NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = H.Flocard Found 76 matches. 2007SE03 Phys.Rev. C 75, 064303 (2007) A.P.Severyukhin, M.Bender, H.Flocard, P.-H.Heenen Large-amplitude Qn-Qp collectivity in the neutron-rich oxygen isotope 20O NUCLEAR STRUCTURE 20O; calculated single particle energies and deformation parameters using HFB model and SLy4 parameterization of Skyrme interaction.
doi: 10.1103/PhysRevC.75.064303
2007SE10 Phys.Atomic Nuclei 70, 1435 (2007) A.P.Severyukhin, M.Bender, H.Flocard, P.-H.Heenen On the Qn-Qp deformation energy surfaces of neutron-rich oxygen isotopes
doi: 10.1134/S1063778807080182
2003BE53 Phys.Rev. C 68, 044321 (2003) M.Bender, H.Flocard, P.-H.Heenen Beyond-mean-field-model analysis of low-spin normal-deformed and superdeformed collective states of 32S, 36Ar, 38Ar, and 40Ca NUCLEAR STRUCTURE 32S, 36,38Ar, 40Ca; calculated levels, J, π, quadrupole moments, B(E2), normal and superdeformed rotational band features, configuration mixing. Comparison with data.
doi: 10.1103/PhysRevC.68.044321
2001HE32 Eur.Phys.J. A 11, 393 (2001) P.-H.Heenen, A.Valor, M.Bender, P.Bonche, H.Flocard GCM Analysis of the Collective Properties of Lead Isotopes with Exact Projection on Particle Numbers NUCLEAR STRUCTURE 204,206,208,210,212Pb; calculated low-lying levels, J, π, configurations, wave functions, binding energy, two-neutron separation energy. Hartree-Fock + BCS model.
doi: 10.1007/s100500170051
1999DA30 Nucl.Phys. (Supplement) A654, 655c (1999) H.Dancer, S.Perries, P.Bonche, H.Flocard, P.-H.Heenen, J.Meyer, M.Meyer Generator Coordinate Method and Superdeformation in A = 190 Nuclei NUCLEAR STRUCTURE 190,192,194,196Hg, 192,194,196,198Pb; calculated E0, E2 transition rates for decay out of superdeformed bands; deduced E2 transition dominance.
doi: 10.1016/S0375-9474(00)88520-6
1999RI07 Phys.Rev. C59, 3120 (1999) C.Rigollet, P.Bonche, H.Flocard, P.-H.Heenen Microscopic Study of the Properties of Identical Bands in the A = 150 Mass Region NUCLEAR STRUCTURE 151,152,153,154Dy, 150Gd, 151Tb; calculated superdeformed bands moments of inertia; deduced identical band features. Cranked mean-field approach, Skyrme force, density-dependent pairing.
doi: 10.1103/PhysRevC.59.3120
1998DA20 Phys.Rev. C58, 2068 (1998) H.Dancer, P.Bonche, H.Flocard, P.-H.Heenen, J.Meyer, M.Meyer Monopole Strength and Decay Out of Superdeformed Bands in the A = 190 Mass Region from Theories Beyond the Mean Field NUCLEAR STRUCTURE 190,192,194,196,198Hg, 192,194,196,198,200Pb; calculated E0, E2 transition rates from superdeformed bands; deduced E2 transitions dominance. Generator coordinate method, comparison with two-level model.
doi: 10.1103/PhysRevC.58.2068
1998NA18 Phys.Lett. 429B, 15 (1998) F.Naulin, J.-Y.Zhang, H.Flocard, D.Vautherin, P.H.Heenen, P.Bonche Radius Evolution of Sodium Isotopes in Mean-Field and Generator Coordinate Methods NUCLEAR STRUCTURE 20,21,22,23,24,25,26Na; calculated neutron, proton radii. Mean-field, generator coordinate methods. Comparison with data.
doi: 10.1016/S0370-2693(98)00428-6
1997KR10 Phys.Rev.Lett. 79, 2217 (1997) A.T.Kruppa, P.-H.Heenen, H.Flocard, R.J.Liotta Particle-Unstable Nuclei in the Hartree-Fock Theory NUCLEAR STRUCTURE 6,8,10He, 10C, 12,14,16,22,24,26,28O; calculated binding energies. 10He, 12,26,28O; calculated ground state decay widths. Complex scaled Hartree-Fock procedure, Skyrme effective interactions, several parametrizations compared.
doi: 10.1103/PhysRevLett.79.2217
1997TE04 Phys.Rev. C55, 1231 (1997) J.Terasaki, H.Flocard, P.-H.Heenen, P.Bonche Superdeformed Bands of Odd Nuclei in A = 190 Region in the Quasiparticle Picture NUCLEAR STRUCTURE 195Pb, 193Hg; calculated superdeformed bands related features; deduced density-dependent pairing forces advantages. Cranked HFB model.
doi: 10.1103/PhysRevC.55.1231
1997TE08 Nucl.Phys. A621, 706 (1997) J.Terasaki, H.Flocard, P.-H.Heenen, P.Bonche Deformation of Nuclei Close to the Two-Neutron Drip Line in the Mg Region NUCLEAR STRUCTURE 22,24,26,28,30,32,34,36,38,40Mg; calculated two-neutron separation energies, deformation parameter, quadrupole moments, rms radii. 34Ne, 42,46Si; calculated deformation energy curves. HFB calculation, Skyrme forces.
doi: 10.1016/S0375-9474(97)00183-8
1997TE19 Acta Phys.Hung.N.S. 6, 201 (1997) J.Terasaki, H.Flocard, P.H.Heenen, P.Bonche Deformation of Nuclei Close to the Two-Neutron Drip Line in Mg Region NUCLEAR STRUCTURE 20,22,24,26,28,30,32,34,36,38,40Mg; calculated ground-state deformation; deduced quenching of N=28 shell effect. HFB calculations, Skyrme forces.
1996BO06 Nucl.Phys. A598, 169 (1996) P.Bonche, H.Flocard, P.-H.Heenen Microscopic Study of Superdeformation in the A = 150 Mass Region NUCLEAR STRUCTURE 160Gd, 151,152Dy, 151Tb; calculated nucleon pairing energies, particle routhians, dynamical moments of inertia for superdeformed bands; deduced method suitability for subtle phenomena studies. Cranked HFB method.
doi: 10.1016/0375-9474(95)00491-2
1996KR14 Phys.Rev. C54, 2399 (1996) S.J.Krieger, P.Bonche, H.Flocard, P.H.Heenen, R.Mehrem, M.S.Weiss Generator Coordinate Method Calculation of the E2 Decay Lifetime of Shape Isomers in the Actinide Region NUCLEAR STRUCTURE 236,238,240Pu; calculated nonconstrained, constrained HF-BCS quadrupole deformation energy, quadrupole moments at different minima and barriers, proton quadrupole transition matrix elements, E2-decay T1/2 for shape isomers. Generator coordinate method.
doi: 10.1103/PhysRevC.54.2399
1996TE06 Nucl.Phys. A600, 371 (1996) J.Terasaki, P.-H.Heenen, H.Flocard, P.Bonche 3D Solution of Hartree-Fock-Bogoliubov Equations for Drip-Line Nuclei NUCLEAR STRUCTURE 52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88,90,92,94Ni; calculated two-neutron separation energies. 84Ni; calculated nucleon densities, neutron pairing gap vs radius. 92Ni; calculated potential energy curve, total energy. HFB method, 3D-solution.
doi: 10.1016/0375-9474(96)00036-X
1995HE12 Nucl.Phys. A588, 490 (1995) P.-H.Heenen, P.Bonche, H.Flocard Microscopic Study of Superdeformation in 193Hg NUCLEAR STRUCTURE 193Hg; calculated superdeformed bands dynamical moment of inertia. Cranked HFB method.
doi: 10.1016/0375-9474(95)00064-8
1995ME07 Nucl.Phys. A588, 597 (1995) J.Meyer, P.Bonche, M.S.Weiss, J.Dobaczewski, H.Flocard, P.-H.Heenen Quadrupole and Octupole Correlations in Normal, Superdeformed and Hyperdeformed States of 194Pb NUCLEAR STRUCTURE 192,194,196,198,200Pb; calculated superdeformed band population evolution, spectra, energy curves vs quadrupole moment, quadrupole, octupole correlations in normal, hyperdeformed bands as well. Generator coordinate method.
doi: 10.1016/0375-9474(95)00055-6
1995RE03 Nucl.Phys. A584, 467 (1995) Nuclear Effective Forces and Isotope Shifts NUCLEAR STRUCTURE 198,200,202,204,206,208,210,214Pb; calculated rms charge neutron radii; analyzed isotope shifts for some of the isotopes of Pb, Ca, Sr; deduced interactions spin-orbit term role.
doi: 10.1016/0375-9474(94)00770-N
1995TE03 Nucl.Phys. A593, 1 (1995) J.Terasaki, P.-H.Heenen, P.Bonche, J.Dobaczewski, H.Flocard Superdeformed Rotational Bands with Density Dependent Pairing Interactions NUCLEAR STRUCTURE 190,192,194Hg, 194Pb; calculated superdeformed bands charge quadrupole moments, nucleon quasi particle routhians, dynamic moments of inertia. 150Gd; calculated dynamic moments of intertia.
doi: 10.1016/0375-9474(95)00316-S
1994BO24 Nucl.Phys. A574, 185c (1994) P.Bonche, E.Chabanat, B.Q.Chen, J.Dobaczewski, H.Flocard, B.Gall, P.H.Heenen, J.Meyer, N.Tajima, M.S.Weiss Microscopic Approach to Collective Motion NUCLEAR STRUCTURE 192Hg, 194Pb; calculated superdeformed bands, energies, quadrupole moments, dynamical, rigid body moments of inertia, Eγ. 194,196,198,200,202,204,206,208,210,212,214,216,218,220Pb; calculated proton, neutron rms radii. Microscopic approach, collective motion.
doi: 10.1016/0375-9474(94)90045-0
1994GA22 Z.Phys. A348, 183 (1994) B.Gall, P.Bonche, J.Dobaczewski, H.Flocard, P.-H.Heenen Superdeformed Rotational Bands in the Mercury Region. A Cranked Skyrme-Hartree-Fock-Bogoliubov Study NUCLEAR STRUCTURE 190,192,194Hg, 194Pb; calculated superdeformed bands moment of inertia, proton, neutron pairing energies, charge quadrupole moments versus angular velocity. Cranked Skyrme-Hartree-Fock-Bogoliubov method.
doi: 10.1007/BF01291916
1994HE23 Phys.Rev. C50, 802 (1994) P.-H.Heenen, J.Skalski, P.Bonche, H.Flocard Octupole Excitations in Light Xenon and Barium Nuclei NUCLEAR STRUCTURE 111,112,113Xe, 113,114,115Ba; calculated levels, B(λ); deduced dynamical correlations role in octupole collectivity enhancement. Hartree-Fock+BCS, generator coordinate methods.
doi: 10.1103/PhysRevC.50.802
1994KR06 Nucl.Phys. A572, 384 (1994) S.J.Krieger, P.Bonche, H.Flocard, P.H.Heenen, M.S.Weiss GCM Calculation of the E2 Decay Lifetimes of Shape Isomers NUCLEAR STRUCTURE 230,232Th, 238U; calculated deformation energy vs mass quadrupole moment, first barrier, second minimum, absolute miminum quadrupole moment, charge quadrupole transition matrix element between superdeformed, ground bands, isomer E2 decay T1/2. Hartree-Fock BCS calculations.
doi: 10.1016/0375-9474(94)90181-3
1993FL04 Nucl.Phys. A557, 559c (1993) H.Flocard, B.Q.Chen, B.Gall, P.Bonche, J.Dobaczewski, P.H.Heenen, M.S.Weiss Hartree-Fock and Hartree-Fock-Bogoliubov Calculations of Superdeformed Bands NUCLEAR STRUCTURE 192,194Hg, 194Pb; calculated superdeformed bands quadrupole moments, dynamical, rigid body moments of inertia. Hartree-Fock, HFB calculations, limitations discussed.
doi: 10.1016/0375-9474(93)90569-J
1993HE12 Nucl.Phys. A561, 367 (1993) P.-H.Heenen, P.Bonche, J.Dobaczewski, H.Flocard Generator-Coordinate Method for Triaxial Quadrupole Dynamics in Sr Isotopes (II). Results for Particle-Number-Projected States NUCLEAR STRUCTURE 78,80,82,84,86,88Sr; calculated levels, isotope shifts, binding energies. Generator coordinate method, quadrupole triaxial HFBCS states.
doi: 10.1016/0375-9474(93)90017-R
1993SK01 Nucl.Phys. A551, 109 (1993) J.Skalski, P.-H.Heenen, P.Bonche, H.Flocard, J.Meyer Octupole Correlations in Superdeformed Mercury and Lead Nuclei: A generator-coordinate method analysis NUCLEAR STRUCTURE 194Pb, 194,192Hg; calculated axial, nonaxial octupole level energies built on superdeformed states, B(λ); deduced weak coupling. Generator coordinate method, self-consistent Hartree-Fock BCS basis.
doi: 10.1016/0375-9474(93)90306-I
1993SK02 Acta Phys.Pol. B24, 413 (1993) J.Skalski, P.-H.Heenen, P.Bonche, H.Flocard Shape Transition and Collective Dynamics in Even 94-100Zr Nuclei NUCLEAR STRUCTURE 94,96,98,100Zr; calculated Hartree-Fock energies, levels, E0 transition strength. Microscopic generator coordinate method.
1993TA01 Nucl.Phys. A551, 409 (1993) N.Tajima, H.Flocard, P.Bonche, J.Dobaczewski, P.-H.Heenen Diabatic Effects in 186Pb: A generator-coordinate analysis NUCLEAR STRUCTURE 186Pb; calculated pairing gaps, potential energy curves vs mass quadrupole moment. Hartree-Fock+BCS basis, generator coordinate method.
doi: 10.1016/0375-9474(93)90455-7
1993TA02 Nucl.Phys. A551, 434 (1993) N.Tajima, P.Bonche, H.Flocard, P.-H.Heenen, M.S.Weiss Self-Consistent Calculation of Charge Radii of Pb Isotopes NUCLEAR STRUCTURE 194,202,214,220Pb; calculated charge radii. Hartree-Fock+BCS method, Skyrme forces.
doi: 10.1016/0375-9474(93)90456-8
1992CH32 Phys.Rev. C46, R1582 (1992) B.-Q.Chen, P.-H.Heenen, P.Bonche, M.S.Weiss, H.Flocard Observation of Identical Bands in Superdeformed Nuclei with the Cranked Hartree-Fock Method NUCLEAR STRUCTURE 194,192Hg, 194Pb; calculated superdeformed band level energies, quadrupole moments, dynamical, rigid moments of inertia; deduced twinning characteristics. Cranked Hartree-Fock, Skyrme effective interaction.
doi: 10.1103/PhysRevC.46.R1582
1992KR07 Nucl.Phys. A542, 43 (1992) S.J.Krieger, P.Bonche, M.S.Weiss, J.Meyer, H.Flocard, P.-H.Heenen Super-Deformation and Shape Isomerism: Mapping the isthmus NUCLEAR STRUCTURE Z=108-152; calculated excitation energy, rigid moment of inertia. 190,192,194,196,198,200,202,204,206,210,212,214,216,218,220,222,224,226,228,230Pb calculated rigid moment of inertia, quadrupole moment, superdeformed isomers; deduced shape isomerism isthmus superdeformation region. Microscopic Hartree-Fock-BCS formalism.
doi: 10.1016/0375-9474(92)90395-Z
1991BE10 Phys.Rev. C43, 2200 (1991) Pairing Effects in Nuclear Collective Motion: Generator Coordinate Method NUCLEAR STRUCTURE 190,198Hg; calculated off-diagonal quadrupole matrix elements. 194Hg; calculated collective levels. Hartree-Fock based hopping model.
doi: 10.1103/PhysRevC.43.2200
1991BO07 Nucl.Phys. A523, 300 (1991) P.Bonche, H.Flocard, P.-H.Heenen Cranked Hartree-Fock Study of the Yrast Line of 80Sr NUCLEAR STRUCTURE 80Sr; calculated levels, quadrupole moments, superdeformed bands. Cranked Hartree-Fock.
doi: 10.1016/0375-9474(91)90005-Q
1991BO19 Phys.Rev.Lett. 66, 876 (1991) P.Bonche, S.J.Krieger, M.S.Weiss, J.Dobaczewski, H.Flocard, P.-H.Heenen Octupole Softness of Superdeformed 194Pb NUCLEAR STRUCTURE 194Pb; analyzed data; deduced band structure, superdeformed softness features. Generator coordinate method, pairing projection.
doi: 10.1103/PhysRevLett.66.876
1991BO27 Nucl.Phys. A530, 149 (1991) P.Bonche, J.Dobaczewski, H.Flocard, P.-H.Heenen Generator Coordinate Method for Triaxial Quadrupole Collective Dynamics in Strontium Isotopes NUCLEAR STRUCTURE 78,80,82,84,86,88Sr; calculated ground state energy, probability densities, levels, isotope shifts, potential energy surfaces. Generator coordinate method.
doi: 10.1016/0375-9474(91)90760-4
1991ME07 Nucl.Phys. A533, 307 (1991) J.Meyer, P.Bonche, J.Dobaczewski, H.Flocard, P.H.Heenen Pairing Vibrations and Stability of Superdeformed States NUCLEAR STRUCTURE 194Hg; calculated levels, quadrupole moments; deduced pairing vibrations role in superdeformed state stability.
doi: 10.1016/0375-9474(91)90492-O
1990AB13 Ann.Rev.Nucl.Part.Sci. 40, 439 (1990) S.Aberg, H.Flocard, W.Nazarewicz Nuclear Shapes in Mean Field Theory NUCLEAR STRUCTURE 188Os; 154Sm; 74,76,78,80,82,84Sr; 96,98,100Zr; compiled, evaluated energy surfaces. 182,184,186W; compiled, reviewed shape variables related features. 158,160,162,164,166,168Yb; compiled, evaluated data. 212Rn; compiled, evaluated spectra. 151,152,153Dy, 150,151Tb, 146,148,149,150Gd; compiled, evaluated superdeformed bands data. 180,182,184,186,188,190,192,194Hg; analyzed prolate-oblate energy difference. 186,188,190,192,194,196,198,200,202,204,206Pb; analyzed level data. Other aspects, nuclei discussed.
doi: 10.1146/annurev.ns.40.120190.002255
1990BO14 Nucl.Phys. A510, 466 (1990) P.Bonche, J.Dobaczewski, H.Flocard, P.-H.Heenen, J.Meyer Analysis of the Generator Coordinate Method in a Study of Shape Isomerism in 194Hg NUCLEAR STRUCTURE 194Hg; calculated deformation energy, large amplitude quadrupole dynamics. Collective BCS basis states, generator coordinate method.
doi: 10.1016/0375-9474(90)90062-Q
1990BO40 Nucl.Phys. A519, 509 (1990) P.Bonche, J.Dobaczewski, H.Flocard, P.H.Heenen, S.J.Krieger, J.Meyer, M.S.Weiss Quadrupole Collective Correlations and the Depopulation of the Superdeformed Bands in Mercury NUCLEAR STRUCTURE 190,192,194,196,198Hg; calculated deformation energy, wave functions, proton quadrupole moments, superdeformed band decay Iγ. Self-consistent generator coordinate method, Hartree-Fock plus BCS wave functions.
doi: 10.1016/0375-9474(90)90443-P
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
1989BE35 Phys.Rev. C40, 2834 (1989) L.Bennour, P.-H.Heenen, P.Bonche, J.Dobaczewski, H.Flocard Charge Distributions of 208Pb, 206Pb, and 205Tl and the Mean-Field Approximation NUCLEAR STRUCTURE 208,206Pb, 205Tl; calculated charge distributions. Hartree-Fock, Hartree-Fock plus BCS formalisms, Skyrme interaction. NUCLEAR REACTIONS 206Pb, 205Tl(e, e), E not given; calculated σ ratio vs momentum transfer.
doi: 10.1103/PhysRevC.40.2834
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
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
1987BO13 Nucl.Phys. A467, 115 (1987) P.Bonche, H.Flocard, P.H.Heenen Self-Consistent Calculation of Nuclear Rotations: The complete yrast line of 24Mg NUCLEAR STRUCTURE 24Mg; calculated levels, yrast sequence, single particle Routhians, hexadecapole moment expectation value vs angular momentum. Self-consistent cranked Hartree-Fock plus BCS equations.
doi: 10.1016/0375-9474(87)90331-9
1987CO18 Phys.Lett. 192B, 263 (1987) A.Coc, P.Bonche, H.Flocard, P.H.Heenen Deformation of 121Cs and of Its Neighbours Calculated in the Mean Field Approximation NUCLEAR STRUCTURE 121,123Cs, 122,124Ba; calculated nucleon separation energies. 120Xe, 120,122,124,128Ba; calculated deformations. 120Xe, 128Ba, 121,123Cs; calculated triaxial deformation energy surfaces. 121,123Cs; calculated moments. Self-consistent mean field approximation.
doi: 10.1016/0370-2693(87)90102-X
1986BO19 Phys.Lett. 175B, 387 (1986) P.Bonche, P.H.Heenen, H.Flocard, D.Vautherin Self-Consistent Calculation of the Quadrupole-Octupole Deformation Energy Surface of 222Ra NUCLEAR STRUCTURE 222Ra; calculated quadrupole-octupole deformation energy surface; deduced nonzero octupole moment. Self-consistent Hartree-Fock plus BCS calculations.
doi: 10.1016/0370-2693(86)90609-X
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
1985BO36 Nucl.Phys. A443, 39 (1985) P.Bonche, H.Flocard, P.H.Heenen, S.J.Krieger, M.S.Weiss Self-Consistent Study of Triaxial Deformations: Application to the isotopes of Kr, Sr, Zr and Mo NUCLEAR STRUCTURE 80,102Zr; calculated quasiparticle energies, deformation energy curves, proton, neutron rms radii, deformation, quadrupole moments, binding energies. 86,88,90,92,94,96,98,100,102,104Zr, 90,92,96,98,104Mo, 88,90,94,102,100Sr, 98,100Kr; calculated deformation energy surfaces. 90Kr; calculated deformation energy surfaces, binding energy. 84,82,80,78,76Zr, 80,78,76,74Sr, 76,74Kr; calculated deformation energy surfaces.
doi: 10.1016/0375-9474(85)90320-3
1984AU14 Phys.Lett. 149B, 6 (1984) D.Auverlot, P.Bonche, P.Bonche, H.Flocard, P.H.Heenen On the Deformation Energy Surface of 16O NUCLEAR STRUCTURE 16O; calculated levels, quadrupole moment, deformation energy surface. Constrained Hartree-Fock, Skyrme force.
doi: 10.1016/0370-2693(84)91539-9
1984BA65 Nucl.Phys. A428, 79c (1984) R.Balian, P.Bonche, H.Flocard, M.Veneroni Mass Dispersions in a Time-Dependent Mean-Field Approach NUCLEAR REACTIONS 16O(16O, X), E(cm)=80 MeV; calculated mass dispersion. Time-dependent mean field approach.
doi: 10.1016/0375-9474(84)90243-4
1984DO09 Nucl.Phys. A422, 103 (1984) J.Dobaczewski, H.Flocard, J.Treiner Hartree-Fock-Bogolyubov Description of Nuclei near the Neutron-Drip Line NUCLEAR STRUCTURE A=100-176; calculated Sn isotope binding energies. HFB near neutron drip line.
doi: 10.1016/0375-9474(84)90433-0
1984FL04 Prog.Theor.Phys.(Kyoto) 72, 1000 (1984) H.Flocard, P.H.Heenen, S.J.Krieger, M.S.Weiss Configuration Space, Cranked Hartree-Fock Calculations for the Nuclei 16O, 24Mg and 32S NUCLEAR STRUCTURE 16O, 32S, 24Mg; calculated levels, band structure, fission modes. Cranked Hartree-Fock method.
doi: 10.1143/PTP.72.1000
1984MA11 Phys.Lett. 134B, 287 (1984) S.Marcos, H.Flocard, P.-H.Heenen Calculation of the Peierls-Yoccoz Translational Mass for Hartree-Fock Wave Functions NUCLEAR STRUCTURE 4He, 16O; calculated Hartree-Fock energy, Peierls-Yocoz mass parameters; deduced galilean invariance breaking evidence.
doi: 10.1016/0370-2693(84)90001-7
1983HE02 Nucl.Phys. A394, 525 (1983) P.H.Heenen, H.Flocard, D.Vautherin Adiabatic Time-Dependent Hartree-Fock Calculation of Fusion Cross Sections: Application to 40Ca - 40Ca NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E(cm)=55-100 MeV; calculated σ(fusion) vs E. Adiabatic TDHF.
doi: 10.1016/0375-9474(83)90121-5
1983MA68 Nucl.Phys. A410, 125 (1983) S.Marcos, H.Flocard, P.H.Heenen Influence of Left-Right Asymmetry Degrees of Freedom in Self-Consistent Calculations of 20Ne NUCLEAR STRUCTURE 20Ne; calculated binding energy, charge radius, charge quadrupole moment; deduced left-right asymmetry, cluster channel degrees of freedom. Self-consistent calculation, α-16O clustering.
doi: 10.1016/0375-9474(83)90405-0
1982FL04 Nucl.Phys. A391, 285 (1982) H.Flocard, P.H.Heenen, S.J.Krieger, M.S.Weiss From Ground State to Scission: The spinning life of 20Ne NUCLEAR STRUCTURE 20Ne; calculated level energy, moment of inertia, quadrupole moment, asymmetry vs L. Cranked Hartree-Fock method.
doi: 10.1016/0375-9474(82)90611-X
1981FL03 Phys.Lett. 105B, 14 (1981) Generation of High-Frequency Components in TDHF Heavy-Ion collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=400 MeV; calculated integrated fragment density, time evolution of fragment rms radius. TDHF.
doi: 10.1016/0370-2693(81)90029-0
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
1980FL02 Nucl.Phys. A339, 336 (1980) H.Flocard, P.H.Heenen, D.Vautherin A Microscopic Calculation of Potentials and Inertia Parameters for Heavy-Ion Collisions NUCLEAR REACTIONS 12C(12C, X), 16O(16O, X), E not given; calculated HI collision potentials, inertia parameters; deduced quasimolecular resonance mechanism. Adiabatic time-dependent Hartree-Fock.
doi: 10.1016/0375-9474(80)90098-6
1979BL03 Phys.Lett. 85B, 163 (1979) Calculation of Giant Resonances with Time-Dependent Hartree-Fock NUCLEAR STRUCTURE 16O, 40Ca; calculated energies of lowest multipole resonances. Time dependent Hartree-Fock, Skyrme interaction.
doi: 10.1016/0370-2693(79)90568-9
1979BO18 Phys.Rev. C20, 641 (1979) P.Bonche, K.T.R.Davies, B.Flanders, H.Flocard, B.Grammaticos, S.E.Koonin, S.J.Krieger, M.S.Weiss Time-Dependent Hartee-Fock Calculations of Fusion Cross Sections for 16O + 40Ca and 28Si + 28Si NUCLEAR REACTIONS 16O(40Ca, X), E(cm)=30-250 MeV; 28Si(28Si, X), E(cm)=35-250 MeV; calculated fusion σ; deduced angular momentum fusion window. Time-dependent Hartree-Fock, Skyrme interaction.
doi: 10.1103/PhysRevC.20.641
1979CU03 Nucl.Phys. A331, 213 (1979) A Microscopic Description of Nuclear Molecules: Application to the 12C + 12C System NUCLEAR REACTIONS 12C(12C, 12C), 12C(12C, 12C'), E(cm)=10-30 MeV; calculated σ(E, θ). Coupled channels approach, oblate 12C ion interaction from Hartree-fork method.
doi: 10.1016/0375-9474(79)90310-5
1978DA18 Phys.Rev. C18, 2631 (1978) K.T.R.Davies, H.T.Feldmeier, H.Flocard, M.S.Weiss Comparison of Two- and Three-Dimensional Time-Dependent Hartree-Fock Calculations of the Reactions 16O + 16O and 40Ca + 40Ca NUCLEAR REACTIONS 16O(16O, X), E=105 MeV; 40Ca(40Ca, X), E=192 MeV; calculated energy loss, deflection function in 2-, 3-dimensional time-dependent Hartree-Fock.
doi: 10.1103/PhysRevC.18.2631
1978FL04 Phys.Rev. C17, 1682 (1978) H.Flocard, S.E.Koonin, M.S.Weiss Three-Dimensional Time-Dependent Hartree-Fock Calculations: Application to 16O + 16O Collisions NUCLEAR REACTIONS 16O(16O, X), E=105 MeV; calculated fusion, strongly damped collisions. 3-D tdhf approximation.
doi: 10.1103/PhysRevC.17.1682
1978FL06 Phys.Rev. C18, 573 (1978) Comparison of Two-Dimensional and Three-Dimensional Time-Dependent Hartree-Fock for 40Ca + 40Ca at E(lab) = 278 MeV NUCLEAR REACTIONS 40Ca(40Ca, X), E=2.78 MeV; calculated 2-, 3-dimensional time-dependent Hartree-Fock interactions.
doi: 10.1103/PhysRevC.18.573
1978KO22 Phys.Lett. 77B, 13 (1978) S.Koonin, B.Flanders, H.Flocard, M.Weiss A Separable Approximation to Time-Dependent Hartree-Fock Calculations NUCLEAR REACTIONS 16O(16O, 16O), 40Ca(40Ca, 40Ca); calculated reaction parameters.
doi: 10.1016/0370-2693(78)90188-0
1977ST13 Phys.Lett. 68B, 108 (1977) F.Stancu, D.M.Brink, H.Flocard The Tensor Part of Skyrme's Interaction NUCLEAR STRUCTURE 48Ca, 56Ni; calculated p, n levels.
doi: 10.1016/0370-2693(77)90178-2
1976FL09 Nucl.Phys. A264, 197 (1976) Generator Coordinate Calculations of Giant Resonances with the Skyrme Interaction NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated wave functions.
doi: 10.1016/0375-9474(76)90428-0
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
1975CA27 Nucl.Phys. A251, 193 (1975) X.Campi, H.Flocard, A.K.Kerman, S.Koonin Shape Transition in the Neutron Rich Sodium Isotopes NUCLEAR STRUCTURE 19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35Na; calculated single particle energies, quadrupole moments, β.
doi: 10.1016/0375-9474(75)90065-2
1975FL02 Phys.Lett. 55B, 259 (1975) Generator Coordinate Calculations of Monopole and Quadrupole Vibrations with Skyrme's Interaction NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated monopole, quadrupole modes.
doi: 10.1016/0370-2693(75)90594-8
1974FL10 Nucl.Phys. A231, 176 (1974) H.Flocard, P.Quentin, D.Vautherin, M.Veneroni, A.K.Kerman Self-Consistent Calculation of the Fission Barrier of 240Pu NUCLEAR STRUCTURE 240Pu; calculated deformation energy curve, levels.
doi: 10.1016/0375-9474(74)90300-5
1973CA23 Phys.Lett. 46B, 11 (1973) M.Cailliau, J.Letessier, H.Flocard, P.Quentin Self Consistent Calculations of a Possible Shape Transition in Neutron Deficient Mercury Isotopes NUCLEAR STRUCTURE 180,184,186,188,190,200Hg; calculated deformation energy curves.
doi: 10.1016/0370-2693(73)90461-9
1973FL02 Nucl.Phys. A203, 433 (1973) H.Flocard, P.Quentin, A.K.Kerman, D.Vautherin Nuclear Deformation Energy Curves with the Constrained Hartree-Fock Method NUCLEAR STRUCTURE 40Ca, 126,134,140,150Ce, 208Pb; calculated deformation energy curves with constrained Hartree-Fock technique.
doi: 10.1016/0375-9474(73)90357-6
1973FL05 Phys.Lett. 46B, 304 (1973) H.Flocard, P.Quentin, D.Vautherin Self-Consistent Calculation of the Ground State Properties of Some Rare-Earth Nuclei NUCLEAR STRUCTURE 152Sm, 158Gd, 162Dy, 166Er, 174Yb, 178Hf, 184W, 190Os; level calculated deformation properties.
doi: 10.1016/0370-2693(73)90125-1
1972SI14 Phys.Lett. 39B, 443 (1972) The Charge Distribution Difference between Lead and Bismuth
doi: 10.1016/0370-2693(72)90313-9
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