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NSR database version of May 19, 2024.

Search: Author = P.Quentin

Found 110 matches.

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2022MI06      Phys.Rev. C 105, 044329 (2022)

N.Minkov, L.Bonneau, P.Quentin, J.Bartel, H.Molique, D.Ivanova

K-isomeric states in well-deformed heavy even-even nuclei

NUCLEAR STRUCTURE 234,236U, 236,238,240,244Pu, 244,246,248Cm, 248Cf, 248,250,256Fm, 252,254No; calculated levels, J, π, neutron and proton single-particle spectra, charge radii, quadrupole moments and magnetic moments for ground and isomeric states. Skyrme HF+BCS energy density functional with axial and parity symmetries, and with self-consistent blocking for the isomeric states. Comparison to experimental data.

doi: 10.1103/PhysRevC.105.044329
Citations: PlumX Metrics

2020QU03      Phys.Rev. C 102, 054305 (2020)

P.Quentin, J.Bartel

Collective coupling between pairing and rotational degrees of freedom within a simple model

NUCLEAR STRUCTURE 152Nd, 154Sm, 156Gd, 164Dy, 162,164,166,168,170,172Er, 174Yb, 170Hf, 178W, 230,232Th, 234,236U, 236,238,240,242Pu, 246,248Cm; calculated rotational energies as function of angular momentum, averaged neutron and proton gaps, kinematical moments of inertia as a function of angular frequency; deduced collective quenching of pairing correlations due to a global rotational motion. Chandrasekhar's S-ellipsoid model coupling intrinsic and global collective rotational currents, and yielding the Coriolis antipairing (CAP) quenching of pairing correlations. Comparison with experimental data.

doi: 10.1103/PhysRevC.102.054305
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2019NO05      Phys.Rev. C 99, 064306 (2019)

N.M.Nor, N.-A.Rezle, K.-W.Kelvin-Lee, M.-H.Koh, L.Bonneau, P.Quentin

Consistency of two different approaches to determine the strength of a pairing residual interaction in the rare-earth region

NUCLEAR STRUCTURE 156,157,158,159,160Sm, 159,161Eu, 160,161,162,163,164,165,166Gd, 161,163,165,167Tb, 162,163,164,165,166,167,168Dy, 167,169Ho, 168,169,170,171,172Er, 169,171,173Tm, 170,171,172,173,174,175,176,177,178Yb, 177,179Lu, 176,177,178,179,180,181,182Hf, 179Ta, 180W; analyzed odd-even staggering of binding energies, and moments of inertia of the first 2+ states of even-even nuclei; calculated neutron and proton pairing residual interaction strengths, binding energies, and moments of inertia. Self-consistent Hartree-Fock plus BCS framework, with the implementation of a self-consistent blocking in the case of odd-mass nuclei, using Skyrme SIII parametrization. Comparison with experimental values, and with other theoretical predictions.

doi: 10.1103/PhysRevC.99.064306
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2018RE14      J.Phys.(London) G45, 115102 (2018)

M.Rebhaoui, M.Imadalou, D.E.Medjadi, P.Quentin

Determination of a pairing residual interaction from Bohr quadrupole collective dynamics

NUCLEAR STRUCTURE 158Sm, 160Gd, 164Dy, 168Er, 172Yb, 180Hf; calculated B(E2) values. Comparison with available data.

doi: 10.1088/1361-6471/aae42a
Citations: PlumX Metrics

2017BE19      Phys.Rev. C 96, 034320 (2017)

K.Benrabia, D.E.Medjadi, M.Imadalou, P.Quentin

Triaxial quadrupole dynamics and the inner fission barrier of some heavy even-even nuclei

NUCLEAR STRUCTURE 236U, 240Pu, 248Cm, 252Cf; calculated potential energy surfaces in (β, γ) plane, positive-parity levels, J, ground, β and γ bands, potential energy surfaces as function of Q22, β and γ deformation parameters corresponding to axial inner barrier solution, rotational energies at the ground state deformation and at the axial saddle point, inner fission barrier heights with associated corrective terms. Hartree-Fock (HF) plus BCS collective dynamics approach, corresponding to β and γ degrees of freedom, with the SkM* Skyrme effective interaction, and a seniority force. Comparison with experimental data.

doi: 10.1103/PhysRevC.96.034320
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2017KO04      Phys.Rev. C 95, 014315 (2017)

M.-H.Koh, L.Bonneau, P.Quentin, T.V.Nhan Hao, H.Wagiran

Fission barriers of two odd-neutron actinide nuclei taking into account the time-reversal symmetry breaking at the mean-field level

NUCLEAR STRUCTURE 239Pu, 235U; calculated deformation-energy curves as function of Q20, inner-barrier heights, fission-isomeric energies, and outer-barrier heights, isomeric energies and intrinsic charge quadrupole moments in the fission isomeric well, levels, J, π, bands in the ground-state and isomeric wells. Hartree-Fock plus BCS approach with self-consistent particle blocking, using SkM*, SLy5* and SIII Skyrme parametrizations. Comparison with experimental data.

doi: 10.1103/PhysRevC.95.014315
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2016KO06      Eur.Phys.J. A 52, 3 (2016)

M.-H.Koh, D.D.Duc, T.V.Nhan Hao, T.L.Ha, P.Quentin, L.Bonneau

Band-head spectra of low-energy single-particle excitations in some well-deformed, odd-mass heavy nuclei within a microscopic approach

NUCLEAR STRUCTURE 234,236,238U, 237Np, 238,239Pu, 241Am, 242Cm; calculated band-head states, energy, J, inertia moment using HF plus BCS approach with blocking and two Skyrme interactions.

doi: 10.1140/epja/i2016-16003-8
Citations: PlumX Metrics

2015BO04      Phys.Rev. C 91, 054307 (2015)

L.Bonneau, N.Minkov, D.D.Duc, P.Quentin, J.Bartel

Effect of core polarization on magnetic dipole moments in deformed odd-mass nuclei

NUCLEAR STRUCTURE 99Sr, 99Y, 103Mo, 103Tc, 175Yb, 175Lu, 179Hf, 179Ta, 235U, 235,237Np; calculated binding energies, mass quadrupole moments, magnetic dipole moments, collective gyromagnetic factors, effective spin gyromagnetic factors; analyzed core-polarization effects. Skyrme-Hartree-Fock-BCS approach with selfconsistent blocking and time-odd terms of the Skyrme EDF. Seniority force in BCS calculations. Axial symmetry. Perturbative analysis of time-odd Hartree-Fock Hamiltonian and core-polarization effect on spin gyromagnetic factor. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.054307
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2015PO05      Phys.Rev. C 91, 054605 (2015)

K.Pomorski, B.Nerlo-Pomorska, P.Quentin

b decay of 252Cf in the transition from the exit point to scission

RADIOACTIVITY 252Cf(SF), (β-); calculated branching ratio for rare Fermi β- decay for 252Cf during the spontaneous fission process up to the scission point, nuclear dissipation. Classical dynamical approach.

NUCLEAR STRUCTURE 252Cf; calculated potential energy surface contours, Proton and neutron single-particle levels in the ground state and at the scission point. Macroscopic-microscopic calculations.

doi: 10.1103/PhysRevC.91.054605
Citations: PlumX Metrics

2014IM03      Phys.Scr. 89, 054025 (2014)

M.Imadalou, D.E.Medjadi, P.Quentin, L.Prochniak

Quadrupole collective dynamics of medium-heavy even-even nuclei within the highly truncated diagonalization approach

NUCLEAR STRUCTURE 102Zr, 104Mo, 110Ru, 110Pd; calculated energy surface vs deformations, energy vs quadrupole moment, levels, J, π, rotational bands using HF plus BCS and HTDA (Highly Truncated Diagonalization Approach). Compared with available data.

doi: 10.1088/0031-8949/89/5/054025
Citations: PlumX Metrics

2014NE03      Phys.Scr. 89, 054004 (2014)

B.Nerlo-Pomorska, K.Pomorski, P.Quentin, J.Bartel

Rotational bands in well deformed heavy nuclei

NUCLEAR STRUCTURE 230,232Th, 234,236,238U, 240,242Pu, 246Cm, 252No; calculated energy levels, J, π, rotational bands. Comparison with experimental data.

doi: 10.1088/0031-8949/89/5/054004
Citations: PlumX Metrics

2012HA17      Int.J.Mod.Phys. E21, 1250051 (2012)

T.V.Nhan Hao, J.Le Bloas, M.-H.Koh, L.Bonneau, P.Quentin

Further microscopic studies of the fission barriers of heavy nuclei

doi: 10.1142/S0218301312500516
Citations: PlumX Metrics

2012HA41      Phys.Rev. C 86, 064307 (2012)

T.V.Nhan Hao, P.Quentin, L.Bonneau

Parity restoration in the highly truncated diagonalization approach: Application to the outer fission barrier of 240Pu

NUCLEAR STRUCTURE 240Pu; calculated deformation energy curves around the isomeric state and the second barrier, outer fission barriers, octupole deformation curves of the projection on the positive states, Kπ=0+ fission isomer. Calculated octupole deformation properties for superdeformed state in 194Pb, and ground state in 222Ra. Particle number conserving pairing calculations with microscopic highly truncated diagonalization approach (HTDA) using Skyrme SkM* energy-density functional. Generalized Wick¬Ěs theorem.

doi: 10.1103/PhysRevC.86.064307
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2012LE12      Phys.Rev. C 86, 034332 (2012); Erratum Phys.Rev. C 91, 049901 (2015)

J.Le Bloas, L.Bonneau, P.Quentin, J.Bartel, D.D.Strottman

Effect of pairing correlations on the isospin-mixing parameter in deformed N=Z even-even nuclei

NUCLEAR STRUCTURE 28Si, 48Cr, 68Se, 76Sr; calculated isospin mixing parameters in the ground states. Particle-number conserving highly truncated diagonalization approach (HTDA) and Skyrme SIII effective interaction.

doi: 10.1103/PhysRevC.86.034332
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2012PR06      Int.J.Mod.Phys. E21, 1250036 (2012)

L.Prochniak, P.Quentin, M.Imadalou

Collective properties of stable even-even Cd isotopes

NUCLEAR STRUCTURE 106,108,110,112,114,116Cd; calculated level energies, J, π, B(E2). ATDHFB theory, comparison with available data.

doi: 10.1142/S021830131250036X
Citations: PlumX Metrics

2011BO08      Int.J.Mod.Phys. E20, 252 (2011)

L.Bonneau, J.Le Bloas, P.Quentin, N.Minkov

Effects of core polarization and pairing correlations on some ground-state properties of deformed odd-mass nuclei within the Higher Tamm-Dancoff approach

NUCLEAR STRUCTURE 23Na, 23,24,25Mg, 25Al, 48Cr; calculated binding energies, magnetic moments.

doi: 10.1142/S0218301311017594
Citations: PlumX Metrics

2011LE15      Int.J.Mod.Phys. E20, 274 (2011)

J.Le Bloas, L.Bonneau, P.Quentin, J.Bartel

Effects of pairing correlations on the isospin-symmetry-breaking correction to super-allowed O+ → O+ Fermi transitions with in the higher Tamm-Dancoff approach

RADIOACTIVITY 50Mn(β+); calculated isospin-symmetry breaking corrections.

NUCLEAR STRUCTURE 48Cr, 52Fe; calculated isospin-symmetry breaking corrections.

doi: 10.1142/S0218301311017624
Citations: PlumX Metrics

2011LE21      Phys.Rev. C 84, 014310 (2011)

J.Le Bloas, M.Koh, P.Quentin, L.Bonneau, J.I.A.Ithnin

Exact Coulomb exchange calculations in the Skyrme-Hartree-Fock-BCS framework and tests of the Slater approximation

NUCLEAR STRUCTURE 16O, 24Mg, 40,48Ca, 48Cr, 48,56Ni, 90Zr, 106Mo, 100,132Sn, 174,176,178Hf, 206,208,210Pb, 238U, 298Fl, 310126; Z=20-34, N=28; Z=40-58, N=64; Z=52-62, N=78; Z=68-80, N=106; Z=76-88, N=126; Z=86-100, N=146; calculated Coulomb interaction and fission properties for even-even nuclei within the Skyrme-Hartree-Fock/Bardeen-Cooper-Schrieffer approach. Pairing correlations. 70Se; calculated deformation energy curves. 212Po, 214Rn, 216Ra, 218Th; calculated α decay properties.

doi: 10.1103/PhysRevC.84.014310
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2010LA17      Nucl.Phys. A845, 33 (2010)

H.Laftchiev, J.Libert, P.Quentin, T.L.Ha

A particle-number conserving description of rotational correlated states

doi: 10.1016/j.nuclphysa.2010.04.014
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2010LA18      J.Phys.:Conf.Ser. 205, 012005 (2010)

H.Laftchiev, J.Libert, P.Quentin, T.L.Ha

Higher Tamm-Dankoff approximation for rotational nuclear states

NUCLEAR STRUCTURE 192,194Pb; calculated moments of inertia, pairing strength using Cr.HTDA (Cranking version of Higher Tamm-Dankoff approximation). Compared with data.

doi: 10.1088/1742-6596/205/1/012005
Citations: PlumX Metrics

2010LE06      Int.J.Mod.Phys. E19, 568 (2010)

J.Le Bloas, L.Bonneau, P.Quentin, J.Bartel, D.Strottman

Effects of vibrational and pairing correlations on isospin mixing in the Higher Tamm-Dancoff Approximation

doi: 10.1142/S0218301310014984
Citations: PlumX Metrics

2010NA05      Phys.Rev. C 81, 044320 (2010)

H.Naidja, P.Quentin, T.L.Ha, D.Samsoen

Pairing and vibrational correlations in the higher Tamm-Dancoff approximation (HTDA) approach

NUCLEAR STRUCTURE 40Ca; calculated excitation energies, EWSR, probabilities of different components of the correlated ground state and isoscalar giant quadrupole resonance (ISGQR) HTDA wave functions using higher Tamm-Dancoff Approximation for vibrational correlations with or without pairing.

doi: 10.1103/PhysRevC.81.044320
Citations: PlumX Metrics

2010QU01      Int.J.Mod.Phys. E19, 611 (2010)

P.Quentin, L.Bonneau, N.Minkov, D.Samsoen

Odd nuclei, time-reversal symmetry breaking, and magnetic polarization of the even-even core

NUCLEAR STRUCTURE 48,49Cr, 49Mn, 98,99Sr, 99Y, 102,103Mo, 103Tc, 174,175Yb, 175Lu, 178,179Hf, 179Ta, 234,235U, 235Np; calculated spin operators and quenching factors, core polarization of magnetic moments. Skyrme force parameterization.

doi: 10.1142/S0218301310015023
Citations: PlumX Metrics

2009BO22      Int.J.Mod.Phys. E18, 951 (2009)

L.Bonneau, J.Le Bloas, P.Quentin, J.Bartel, D.Strottman

Isospin mixing in the higher Tamm-Dancoff approximation

NUCLEAR STRUCTURE 16O, 40Ca, 56Ni, 100Sn; calculated mass excess; 100Sn; calculated isospin mixing.

doi: 10.1142/S0218301309013099
Citations: PlumX Metrics

2008QU02      Int.J.Mod.Phys. E17, 228 (2008)

P.Quentin, H.Naidja, L.Bonneau, J.Bartel, T.L.Ha

The higher TAMM-DANCOFF approximation theoretical context and phenomenological aspects

NUCLEAR STRUCTURE 40Ca; calculated quadrupole-quadrupole residual interaction parameters, odd-even mass differences and energy shifts using Higher Tamm-Dancoff approximation.

doi: 10.1142/S0218301308009732
Citations: PlumX Metrics

2007BO21      Phys.Rev. C 75, 064313 (2007)

L.Bonneau, P.Quentin, I.N.Mikhailov

Scission configurations and their implication in fission-fragment angular momenta

RADIOACTIVITY 252Cf(SF); calculated fission fragment spin distribution as a function of fragment total excitation energy using Skyrme-Hartree-Fock plus BCS-pairing formalism.

doi: 10.1103/PhysRevC.75.064313
Citations: PlumX Metrics

2007BO23      Phys.Rev. C 76, 014304 (2007)

L.Bonneau, P.Quentin, K.Sieja

Ground-state properties of even-even N = Z nuclei within the Hartree-Fock-BCS and higher Tamm-Dancoff approaches

NUCLEAR STRUCTURE A=56-100; calculated ground state properties for well deformed even-even N=Z nuclei using Hartree-Fock-BCS and Higher Tamm-Dancoff Approximation.

doi: 10.1103/PhysRevC.76.014304
Citations: PlumX Metrics

2007BO29      Phys.Rev. C 76, 024320 (2007)

L.Bonneau, P.Quentin, P.Moller

Global microscopic calculations of ground-state spins and parities for odd-mass nuclei

doi: 10.1103/PhysRevC.76.024320
Citations: PlumX Metrics

2007SI07      Int.J.Mod.Phys. E16, 289 (2007)

K.Sieja, T.L.Ha, P.Quentin, A.Baran

Particle number conserving approach to correlations

NUCLEAR STRUCTURE 64Ge; calculated ground-state configurations, pairing interactions. Higher TDA.

doi: 10.1142/S0218301307005727
Citations: PlumX Metrics

2006BA13      Int.J.Mod.Phys. E15, 553 (2006)

J.Bartel, K.Bencheikh, P.Quentin

Spin densities and currents in the Routhian approximation

NUCLEAR STRUCTURE 90Zr, 154Sm; calculated deformation vs angular momentum, spin densities and currents.

doi: 10.1142/S021830130600451X
Citations: PlumX Metrics

2006BE06      Nucl.Phys. A764, 79 (2006)

K.Bencheikh, J.Bartel, P.Quentin

Semiclassical description of finite fermion systems at finite temperature in a generalised Routhian approach

NUCLEAR STRUCTURE 90Zr; calculated proton and neutron contributions to moment of inertia. Semi-classical Extended Thomas Fermi approach.

doi: 10.1016/j.nuclphysa.2005.08.018
Citations: PlumX Metrics

2006SI35      Phys.Scr. T125, 220 (2006)

K.Sieja, A.Baran, P.Quentin

Skyrme force-like extension of the nuclear pairing interaction

NUCLEAR STRUCTURE 62,64,66,68Ge; calculated pair gap energies. 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40Ca, 44Ti, 48Cr, 52Fe, 56Ni, 60Zn, 64Ge, 68Se, 72Kr, 76Sr, 80Zr; calculated Wigner energy constant.

doi: 10.1088/0031-8949/2006/T125/060
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2005BA48      Int.J.Mod.Phys. E14, 437 (2005)

J.Bartel, K.Bencheikh, P.Quentin

Cranking of nuclei at finite temperature: A semiclassical approach

NUCLEAR STRUCTURE 90Zr; calculated proton and neutron contributions to moment of inertia, dependence on nuclear temperature. Extended Thomas Fermi theory.

doi: 10.1142/S0218301305003247
Citations: PlumX Metrics

2005BO29      Phys.Rev. C 72, 014311 (2005)

L.Bonneau, P.Quentin

Fission barriers and fission paths of the 70Se nucleus within a microscopic approach

NUCLEAR STRUCTURE 70Se; calculated fission barrier energies, fission paths, role of asymmetric deformation. Constrained Skyrme-Hartree-Fock plus BCS approach.

doi: 10.1103/PhysRevC.72.014311
Citations: PlumX Metrics

2005VE05      Int.J.Mod.Phys. E14, 751 (2005)

J.D.Vergados, P.Quentin, D.Strottman

Direct detection of supersymmetric dark matter: theoretical rates for transitions to excited states

NUCLEAR STRUCTURE 127I; calculated matrix elements, transition rate for interaction with light supersymmetric particle.

doi: 10.1142/S0218301305003508
Citations: PlumX Metrics

2004BA15      Int.J.Mod.Phys. E13, 225 (2004)

J.Bartel, K.Bencheikh, P.Quentin

Currents, spin densities and mean-field form factors in rotating nuclei: A semi-classical approach

NUCLEAR STRUCTURE 90Zr; calculated spin densities, form factors, deformation, related features. Semi-classical approach.

doi: 10.1142/S0218301304001989
Citations: PlumX Metrics

2004BO34      Eur.Phys.J. A 21, 391 (2004)

L.Bonneau, P.Quentin, D.Samsoen

Fission barriers of heavy nuclei within a microscopic approach

NUCLEAR STRUCTURE 230,232Th, 234,236U, 240Pu, 248,250,252,254,256Cf, 240,242,244,246,248,250,252,254,256,258,260,262,264Fm, 252,254,256No; calculated deformation energy, fission barrier features. Constrained Hartree-Fock plus pairing approach.

doi: 10.1140/epja/i2003-10224-x
Citations: PlumX Metrics

2004PR01      Nucl.Phys. A730, 59 (2004)

L.Prochniak, P.Quentin, D.Samsoen, J.Libert

A self-consistent approach to the quadrupole dynamics of medium heavy nuclei

NUCLEAR STRUCTURE 102Zr, 104Mo, 110Ru, 110Pd, 124Xe, 126Ba; calculated levels, J, π, deformation, B(E2). Self-consistent model, Skyrme forces.

doi: 10.1016/j.nuclphysa.2003.10.011
Citations: PlumX Metrics

2004QU01      Nucl.Phys. A734, 477 (2004)

P.Quentin, H.Laftchiev, D.Samsoen, I.N.Mikhailov, J.Libert

Pairing correlations in high spin states

NUCLEAR STRUCTURE 192Hg; calculated rotational bands moments of inertia, pairing correlation effects. Relativistic HFB and TDA approaches.

doi: 10.1016/j.nuclphysa.2004.01.130
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2004QU03      Phys.Rev. C 69, 054315 (2004)

P.Quentin, H.Lafchiev, D.Samsoen, I.N.Mikhailov

Simple model for the quenching of the moments of inertia due to pairing correlations in rigidly deformed rotational bands

NUCLEAR STRUCTURE 150Gd, 154Sm, 178Hf, 192Hg, 254No; calculated rotational bands moments of inertia, related parameters; deduced mechanism for quenching of pairing correlations.

doi: 10.1103/PhysRevC.69.054315
Citations: PlumX Metrics

2003LA02      Phys.Rev. C 67, 014307 (2003)

H.Laftchiev, D.Samsoen, P.Quentin, I.N.Mikhailov

Equivalence of pairing correlations and intrinsic vortical currents in rotating nuclei

NUCLEAR STRUCTURE 150Gd, 192Hg, 254No; calculated rotational bands moments of inertia, pairing correlations, collective vortical modes. 150Gd, 192Hg calculated superdeformed bands features. Comparisons with data.

doi: 10.1103/PhysRevC.67.014307
Citations: PlumX Metrics

2003PR15      Acta Phys.Pol. B34, 2461 (2003)

L.Prochniak, P.Quentin, D.Samsoen, J.Libert

Quadrupole collective excitations in medium heavy transitional nuclei with in a selfconsistent approach with Skyrme forces

NUCLEAR STRUCTURE 102Zr, 104Mo, 110Ru, 110Pd, 124Xe, 126Ba; calculated levels, J, B(E2), collective features. Comparison with data.

2003QU03      Nucl.Phys. A722, 395c (2003)

P.Quentin, H.Laftchiev, D.Samsoen, I.N.Mikhailov

Pairing correlations in high spin states

NUCLEAR STRUCTURE 192Hg; calculated rotational band moments of inertia, pair correlation effects.

doi: 10.1016/S0375-9474(03)01396-4
Citations: PlumX Metrics

2002PI01      Nucl.Phys. A697, 141 (2002)

N.Pillet, P.Quentin, J.Libert

Pairing Correlations in an Explicitly Particle-Number Conserving Approach

NUCLEAR STRUCTURE 178Hf; calculated pair correlation energies vs quadrupole moment, total deformation energy, level energies and configurations. Particle-number conserving approach.

doi: 10.1016/S0375-9474(01)01240-4
Citations: PlumX Metrics

2001LA27      Eur.Phys.J. A 12, 155 (2001)

H.Laftchiev, D.Samsoen, P.Quentin, J.Piperova

Hartree-Fock-Bogoliubov Calculations of the Rotational Band of the Very Heavy 254No Nucleus

NUCLEAR STRUCTURE 254No; calculated rotational band moment of inertia, single-particle Routhians, deformation. Hartree-Fock-Bogoliubov approach.

doi: 10.1007/s100500170023
Citations: PlumX Metrics

2001MI27      Yad.Fiz. 64, No 6, 1185 (2001); Phys.Atomic Nuclei 64, 1110 (2001)

I.N.Mikhailov, P.Quentin, Ch.Briancon

Angular Momentum of Fission Fragments

doi: 10.1134/1.1383626
Citations: PlumX Metrics

2001YU07      Ukr.J.Phys. 46, 21 (2001)

E.Kh.Yuldashbaeva, J.Libert, P.Quentin, M.Girod, B.K.Poluanov

Strong variations of adiabatic mass parameters

NUCLEAR STRUCTURE 110Cd, 148,150,152Gd, 238U; calculated pairing energies, mass parameters vs deformation.

2000KA45      Part. and Nucl., Lett. 98, 39 (2000)

V.G.Kartavenko, I.N.Mikhailov, T.I.Mikhailova, P.Quentin

On the Fermi-Surface Dynamics of Rotating Nuclei

1999MI29      Phys.Lett. 462B, 7 (1999)

I.N.Mikhailov, P.Quentin

On the Spin of Fission Fragments, An Orientation Pumping Mechanism

doi: 10.1016/S0370-2693(99)00891-6
Citations: PlumX Metrics

1999MI40      Eur.Phys.J. A 6, 399 (1999)

S.Misicu, Ph.Quentin

Semi-Microscopical Description of the Scission Configuration in the Neutronless Fission of 252Cf

RADIOACTIVITY 252Cf(SF); calculated scission configuration vs excitation energy, fragments total energy for neutronless fission. Molecular model.

doi: 10.1007/s100500050362
Citations: PlumX Metrics

1999PI05      Nucl.Phys. A652, 142 (1999)

J.Piperova, D.Samsoen, P.Quentin, K.Bencheikh, J.Bartel, J.Meyer

Bulk Properties of Rotating Nuclei and the Validity of Liquid Drop Model at Finite Angular Momenta

NUCLEAR STRUCTURE Z=20-98; calculated Routhians; deduced liquid-drop model parameters vs spin. 90Zr, 150Sm, 208Pb, 240Pu; calculated proton distribution radii, Coulomb energies. 236U; calculated fissility parameter vs spin.

doi: 10.1016/S0375-9474(99)00159-1
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1999SA19      Nucl.Phys. A652, 34 (1999)

D.Samsoen, P.Quentin, J.Bartel

Generalized Routhian Calculations within the Skyrme-Hartree-Fock Approximation

NUCLEAR STRUCTURE 80Sr, 150Gd; calculated moments of inertia, single-particle Routhians, quadrupole moments. Generalized Routhian calculations, Skyrme-Hartree-Fock approximation.

doi: 10.1016/S0375-9474(99)00134-7
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1999SA26      Phys.Rev. C60, 014301 (1999)

D.Samsoen, P.Quentin, I.N.Mikhailov

Period of the γ-ray Staggering in the 150Gd Superdeformed Region

NUCLEAR STRUCTURE 150Gd; calculated superdeformed bands moments of inertia; deduced possible mechanism for ΔI=4 staggering.

doi: 10.1103/PhysRevC.60.014301
Citations: PlumX Metrics

1999YU09      Phys.Lett. 461B, 1 (1999)

E.Kh.Yuldashbaeva, J.Libert, P.Quentin, M.Girod

Mass Parameters for Large Amplitude Collective Motion: A perturbative microscopic approach

NUCLEAR STRUCTURE 110Cd, 150Gd, 238U; calculated mass parameters, pairing energy vs deformation. Time-dependent HFB.

doi: 10.1016/S0370-2693(99)00836-9
Citations: PlumX Metrics

1998MI05      Eur.Phys.J. A 1, 229 (1998)

I.N.Mikhailov, P.Quentin

High-Spin Nuclear States and Persistent Currents in Mesoscopic Rings

doi: 10.1007/s100500050052
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1997MI23      Nucl.Phys. A627, 259 (1997)

I.N.Mikhailov, P.Quentin, D.Samsoen

Nuclear Intrinsic Vorticity and Its Coupling to Global Rotations

NUCLEAR STRUCTURE 190Hg; calculated high-spin rotational bands energies vs deformation, related features. Vortical collective motion.

doi: 10.1016/S0375-9474(97)00401-6
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1997PE04      Phys.Rev. C55, 1797 (1997)

S.Perries, D.Samsoen, J.Meyer, M.Meyer, P.Quentin

Collective Gyromagnetic Ratios and the Structure of Odd Superdeformed A = 190 Nuclei

NUCLEAR STRUCTURE 152Sm, 158Gd, 162Dy, 166Er, 174Yb, 178Hf, 182,184W, 188,190,192Os, 194Pt; calculated ground state collective gyromagnetic factors. 190,192,194,196,198,200Pb, 188,190,192,194,196,198Hg; calculated gyromagnetic ratios at superdeformed minima, (g(K)-g(R)/Q0)K. 193Hg, 193Pb, 193,195Tl; calculated superdeformed minima magnetic properties. Microsocopic approach.

doi: 10.1103/PhysRevC.55.1797
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1996BA49      Acta Phys.Pol. B27, 133 (1996)

J.Bartel, K.Bencheikh, E.Chabanat, J.Meyer, I.Mikhailov, J.Piperova, P.Quentin, D.Samsoen

Extended Thomas-Fermi Description of Rotating Nuclei

1996MI31      Fiz.Elem.Chastits At.Yadra 27, 303 (1996); Phys.Part.Nucl. 27, 121 (1996)

I.N.Mikhailov, Ch.Briancon, P.Quentin

Studies of Collective Currents in Nuclei

1995MI09      Phys.Rev.Lett. 74, 3336 (1995)

I.N.Mikhailov, P.Quentin

Band Staggering in Some Superdeformated States and Intrinsic Vortical Motion

doi: 10.1103/PhysRevLett.74.3336
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1994BE05      Nucl.Phys. A571, 518 (1994)

K.Bencheikh, P.Quentin, J.Bartel

Rotations in Nuclei - A Semiclassical Description

NUCLEAR STRUCTURE A ≤ 250; calculated moments of inertia. Semi-classical framework, rotating nuclei.

doi: 10.1016/0375-9474(94)90223-2
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1994BO15      Phys.Rev.Lett. 72, 2689 (1994)

N.Boos, F.Le Blanc, M.Krieg, J.Pinard, G.Huber, M.D.Lunney, D.Le Du, R.Meunier, M.Hussonnois, O.Constantinescu, J.B.Kim, Ch.Briancon, J.E.Crawford, H.T.Duong, Y.P.Gangrski, T.Kuhl, B.N.Markov, Yu.Ts.Oganessian, P.Quentin, B.Roussiere, J.Sauvage

Nuclear Properties of the Exotic High-Spin Isomer 178m2Hf from Collinear Laser Spectroscopy

RADIOACTIVITY 178mHf(IT) [from 176Yb(α, 2n), E=36 MeV]; measured hfs spectrum; deduced hyperfine parameters. 178Hf levels deduced charge rms radius difference, high spin isomer spectroscopic quadrupole moment.

doi: 10.1103/PhysRevLett.72.2689
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1994CH24      Phys.Lett. 325B, 13 (1994)

E.Chabanat, J.Meyer, K.Bencheikh, P.Quentin, J.Bartel

Equilibrium Deformations of Rotating Nuclei in a Self-Consistent Semiclassical Approach

NUCLEAR STRUCTURE 90Zr, 56Ni, 208Pb; calculated deformation to sphericity energies ratio. 90Zr; calculated extended Thomas-Fermi moment of inertia vs rotational energy frequency. Other nuclei also studied. Self-consistent semi-classical approach.

doi: 10.1016/0370-2693(94)90064-7
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1993BE31      Nucl.Phys. A557, 459c (1993)

K.Bencheikh, P.Quentin, J.Bartel, J.Meyer

A Semiclassical Description of Rapidly Rotating Nuclei

NUCLEAR STRUCTURE 16O, 56Ni, 90Zr, 140Ce, 240Pu, 202,208,214Pb, 116,132Sn; calculated moments of inertia. Extended Thomas-Fermi model, other Sn, Pb isotopes included.

doi: 10.1016/0375-9474(93)90562-C
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1992ME01      Phys.Rev. C45, 233 (1992)

M.Meyer, N.Redon, P.Quentin, J.Libert

Superdeformed Single-Particle Orbitals in the A = 190 Region from Hartree-Fock Plus BCS Calculations

NUCLEAR STRUCTURE 192,194,196,198,200Pb, 194,192,190Hg; calculated superdeformed nucleon state components, spectra; deduced particle number symmetry restoration role. Self-consistent axial Hartree-Fock plus BCS.

doi: 10.1103/PhysRevC.45.233
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1990GL02      Ann.Phys.(New York) 197, 205 (1990)

P.Gleissl, M.Brack, J.Meyer, P.Quentin

A Density Variational Approach to Nuclear Giant Resonances at Zero and Finite Temperature

NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 140Ce, 208Pb; calculated giant resonances, sum rule quantities. Density variational approach, zero, finite temperatures.

doi: 10.1016/0003-4916(90)90211-6
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1990KR11      Nucl.Phys. A517, 275 (1990)

S.J.Krieger, P.Bonche, H.Flocard, P.Quentin, M.S.Weiss

An Improved Pairing Interaction for Mean Field Calculations using Skyrme Potentials

NUCLEAR STRUCTURE 194Hg, 232Th; calculated total energy vs quadrupole moment. Mean field calculations, Skyrme potentials.

doi: 10.1016/0375-9474(90)90035-K
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1990QU01      Phys.Rev. C41, 341 (1990); Erratum Phys.Rev. C43, 361 (1991)

P.Quentin, N.Redon, J.Meyer, M.Meyer

Approximate Energy Correction for Particle Number Symmetry Breaking in Constrained Hartree-Fock plus BCS Calculations

NUCLEAR STRUCTURE 40Ca; calculated nucleon gap energies, deformation potential energy vs mass quadrupole moment. 106Cd; calculated deformation potential energy vs mass quadrupole moment. 92,94,96,98,100,102Zr; calculated proton quadrupole deformation parameter vs nucleon number. 196Pt, 240Pu; calculated axial deformation potential energy vs instrinsic quadrupole moment. Constrained Hartree-Fock plus BCS.

doi: 10.1103/PhysRevC.41.341
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1989BO24      Nucl.Phys. A500, 308 (1989)

P.Bonche, S.J.Krieger, P.Quentin, M.S.Weiss, J.Meyer, M.Meyer, N.Redon, H.Flocard, P.-H.Heenen

Superdeformation and Shape Isomerism at Zero Spin

NUCLEAR STRUCTURE 186,196,194,192,190,188,186,202,210Os, 200,198,196,194,192,190,188,186Pt, 194,202,210,218Hg; calculated Hartree-Fock energies, energy surfaces. 192,194,196,198,200,202,204,206,208,210,212,214,216,218Hg; calculated secondary minima deformations. 194,196,198Pt; calculated axial deformation energies. 66,68Ni, 190,192Pt, 206,208,210Os, 194,196,214Hg; deduced possible superdeformation effects. Microscopic Hartree-Fock plus BCS.

doi: 10.1016/0375-9474(89)90426-0
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1989DE44      Phys.Lett. 233B, 16 (1989)

I.Deloncle, J.Libert, L.Bennour, P.Quentin

The Low Energy Spectra of Heavy Transitional Even Nuclei from an Effective Nucleon-Nucleon Interaction

NUCLEAR STRUCTURE 74Ge, 76Se, 110Cd, 186Pt; calculated levels, potential energy surfaces. Adiabatic, time-dependent HFB theory.

doi: 10.1016/0370-2693(89)90608-4
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1988QU03      J.Phys.(London) G14, Supplement S47 (1988)

P.Quentin, L.Bennour, J.Libert, M.-G.Porquet, D.E.Medjadi, M.Meyer

Low-Energy Coupling of Individual and Collective Degrees of Freedom: A general microscopic approach

NUCLEAR STRUCTURE 234Pa, 238Np, 240,242,244Am, 248,250Bk; calculated levels; deduced coupling effects. Microscopic model.

doi: 10.1088/0305-4616/14/S/005
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1988RE08      Phys.Rev. C38, 550 (1988)

N.Redon, J.Meyer, M.Meyer, P.Quentin, P.Bonche, H.Flocard, P.-H.Heenen

Proton-Rich Exotic Heavy Nuclei: Self-consistent calculations

NUCLEAR STRUCTURE 92,96,98,100,102,104,106,108,110Cd; 142,140,138,136,134,132Sm; calculated potential energy surfaces; deduced deformation features.

doi: 10.1103/PhysRevC.38.550
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1987BE51      Nucl.Phys. A465, 35 (1987)

L.Bennour, J.Libert, M.Meyer, P.Quentin

A Self-Consistent Description of the Spectroscopic Properties of Odd-Odd Nuclei

NUCLEAR STRUCTURE 172Yb, 174Hf, 158Gd, 162Dy; calculated n, p single particle energies. 172,174Yb, 174,176Hf; calculated charge radii, quadrupole moments, charge distribution deformation parameter. 174Lu, 238Np, 160Tb; calculated levels, bandhead energies. Rotor plus two-quasiparticle model.

doi: 10.1016/0375-9474(87)90298-3
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1987GL08      J.Phys.(Paris), Colloq.C-2, 3 (1987)

P.Gleissl, M.Brack, J.Meyer, Ph.Quentin

Nuclear Giant Resonances in Coordinate Space - A Semiclassical Density Functional Approach

NUCLEAR STRUCTURE 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb; calculated isoscalar, isovector energies. A=20-235; calculated giant resonance energies vs mass. 40Ca, 90Zr, 208Pb; calculated sum rules, monopole energies. 208Pb; calculated giant resonance energies vs temperature. Semi-classical model.

1986DE28      Phys.Rev. C34, 1706 (1986)

J.de Bettencourt, Ch.Briancon, J.Libert, J.P.Thibaud, R.J.Walen, A.Gizon, M.Meyer, Ph.Quentin

Coulomb Excitation Study of 235U: Assessment of theoretical quasiparticle states

NUCLEAR REACTIONS 235U(84Kr, 84Kr'), E=370, 450 MeV; measured Eγ, Iγ, γγ-, γ(particle)-coin, Coulomb excitation. 235U deduced levels, band structure, J, π, γ-branching, Nilsson assigments, intraband B(λ), ground state band magnetic dipole, quadrupole moments. Enriched target, γ-ray spectroscopy. Rotor-plus-quasiparticle approach.

doi: 10.1103/PhysRevC.34.1706
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1986ME03      Phys.Lett. 172B, 122 (1986)

J.Meyer, J.Bartel, M.Brack, P.Quentin, S.Aicher

A Simple Gaussian Approximation for the One-Body Density Matrix

NUCLEAR STRUCTURE 40Ca, 208Pb; calculated defect function, proton distribution, total binding energies. 16O, 48Ca, 90Zr; calculated total binding energies. Gaussian density matrix approach.

doi: 10.1016/0370-2693(86)90820-8
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1986ME15      Phys.Lett. 181B, 185 (1986)

D.E.Medjadi, P.Quentin, M.Meyer, J.Libert

A Microscopic Approach to the Coupling of Collective and Individual Degrees of Freedom to Describe Low Energy Excitations of Odd-Even Nuclei

NUCLEAR STRUCTURE 107,109,110,111Cd; calculated levels. Microscopic approach, collective, individual degrees of freedom coupling.

doi: 10.1016/0370-2693(86)90028-6
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1986PO04      Nucl.Phys. A451, 365 (1986)

M-G.Porquet, J.Sauvage, M.Meyer, P.Quentin

Spectroscopic Properties of some Odd-A Re, Ir, and Au Isotopes: A self-consistent approach

NUCLEAR STRUCTURE 183,185,187Re, 183,185,187,189,191Au; calculated levels, B(λ). 185,189,191Ir; calculated levels, B(λ), μ. Rotor-plus-quasiparticle model, axial symmetry, Skyrme forces.

doi: 10.1016/0375-9474(86)90066-7
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1986RE15      Phys.Lett. 181B, 223 (1986)

N.Redon, J.Meyer, M.Meyer, P.Quentin, M.S.Weiss, P.Bonche, H.Flocard, P.-H.Heenen

A Self-Consistent Study of Triaxial Deformations in Heavy Nuclei

NUCLEAR STRUCTURE 138Sm, 186Pt, 192Os; calculated constant pairing matrix elements, potential energy surfaces. Lattice Hartree-Fock + BCS calculations.

doi: 10.1016/0370-2693(86)90036-5
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1985BA05      Phys.Lett. 152B, 29 (1985)

J.Bartel, P.Quentin

Fission Barriers of Excited Nuclei

NUCLEAR STRUCTURE 240Pu; calculated fission barrier vs temperature. Hartree-Fock approximation, finite temperature, Skyrme interaction.

doi: 10.1016/0370-2693(85)91132-3
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1985ME12      Nucl.Phys. A441, 291 (1985)

D.E.Medjadi, P.Quentin

A Simple Microscopic Approach for the Study of Giant Resonances

NUCLEAR STRUCTURE 16O, 40Ca; calculated levels, monopole, giant quadrupole resonances, transition densities, sum rules, collective wave functions. Generator coordinate method, Skyrme force parametrization.

doi: 10.1016/0375-9474(85)90035-1
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1984BO31      ATOMKI Kozlem. 26, 51 (1984)

C.Bourgeois, P.Kilcher, B.Roussiere, J.Sauvage, M.G.Porquet, M.Meyer, P.Quentin

Theoretical Description of 185Pt

NUCLEAR STRUCTURE 185Pt; calculated levels, quasirotational bands. Axial rotor plus quasiparticle model.

1984LE12      Phys.Rev. C30, 416 (1984)

G.A.Leander, J.Dudek, W.Nazarewicz, J.R.Nix, Ph.Quentin

Single-Particle Levels in the Doubly Magic 132Sn and 100Sn Nuclei

NUCLEAR STRUCTURE 56Ni, 100,132Sn, 208Pb; calculated single particle binding energies. Woods-Saxon, folded Yukawa, Skyrme interaction models.

doi: 10.1103/PhysRevC.30.416
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1983ME19      Phys.Lett. 133B, 279 (1983)

J.Meyer, P.Quentin, M.Brack

A Sum Rule Description of Giant Resonances at Finite Temperature

NUCLEAR STRUCTURE 208Pb; calculated isovector dipole, isoscalar monopole resonance energy vs temperature. Sum rule method.

doi: 10.1016/0370-2693(83)90146-6
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1982BA39      Nucl.Phys. A386, 79 (1982)

J.Bartel, P.Quentin, M.Brack, C.Guet, H.-B.Hakansson

Towards a Better Parametrisation of Skyrme-Like Effective Forces: A critical study of the SkM Force

NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 114,132Sn, 140Ce, 208Pb; calculated rms charge radii, Hartree-Fock, extended Thomas-Fermi binding energies. 90Zr, 208Pb, 166Er, 240Pu; calculated neutron, proton single particle levels. 166Er, 240Pu; calculated rms charge radii, quadrupole, hexadecapole moments. 240Pu calculated fission barrier. Hartree-Fock plus BCS, Skyrme type forces.

doi: 10.1016/0375-9474(82)90403-1
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1982LI01      Phys.Rev. C25, 571 (1982)

J.Libert, P.Quentin

Self-Consistent Description of Heavy Nuclei. I. Static Properties of Some Even Nuclei

NUCLEAR STRUCTURE 224Ra, 230,232Th, 232,234,236,238U, 238,240,244Pu, 244,248Cm, 252Cf, 258Fm, 260Rf; calculated binding energy, charge radii, quadrupole, hexadecapole moments, single particle energies. Hartree-Fock plus BCS, Skyrme forces.

doi: 10.1103/PhysRevC.25.571
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1982LI02      Phys.Rev. C25, 586 (1982)

J.Libert, M.Meyer, P.Quentin

Self-Consistent Description of Heavy Nuclei. II. Spectroscopic Properties of Some Odd Nuclei

NUCLEAR STRUCTURE 229,231,233Th, 237,239,241Pu, 233,235,237,239U, 233,235,237,239Np; calculated levels. 229Th, 233,235U, 239,241Pu, 231,233Pa, 237,239Np, 241Am; calculated μ, quadrupole moment. 229Th, 233U, 231Pa, 237Np, 239Pu calculated B(λ), δ. 235U calculated B(λ). Rotor plus quasiparticle model, self-consistent approach.

doi: 10.1103/PhysRevC.25.586
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1982LI11      Z.Phys. A306, 315 (1982)

J.Libert, P.Quentin

A General Solution of the Bohr Collective Hamiltonian

NUCLEAR STRUCTURE 154,156,158Er, 232Th; calculated levels, potential energy surfaces. Collective Hamiltonian.

doi: 10.1007/BF01432372
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1982ME08      Nucl.Phys. A385, 269 (1982)

J.Meyer, P.Quentin, B.K.Jennings

The Isovector Dipole Mode: A simple sum rule approach

NUCLEAR REACTIONS 16O, 40Ca, 208Pb(γ, X), E not given; calculated σ(photoabsorption). Sum rules, different models.

doi: 10.1016/0375-9474(82)90172-5
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1981SA31      Nucl.Phys. A370, 231 (1981)

J.Sauvage-Letessier, P.Quentin, H.Flocard

Deformation Properties of Osmium, Platinum, Mercury Isotopes from Self-Consistent Calculations: Influence of the pairing treatment

NUCLEAR STRUCTURE 184,188,192,196Os, 182,184,186,188,190,192,196Pt, 180,184,186,188,190,192,200Hg; calculated binding energies, deformation parameters β2, β4, rms charge radii, neutron, proton pairing gaps; 184,188,192Os, 196Pt, 200Hg; calculated quadrupole moment. Hartree-Fock, BCS, Skyrme interaction.

doi: 10.1016/0375-9474(81)90074-9
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1980GI05      Phys.Rev. C21, 2076 (1980)

M.J.Giannoni, P.Quentin

Mass Parameters in the Adiabatic Time-Dependent Hartree-Fock Approximation. II. Results for the Isoscalar Quadrupole Mode

NUCLEAR STRUCTURE 12C, 16O, 40,48Ca, 56Ni, 90Zr, 140Ce, 208Pb; calculated T=0, quadrupole mode mass parameters, deformation energy. Adiabatic time-dependent Hartree-Fock, Skyrme type interactions.

doi: 10.1103/PhysRevC.21.2076
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1980LI15      Phys.Lett. B95, 175 (1980)

J.Libert, M.Meyer, P.Quentin

Spectroscopic Properties of 237,239Pu Fission Isomers from Self-Consistent Calculations

NUCLEAR STRUCTURE 237,239Pu; calculated levels, B(λ), fission isomer spectroscopic properties. Rotor plus quasiparticle model, self-consistent single particle states.

doi: 10.1016/0370-2693(80)90463-3
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1980QU01      Z.Phys. A298, 37 (1980)

P.Quentin, I.Brissaud, R.de Swiniarski

The Determination of Hexadecapole Deformation Parameters in Actinide Nuclei and Their Variation Near the Nuclear Surface

NUCLEAR STRUCTURE 238U; calculated nuclear density; deduced hexadecapole deformation β dependence on nuclear surface. Self-consistent calculation, Skyrme forces.

doi: 10.1007/BF01416026
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1979BO04      Phys.Lett. 82B, 5 (1979)

P.Bonche, H.Doubre, P.Quentin

Adiabatic Analysis of Time-Dependent Hartree-Fock Solutions in the Testing Case of Vibrating Nuclei

NUCLEAR STRUCTURE 16O, 40Ca; calculated time evolution of Baranger-Veneroni operator chi for T=0, monopole, quadrupole vibration. time-dependent Hartree-Fock method.

doi: 10.1016/0370-2693(79)90411-8
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1979ME02      Nucl.Phys. A316, 93 (1979)

M.Meyer, J.Daniere, J.Letessier, P.Quentin

A Description of Odd Neutron-Deficient Cadmium Isotopes within the Rotor-Plus-Particle Model Using Self-Consistent Core Single-Particle States

NUCLEAR STRUCTURE 98,102,106,110Cd; calculated spectroscopic properties. Self-consistent core single-particle states, rotor-plus-particle model.

doi: 10.1016/0375-9474(79)90674-2
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1979SP05      Nucl.Phys. A326, 37 (1979)

D.W.L.Sprung, S.G.Lie, M.Vallieres, P.Quentin

Collective Gyromagnetic Ratio and Moment of Inertia from Density-Dependent Hartree-Fock Calculations

NUCLEAR STRUCTURE A=152-258; calculated gyromagnetic ratio, moment of inertia. Density-dependent Hartree-Fock calculations, Skyrme interaction. Axially symmetric even-even nuclei.

doi: 10.1016/0375-9474(79)90364-6
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1976GI11      Phys.Lett. 65B, 305 (1976)

M.J.Giannoni, F.Moreau, P.Quentin, D.Vautherin, M.Veneroni, D.M.Brink

A Method for Calculating Adiabatic Mass Parameters: Application to Isoscalar Quadrupole Modes in Light Nuclei

NUCLEAR STRUCTURE 12C; calculated quadrupole mass.

doi: 10.1016/0370-2693(76)90227-6
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1975BE05      Nucl.Phys. A238, 29 (1975)

M.Beiner, H.Flocard, Nguyen Van Giai, P.Quentin

Nuclear Ground-State Properties and Self-Consistent Calculations with the Skyrme Interaction (I). Spherical Description

NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 140Ce, 208Pb; calculated levels, binding energies. 152Sm, 158Gd, 162Dy, 166Er, 174Yb, 178Hf, 184W, 190Os; calculated binding energy.

doi: 10.1016/0375-9474(75)90338-3
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1975BR18      Phys.Lett. 56B, 421 (1975)

M.Brack, P.Quentin

Self-Consistent Average Density Matrices and the Strutinsky Energy Theorem

NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 168Yb, 208Pb; calculated ground state energy. Skyrme force.

doi: 10.1016/0370-2693(75)90401-3
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1974BR32      Phys.Lett. 52B, 159 (1974)

M.Brack, P.Quentin

Selfconsistent Calculations of Highly Excited Nuclei

NUCLEAR STRUCTURE 208Pb; calculated temperature dependence of proton levels. 168Yb; calculated deformation energy.

doi: 10.1016/0370-2693(74)90077-X
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