions - A Signal for Quark-Gluon Plasma Phase Transition ?

NUCLEAR REACTIONS 197Au(197Au, X), E(cm)=4.9 GeV/nucleon; calculated baryon density vs time. Pb(Pb, X), E=11-160 GeV/nucleon; calculated entropy per baryon vs time, relative particle yields; deduced no quark-gluon plasma signature. Relativistic multi-fluid hydrodynamics.

doi: 10.1016/S0375-9474(98)00556-9
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1998RU03      Nucl.Phys. A634, 67 (1998)

K.Rutz, M.Bender, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Odd Nuclei and Single-Particle Spectra in the Relativistic Mean-Field Model

NUCLEAR STRUCTURE 16,17O, 17F, 40,41,48,49Ca, 41,49Sc, 56,57Ni, 57Cu, 100,101,132,133Sn, 101,133Sb, 208,209Pb, 209Bi, 218,219U, 219Np; calculated levels, J, π, neutron, proton separation energies; deduced core polarization effects. Relativistic mean-field approach.

doi: 10.1016/S0375-9474(98)00153-5
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1997BE61      Nucl.Phys. A625, 473 (1997)

S.Bernard, D.H.Rischke, J.A.Maruhn, W.Greiner

Kaon Interferometry as Signal for the QCD Phase Transition at RHIC

doi: 10.1016/S0375-9474(97)00164-4
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1997BE84      Acta Phys.Hung.N.S. 5, 445 (1997)

S.Bernard, D.H.Rischke, J.A.Maruhn, W.Greiner

Correlations of Pions and Kaons as a Measure for Delayed Expansion Due To the QCD Phase Transition


1997BR13      Nucl.Phys. A619, 391 (1997)

J.Brachmann, A.Dumitru, J.A.Maruhn, H.Stocker, W.Greiner, D.H.Rischke

Non-Equilibrium Fluid-Dynamics in the Early Stage of Ultrarelativistic Heavy-Ion Collisions

NUCLEAR REACTIONS 197Au(197Au, X), E=11 GeV/nucleon; calculated projectile fluid energy density profile, baryon fluid evolution, other aspects. Ultrarelativistic collisions, three-fluid hydrodynamical model.

doi: 10.1016/S0375-9474(97)00182-6
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1997RE15      Z.Phys. A358, 277 (1997)

P.-G.Reinhard, M.Bender, K.Rutz, J.A.Maruhn

An HFB Scheme in Natural Orbitals

doi: 10.1007/s002180050328
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1997RU04      Phys.Rev. C56, 238 (1997)

K.Rutz, M.Bender, T.Burvenich, T.Schilling, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Superheavy Nuclei in Self-Consistent Nuclear Calculations

NUCLEAR STRUCTURE 264Hs; calculated binding energy, quadrupole deformation; deduced superheavy magic numbers. Z=110-140; N ≈ 140-280; calculated nucleon gaps plots. Z=120; N=160-260; calculated single proton levels vs neutron number. Relativistic mean-field, spherical HF calculations, comparison of several parametrizations.

doi: 10.1103/PhysRevC.56.238
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1996BA20      Phys.Rev. C53, 2358 (1996)

S.A.Bass, A.Bischoff, J.A.Maruhn, H.Stocker, W.Greiner

Neural Networks for Impact Parameter Determination

doi: 10.1103/PhysRevC.53.2358
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1996BE49      Nucl.Phys. A605, 566 (1996)

S.Bernard, J.A.Maruhn, W.Greiner, D.H.Rischke

Relativistic Hydrodynamics for Heavy-Ion Collisions. Freeze-Out and Particle Spectra

doi: 10.1016/0375-9474(96)00165-0
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1996NA03      Phys.Rev. C53, 740 (1996)

W.Nazarewicz, J.Dobaczewski, T.R.Werner, J.A.Maruhn, P.-G.Reinhard, K.Rutz, C.R.Chinn, A.S.Umar, M.R.Strayer

Structure of Proton Drip-Line Nuclei Around Doubly Magic 48Ni

NUCLEAR STRUCTURE 42,44Cr, 46,48Fe, 48,50Ni; calculated 2-proton separation energies, deformations, single-particle levels, diproton partial decay T1/2. Self-consistent, relativistic mean-field theories.

doi: 10.1103/PhysRevC.53.740
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1996RE08      Phys.Rev. C53, 2776 (1996)

P.-G.Reinhard, W.Nazarewicz, M.Bender, J.A.Maruhn

Lipkin-Nogami Pairing Scheme in Self-Consistent Nuclear Structure Calculations

NUCLEAR STRUCTURE 48Cr; calculated potential energy surface, single particle (proton) occupation coefficient vs single particle energy. 208Pb, 148Gd, 120Sn, 90Zr, 40Ca; calculated nucleon average level density at Fermi energy vs (effective mass)/mass. 258Fm; calculated potential energy surface. 198,200,202,204,206,208,210,212,214,216,220Pb; calculated binding energy per nucleon, proton rms radii, isotope shifts. Lipkin-Nogami pairing scheme, self-consistent approach.

doi: 10.1103/PhysRevC.53.2776
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1995DU01      Phys.Rev. C51, 2166 (1995)

A.Dumitru, U.Katscher, J.A.Maruhn, H.Stocker, W.Greiner, D.H.Rischke

Pion and Thermal Photon Spectra as a Possible Signal for a Phase Transition

NUCLEAR REACTIONS 197Au(S, X), E=200 GeV/nucleon; 197Au(197Au, X), E=11 GeV/nucleon; Pb(Pb, X), E=160 GeV/nucleon; analyzed thermal photon, π0 spectra; deduced phase transition evidence. Three-fluid hydrodynamics model.

doi: 10.1103/PhysRevC.51.2166
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1995DU11      Z.Phys. A353, 187 (1995)

A.Dumitru, U.Katscher, J.A.Maruhn, H.Stocker, W.Greiner, D.H.Rischke

Thermal Photons as a Measure for the Rapidity Dependence of the Temperature

NUCLEAR REACTIONS Pb(Pb, X), E=high; calculated thermal photons rapidity distributions; deduced model dependence. Scaling, three-fluid hydrodynamics scenarios.

doi: 10.1007/BF01295896
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1995MI01      Phys.Rev. C51, 2099 (1995)

I.N.Mishustin, L.M.Satarov, J.A.Maruhn, H.Stocker, W.Greiner

Bose-Stimulated Pion Production in Relativistic Nuclear Collisions

NUCLEAR REACTIONS 197Au(197Au, X), E=10.7 GeV/nucleon; S(S, X), 197Au(197Au, X), E=200 GeV/nucleon; analyzed pion production data, relativistic collisions; deduced Bose enhancement related features. Simple kinetic model, quasideuteron, Δ-isobar mechanism.

doi: 10.1103/PhysRevC.51.2099
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1995RI09      Nucl.Phys. A595, 346 (1995)

D.H.Rischke, S.Bernard, J.A.Maruhn

Relativistic Hydrodynamics for Heavy-Ion Collisions. I. General Aspects and Expansion into Vacuum

doi: 10.1016/0375-9474(95)00355-1
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1995RI10      Nucl.Phys. A595, 383 (1995); Erratum Nucl.Phys. A596, 717 (1996)

D.H.Rischke, Y.Pursun, J.A.Maruhn

Relativistic Hydrodynamics for Heavy-Ion Collisions. II. Compression of Nuclear Matter and the Phase Transition to the Quark-Gluon Plasma

doi: 10.1016/0375-9474(95)00356-3
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1995RU10      Nucl.Phys. A590, 680 (1995)

K.Rutz, J.A.Maruhn, P.-G.Reinhard, W.Greiner

Fission Barriers and Asymmetric Ground States in the Relativistic Mean-Field Theory

NUCLEAR STRUCTURE 240Pu, 232Th, 226Ra; calculated potential energy surfaces, fission barrier heights; deduced symmetric, asymmetric fission path related features. 216,218,220,222,224,226,228,230,232,234Ra; calculated intrinsic ground states vector densities, binding energy difference relative to experiment, octupole deformation. Relativistic mean field theory.

doi: 10.1016/0375-9474(95)00192-4
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1994BA08      J.Phys.(London) G20, L21 (1994)

S.A.Bass, A.Bischoff, C.Hartnack, J.A.Maruhn, J.Reinhardt, H.Stocker, W.Greiner

Neural Networks for Impact Parameter Determination

NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; calculated θ(flow), (Q(ZZ)) observable vs impact parameter; deduced neural network impact parameter determination capabilities.

doi: 10.1088/0954-3899/20/1/004
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1994BL02      Phys.Lett. 323B, 262 (1994)

V.Blum, J.A.Maruhn, P.-G.Reinhard, W.Greiner

The Fission Barrier of 240Pu in the Relativistic Mean Field Theory

NUCLEAR STRUCTURE 240Pu; calculated nucleon density, binding energy, fission barrier, potential energy surfaces. Relativistic mean field theory.

doi: 10.1016/0370-2693(94)91217-3
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1994SC34      Z.Phys. A350, 91 (1994)

J.Schaffner, J.A.Maruhn, H.Stocker, W.Greiner

Proton Halos in 100Sn using a Relativistic Shell Model

NUCLEAR STRUCTURE 100Sn; calculated binding energy, proton, neutron separation energies.

doi: 10.1007/BF01290673
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1994TR04      Z.Phys. A348, 1 (1994)

D.Troltenier, J.A.Maruhn, W.Greiner

The g(R)-Factor of Rare-Earth Nuclei in the Geometric Collective Model

NUCLEAR STRUCTURE 166,168,170Er; calculated potential energy surfaces, levels, intraground state band B(λ), g(R)-factor vs angular momentum. 156,158,160Gd, 160,164Dy, 170,172,174Yb; calculated g(R)-factor vs angular momentum. Geometric collective model, parameter-free collective magnetic dipole operator.

doi: 10.1007/BF01291645
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1994VA23      Nucl.Phys. A577, 605 (1994)

H.van Geel, P.O.Hess, D.Troltenier, J.A.Maruhn, W.Greiner

Microscopically Derived Potential-Energy Surfaces for the Chain of Sm-Isotopes

NUCLEAR STRUCTURE 148,150,152Sm; calculated levels, potential energy surfaces. Microscopic approach.

doi: 10.1016/0375-9474(94)90935-0
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1993OB02      Phys.Rev. C48, 1297 (1993)

V.E.Oberacker, A.S.Umar, J.C.Wells, C.Bottcher, M.R.Strayer, J.A.Maruhn

Muon-Induced Fission: A probe for nuclear dissipation and fission dynamics

NUCLEAR STRUCTURE 238U; calculated mesonic atom levels, Coulomb interaction potential; deduced muon induced fission features.

ATOMIC PHYSICS, Mesic-Atoms 238U; calculated mesonic atom levels, Coulomb interaction potential; deduced muon induced fission features.

doi: 10.1103/PhysRevC.48.1297
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1992TR04      Z.Phys. A343, 25 (1992)

D.Troltenier, J.A.Maruhn, W.Greiner, P.O.Hess

A General Numerical Solution of Collective Quadrupole Surface Motion Applied to Microscopically Calculated Potential Energy Surfaces

NUCLEAR STRUCTURE 190Pt, 238U; calculated levels, potential energy surfaces, B(λ). Pseudo-symplectic model.

doi: 10.1007/BF01291593
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1991TR01      Z.Phys. A338, 261 (1991)

D.Troltenier, J.A.Maruhn, W.Greiner, V.V.Aguilar, P.O.Hess, J.H.Hamilton

Shape Transitions and Shape Coexistence in the Ru and Hg Chains

NUCLEAR STRUCTURE 182,184,186,188,190,192,194,196Hg, 96,98,100,102,104,106,108Ru; calculated levels, B(λ), potential energy surfaces, quadrupole moments.

doi: 10.1007/BF01288188
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1990BA04      Z.Phys. A335, 139 (1990)

S.I.Bastrukov, J.A.Maruhn

Fluid-Dynamics of the Nuclear Surface Fermi-Layer

NUCLEAR STRUCTURE A=50-250; calculated quantum-capillary 2+ state energy vs mass. Long mean free path approach, fluid dynamical model.


1989BL04      Phys.Lett. 223B, 123 (1989)

V.Blum, J.Fink, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Potential Energy Surfaces of Gd-Isotopes in a Relativistic Model

NUCLEAR STRUCTURE 146,148,150,152,154,156,158Gd; calculated potential energy surfaces, proton distribution quadrupole moments. Relativistic mean field theory.

doi: 10.1016/0370-2693(89)90225-6
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1989FI04      Phys.Lett. 218B, 277 (1989)

J.Fink, V.Blum, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Systematic Study of Potential Energy Surfaces of Light Nuclei in Relativistic Hartree Calculations

NUCLEAR STRUCTURE 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca; calculated ground state energy, charge radii, quadrupole moment. Relativistic Hartree-Fock.

doi: 10.1016/0370-2693(89)91580-3
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