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NSR database version of April 29, 2024.

Search: Author = J.Nemeth

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1999NE02      Nucl.Phys. A647, 107 (1999)

J.Nemeth, G.Papp, H.Feldmeier

Au + Au Central Collisions at 150, 250 and 400 A MeV Energies in QMD with Relativistic Forces

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=150, 250, 400 MeV/nucleon; calculated light, intermediate fragments charge, multiplicity distributions, angular distributions, transverse spectra. Relativistic scalar-vector force, quantum molecular dynamics. Comparison with data.

doi: 10.1016/S0375-9474(99)00009-3
Citations: PlumX Metrics

1999NE03      Phys.Rev. C59, 1802 (1999)

J.Nemeth, G.Papp

Collective Flow in Central Au-Au Collisions at 150, 250, and 400 A MeV

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=150, 250, 400 MeV/nucleon; calculated collective radial flow related features. Comparison with data.

doi: 10.1103/PhysRevC.59.1802
Citations: PlumX Metrics

1997NE10      Acta Phys.Hung.N.S. 5, 249 (1997)

J.Nemeth

Multifragmentation, Equation of State, Effective Mass

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁹⁷Au, X), E=400 MeV/nucleon; calculated intermediate mass fragment multiplicities; deduced dependence on equation of state.

1996CS06      Acta Phys.Hung.N.S. 3, 17 (1996)

L.P.Csernai, J.Nemeth, G.Papp

Instabilities in Nuclear Multifragmentation

1996FE18      Acta Phys.Hung.N.S. 3, 71 (1996)

H.Feldmeier, J.Nemeth, G.Papp

Multifragmentation Calculated with Relativistic Forces

NUCLEAR REACTIONS Ca(Ca, X), E=200, 400, 800 MeV/nucleon; calculated relative momenta distributions vs time. Br(O, X), E=50-200 MeV/nucleon; calculated fragments charge distribution vs time. Coordinate and momentum dependent relativistic forces.

1994SO05      Nucl.Phys. A571, 159 (1994)

S.R.Souza, L.de Paula, S.Leray, J.Nemeth, C.Ngo, H.Ngo

A Dynamical Model for Multifragmentation of Nuclei

NUCLEAR REACTIONS ⁸⁰Br(¹⁶O, X), E ≤ 200 MeV/nucleon; calculated fragment charge distribution, multi-fragmentation probability vs impact parameter. Molecular dynamics based schematic model.

doi: 10.1016/0375-9474(94)90346-8
Citations: PlumX Metrics

1991DE16      Phys.Lett. 258B, 251 (1991)

L.De Paula, J.Nemeth, B.-H.Sa, S.Leray, C.Ngo, H.Ngo, S.R.Souza, Y.-M.Zheng

Stability of Excited Nuclei in a Dynamical Simulation

NUCLEAR STRUCTURE ¹⁹⁷Au; calculated stability against multifragmentation. Heat, compression, rotation type excitations, dynamical simulation.

doi: 10.1016/0370-2693(91)91079-B
Citations: PlumX Metrics

1989GA10      Nucl.Phys. A495, 169c (1989)

F.Garcias, M.Barranco, J.Nemeth, C.Ngo, X.Vinas

The Fission of Hot Rotating Nuclei: A selfconsistent Thomas-Fermi calculation

NUCLEAR STRUCTURE ¹⁰⁹Cd, ¹¹⁸Sn, ¹⁶⁴Ho, ¹⁸⁶Os, ²⁰⁷Bi, ²⁴⁰Pu; calculated fission barrier thermal evolution. Axially deformed Thomas-Fermi model.

doi: 10.1016/0375-9474(89)90316-3
Citations: PlumX Metrics

1989GA13      Phys.Rev. C40, 1522 (1989)

F.Garcias, M.Barranco, H.S.Wio, C.Ngo, J.Nemeth

Fission Stability Diagram of ²⁴⁰Pu

NUCLEAR STRUCTURE ²⁴⁰Pu; calculated fission barrier vs quadrupole moment. Axially symmetric deformed Thomas-Fermi model.

doi: 10.1103/PhysRevC.40.1522
Citations: PlumX Metrics

1988CE01      Nucl.Phys. A476, 74 (1988)

C.Cerruti, J.Desbois, R.Boisgard, C.Ngo, J.Natowitz, J.Nemeth

Multifragmentation and Incomplete Fusion in Central Heavy Ion Collisions within a Schematic Phenomenological Model

NUCLEAR REACTIONS ¹⁹⁷Au(¹²C, X), (²⁰Ne, X), (⁴⁰Ar, X), E=10-80 MeV/nucleon; calculated emitted nucleon number per projectile nucleon characteristics. Schematic phenomenological model.

doi: 10.1016/0375-9474(88)90374-0
Citations: PlumX Metrics

1988GA07      Phys.Lett. 206B, 177 (1988)

F.Garcias, M.Barranco, J.Nemeth, C.Ngo

Thomas-Fermi Calculations of the Level Density Parameter of Deformed Nuclei

NUCLEAR STRUCTURE ¹⁶⁴Ho, ⁶³Cu; calculated fission barrier vs quadrupole moment. ⁶³Cu, ¹⁶⁴Ho, ²⁰⁵At, ²⁴⁰Pu; calculated level density parameter vs quadrupole moment. Constrained Thomas-Fermi model.

doi: 10.1016/0370-2693(88)91487-6
Citations: PlumX Metrics

1987BA08      Nucl.Phys. A464, 29 (1987)

M.Barranco, M.Pi, J.Nemeth, C.Ngo, E.Tomasi

Spurious Continuum Effects on Excited Giant Resonances

NUCLEAR STRUCTURE ⁴⁰Ca; calculated giant monopole isoscalar strength function. ²⁰⁸Pb; calculated sum rules, average energies; deduced spurious continuum effects role. Time-dependent Thomas-Fermi model.

doi: 10.1016/0375-9474(87)90420-9
Citations: PlumX Metrics

1987DE30      Z.Phys. A328, 101 (1987)

J.Desbois, R.Boisgard, C.Ngo, J.Nemeth

Multifragmentation of Excited Nuclei within a Schematic Hydrodynamical and Percolation Picture

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁶⁰Ni, ⁹⁰Zr, ¹¹⁶Sn, ¹⁴⁰Ce, ²⁰⁸Pb, ²³⁸U; calculated binding energy. ²⁰⁸Pb; calculated nucleon density time evolution. Hydrodynamical model, hot compressed nuclei.

1987NG04      J.Phys.(Paris), Colloq.C-2, 157 (1987)

C.Ngo, R.Boisgard, J.Desbois, J.Nemeth, M.Barranco

Multifragmentation of Nuclei

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated multi-fragmentation instability, per nucleon excitation energy/binding energy, density vs radius. Irrotational hydrodynamical model.

1986NE02      Z.Phys. A323, 419 (1986)

J.Nemeth, M.Barranco, C.Ngo, E.Tomasi

Model for the Evolution of Hot and Compressed Spherical Nuclei

NUCLEAR STRUCTURE ⁴⁰Ca; calculated rms radius time evolution. ²⁰⁸Pb, ¹⁶O calculated density profile vs radius evolution. Hydrodynamical approach.

1986NE04      Z.Phys. A325, 347 (1986)

J.Nemeth, M.Barranco, J.Desbois, C.Ngo

Multifragmentation of Hot and Compressed Nuclei within a Time Dependent Thomas Fermi and Percolation Model

NUCLEAR STRUCTURE ²⁰⁸Pb; calculated dynamical evolution, density profile, primary, secondary mass distribution, multifragmentation, normal de-excitation regions, maximum thermal excitation energy per nucleon; deduced hot compressed nuclei multifragmentation. Time dependent Thomas-Fermi, percolation models.

1986PI02      Phys.Lett. 166B, 1 (1986)

M.Pi, M.Barranco, J.Nemeth, C.Ngo, E.Tomasi

Time-Dependent Thomas-Fermi Approach to Nuclear Monopole Oscillations

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca; calculated isoscalar strength function. Time-dependent Thomas-Fermi approach.

doi: 10.1016/0370-2693(86)91143-3
Citations: PlumX Metrics

1985DA05      Z.Phys. A321, 335 (1985)

D.Dalili, J.Nemeth, C.Ngo

A Self Consistent Thomas Fermi Calculation of Fission Barriers at Finite Temperature and Angular Momentum as Applied to the ²⁰⁵At

NUCLEAR STRUCTURE ²⁰⁵At; calculated fission barrier vs temperature, free, binding energies vs quadrupole moment. Self-consistent Thomas-Fermi calculation.

doi: 10.1007/BF01493455
Citations: PlumX Metrics

1985NE02      Phys.Lett. 154B, 11 (1985)

J.Nemeth, D.Dalili, C.Ngo

Hartree-Fock and Thomas-Fermi Self-Consistent Calculations of the ¹⁴⁴Nd Nucleus at Finite Temperature and Angular Momentum

NUCLEAR STRUCTURE ¹⁴⁴Nd; calculated fission barrier; deduced temperature, angular momentum dependences. Constrained Hartree-Fock, Thomas-Fermi approximations.

doi: 10.1016/0370-2693(85)91557-6
Citations: PlumX Metrics

1985NE03      Z.Phys. A320, 691 (1985)

J.Nemeth, M.Barranco, C.Ngo, E.Tomasi

Spherical Time Dependent Thomas-Fermi Calculation of the Dynamical Evolution of Hot and Compressed Nuclei

NUCLEAR STRUCTURE ⁴⁰Ca; calculated density profile vs temperature. Self consistent time-dependent Thomas-Fermi model.

doi: 10.1007/BF01411873
Citations: PlumX Metrics

1985NE10      Acta Phys.Acad.Sci.Hung. 58, 5 (1985)

J.Nemeth, J.M.Irvine

High Energy Proton Induced Fission of Light Nuclei

NUCLEAR STRUCTURE ¹⁴⁴Nd; calculated proton induced fission probability. Extended TDHF calculation.

1985OK01      J.Phys.(London) G11, 721 (1985)

J.Okolowicz, J.M.Irvine, J.Nemeth

Nuclear Temperatures and Collective Motion

NUCLEAR STRUCTURE ¹¹⁰Zr; calculated collective energy, quadrupole moment, rms radius, temperature time evolution. ¹⁴⁴Nd; calculated fission barriers vs quadrupole moment, two-center separation distance. TDHF, collective motion.

doi: 10.1088/0305-4616/11/6/009
Citations: PlumX Metrics

1984NE02      Phys.Lett. 134B, 290 (1984)

J.Nemeth, J.M.Irvine, J.Okolowicz

Rotationally Constrained Hartree-Fock Calculations and Nuclear Fission

NUCLEAR STRUCTURE ¹⁴⁴Nd; calculated fission barrier vs quadrupole constraint. Static Hartree-Fock method.

doi: 10.1016/0370-2693(84)90002-9
Citations: PlumX Metrics

1976AP01      Nucl.Phys. A272, 303 (1976)

B.Apagyi, G.Fai, J.Nemeth

Alpha Decay of Light Nuclei

NUCLEAR STRUCTURE ¹⁶O; calculated α-spectroscopic amplitudes, Γα of lowest 2+ levels. Zuker, Buck, McGrory shell-model wave functions.

doi: 10.1016/0375-9474(76)90333-X
Citations: PlumX Metrics

1976AP02      Nucl.Phys. A272, 317 (1976)

B.Apagyi, G.Fai, J.Nemeth

Calculation of the Parity Violating Alpha-Decay Width of ¹⁶O

NUCLEAR STRUCTURE ¹⁶O; calculated Γα of 8.87-MeV 2- level.

doi: 10.1016/0375-9474(76)90334-1
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1975MA33      Nucl.Phys. A251, 93 (1975)

R.Machleidt, K.Holinde, J.Nemeth

One-Boson-Exchange Potential and Structure of Finite Nuclei in the Local-Density Approximation

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated levels.

doi: 10.1016/0375-9474(75)90703-4
Citations: PlumX Metrics

1974NE06      Phys.Lett. 48B, 191 (1974)

J.Nemeth, G.Fai

The Hartree-Fock Lane Potential

NUCLEAR REACTIONS ⁴⁸Ca(p, p); measured nothing, calculated Lane potential.

doi: 10.1016/0370-2693(74)90006-9
Citations: PlumX Metrics

1973FA09      Nucl.Phys. A208, 463 (1973)

G.Fai, J.Nemeth

Density-Dependent Effective Interactions in Finite Nuclei (II)

NUCLEAR REACTIONS ¹⁶O, ^40,48Ca, ⁹⁰Zr, ²⁰⁸Pb(e, e'); calculated σ(θ), effect of the density dependence of effective forces.

doi: 10.1016/0375-9474(73)90668-4
Citations: PlumX Metrics

1972NE13      Nucl.Phys. A194, 329 (1972)

J.Nemeth, G.Ripka

Density-Dependent Effective Interactions in Finite Nuclei (I)

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁵⁶Ni, ²⁰⁸Pb; calculated binding energies, single-particle energies, rms radii, residual surface terms, Coulomb energies, spin-orbit energies. Hartree-Fock theory, density-dependent effective interactions.

doi: 10.1016/0375-9474(72)91043-3
Citations: PlumX Metrics

1971NE02      Phys.Lett. 34B, 117 (1971)

J.Nemeth, E.Gadioli Erba

The Validity of the Thomas Fermi Approximation

NUCLEAR STRUCTURE A=50-240; calculated nucleon density distributions. Thomas-Fermi method.

doi: 10.1016/0370-2693(71)90683-6
Citations: PlumX Metrics

1971NE09      Acta Phys. 30, 39 (1971)

J.Nemeth

The Effect of the Density Dependence of the Forces on First Order Finite Nuclear Calculations

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁴⁸Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated single-particle energies, nucleon, charge radii. Density-dependent forces.

1971NE10      Acta Phys. 30, 11 (1971)

J.Nemeth

A Simple Thomas-Fermi Model for Nuclei with Different Proton and Neutron Number

NUCLEAR STRUCTURE A=64, A=125, A=216; calculated neutron, proton density distributions. Modified Thomas-Fermi model.

1971NE18      Acta Phys. 30, 273 (1971)

J.Nemeth

Rearrangement Contribution to the Symmetry Energy and Single Particle Potential

1970NE13      Phys.Lett. 32B, 561 (1970)

J.Nemeth, D.Vautherin

Study of Finite Nuclei in the Local Density Approximation

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated binding energies, single-particle energies, mass distributions.

doi: 10.1016/0370-2693(70)90543-5
Citations: PlumX Metrics

1970NE15      Nucl.Phys. A156, 183 (1970)

J.Nemeth

Comparison of Hartree-Fock, Slater and Thomas-Fermi Approximations

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated single-particle energies, neutron, proton radii.

doi: 10.1016/0375-9474(70)91124-3
Citations: PlumX Metrics