NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = F.Tondeur Found 33 matches. 2002GO26 Phys.Rev. C66, 024326 (2002) S.Goriely, M.Samyn, P.H.Heenen, J.M.Pearson, F.Tondeur Hartree-Fock mass formulas and extrapolation to new mass data NUCLEAR STRUCTURE Z=8-120; analyzed masses, mass formulas; deduced parameters. ATOMIC MASSES Z=8-120; analyzed masses, mass formulas; deduced parameters.
doi: 10.1103/PhysRevC.66.024326
2002SA14 Nucl.Phys. A700, 142 (2002) M.Samyn, S.Goriely, P.-H.Heenen, J.M.Pearson, F.Tondeur A Hartree-Fock-Bogoliubov Mass Formula NUCLEAR STRUCTURE Z=8-120; calculated masses, binding energies. Hartree-Fock-Bogoliubov method.
doi: 10.1016/S0375-9474(01)01316-1
2001FA22 Nucl.Phys. A696, 396 (2001) M.Farine, J.M.Pearson, F.Tondeur Skyrme Force with Surface-Peaked Effective Mass NUCLEAR STRUCTURE 84Ni, 122Zr, 190Gd, 266Pb, 276U; calculated mass, neutron separation energy, Qβ. 16O, 90Zr, 208Pb; calculated single-particle levels. Skyrme force with effective mass.
doi: 10.1016/S0375-9474(01)01136-8
2001GO20 At.Data Nucl.Data Tables 77, 311 (2001) S.Goriely, F.Tondeur, J.M.Pearson A Hartree-Fock Nuclear Mass Table ATOMIC MASSES Z=8-120; calculated masses, deformation parameters. Hartree-Fock-BCS approach, Skyrme force, pairing force, Wigner term. NUCLEAR STRUCTURE Z=8-120; calculated masses, deformation parameters. Hartree-Fock-BCS approach, Skyrme force, pairing force, Wigner term.
doi: 10.1006/adnd.2000.0857
2001GO30 Nucl.Phys. A688, 349c (2001) S.Goriely, M.Pearson, F.Tondeur At Last a Hartree-Fock + BCS Mass Table NUCLEAR STRUCTURE Z=8-120; calculated mass, deformation parameters, neutron and proton separation energies. Comparison with data.
doi: 10.1016/S0375-9474(01)00725-4
2001MA04 Nucl.Phys. A679, 337 (2001) A.Mamdouh, J.M.Pearson, M.Rayet, F.Tondeur Fission Barriers of Neutron-Rich and Superheavy Nuclei Calculated with the ETFSI Method NUCLEAR STRUCTURE Z=84-120; A=214-318; calculated fission barrier heights. Extended Thomas-Fermi plus Strutinsky integral method.
doi: 10.1016/S0375-9474(00)00358-4
2000DU06 Phys.Rev. C61, 054303 (2000) A.K.Dutta, J.M.Pearson, F.Tondeur Triaxial Nuclei Calculated with the Extended Thomas-Fermi plus Strutinsky Integral (ETFSI) Method NUCLEAR STRUCTURE 62Zn, 74Ge, 110,111,112,113,114,115,116,117,118Zr, 132Ba, 134Ce, 138Sm, 168Er, 186W, 188,192Os, 222Ra, 233Th, 236,262U, 271Np, 240Pu, 244Cm, 287Bk, 252Cf, 255,286Fm, 259,292Rf, 294Hs, 288,294Cn, 298Fl; calculated ground state energy shift due to triaxial deformation. 233Th, 236,262U, 240Pu, 244Cm, 287Bk, 252Cf, 255,286Fm, 292Rf, 294Hs, 288,294Cn, 298Fl; calculated fission barrier energy shift due to triaxial deformation. Extended Thomas-Fermi plus Strutinsky integral method.
doi: 10.1103/PhysRevC.61.054303
2000TO06 Phys.Rev. C62, 024308 (2000) F.Tondeur, S.Goriely, J.M.Pearson, M.Onsi Towards a Hartree-Fock Mass Formula
doi: 10.1103/PhysRevC.62.024308
1999PE22 Acta Phys.Hung.N.S. 10, 159 (1999) J.M.Pearson, F.Tondeur, A.Mamdouh, M.Rayet Nuclear Masses and Fission Barriers via the ETFSI Method NUCLEAR STRUCTURE Z=92; calculated fission barriers for N ≈ 140-190. ETFSI method, Skyrme force.
1998MA86 Nucl.Phys. A644, 389 (1998); Erratum Nucl.Phys. A648, 282 (1999) A.Mamdouh, J.M.Pearson, M.Rayet, F.Tondeur Large-Scale Fission-Barrier Calculations with the ETFSI Method NUCLEAR STRUCTURE Z=80-100; calculated fission barrier heights. Extended Thomas-Fermi plus Strutinsky Integral method. Astrophysical implications discussed.
doi: 10.1016/S0375-9474(98)00576-4
1997FA06 Nucl.Phys. A615, 135 (1997) M.Farine, J.M.Pearson, F.Tondeur Nuclear-Matter Incompressibility from Fits of Generalized Skyrme Force to Breathing-Mode Energies NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 112,114,116,120,124,132Sn, 144Sm, 208Pb; calculated internal energy, rms charge radius. Breathing modes, generalized Skyrme forces.
doi: 10.1016/S0375-9474(96)00453-8
1995AB38 At.Data Nucl.Data Tables 61, 127 (1995) Y.Aboussir, J.M.Pearson, A.K.Dutta, F.Tondeur Nuclear Mass Formula via an Approximation to the Hartree-Fock Method NUCLEAR STRUCTURE A=36-300; calculated masses, n-, p-separation, β-decay energies. Extended Thomas-Fermi, plus Strutinsky integral method.
doi: 10.1016/S0092-640X(95)90014-4
1994BU06 Phys.Rev. C49, 1402 (1994) F.Buchinger, J.E.Crawford, A.K.Dutta, J.M.Pearson, F.Tondeur Nuclear Charge Radii in Modern Mass Formulas NUCLEAR STRUCTURE 78,80,82,84,86,88,90,92,94,96,98,100Sr; calculated β2 deformation parameter. A=36-238; calculated absolute rms charge radii. Extended Thomas-Fermi, finite-range droplet models mass formula.
doi: 10.1103/PhysRevC.49.1402
1992AB08 Nucl.Phys. A549, 155 (1992) Y.Aboussir, J.M.Pearson, A.K.Dutta, F.Tondeur Thomas-Fermi Approach to Nuclear-Mass Formula (IV). The ETFSI-1 Mass Formula NUCLEAR STRUCTURE A=36-300; analyzed mass data; calculated equilibrium deformations, fission barriers; deduced Skyrme, δ-function pairing forces parameters. Hartree-Fock, BCS method, semi-classical approximations.
doi: 10.1016/0375-9474(92)90038-L
1991PE03 Nucl.Phys. A528, 1 (1991) J.M.Pearson, Y.Aboussir, A.K.Dutta, R.C.Nayak, M.Farine, F.Tondeur Thomas-Fermi Approach to Nuclear Mass Formula (III). Force Fitting and Construction of Mass Table NUCLEAR STRUCTURE A=100-260; calculated energies, equilibrium deformation parameters. 186Os, 210Po, 240Pu, 250Cm, 262U; calculated fission barriers. Thomas-Fermi approach to mass formula.
doi: 10.1016/0375-9474(91)90418-6
1988BE08 Z.Phys. A329, 393 (1988) D.Berdichevsky, R.Fleming, D.W.L.Sprung, F.Tondeur Charge and Mass Radii of the Tin Isotopes NUCLEAR STRUCTURE 108,110,112,114,116,118,120,122,124Sn; analyzed isotope shifts, rms radii; deduced proton rms radius average variation rate. Hartree-Fock, droplet models.
1987TO13 Nucl.Phys. A470, 93 (1987) F.Tondeur, A.K.Dutta, J.M.Pearson, R.Behrman Thomas-Fermi Approach to Nuclear Mass Formula (II). Deformed Nuclei and Fission Barriers NUCLEAR STRUCTURE 162Dy, 174Yb, 184W, 232Th, 240Pu, 252Cf, 262U; calculated deformed ground states, fission barriers, isomers. Skyrme-extended Thomas-Fermi method.
doi: 10.1016/0375-9474(87)90122-9
1986DU12 Nucl.Phys. A458, 77 (1986) A.K.Dutta, J.-P.Arcoragi, J.M.Pearson, R.Behrman, F.Tondeur Thomas-Fermi Approach to Nuclear Mass Formula. (I). Spherical Nuclei NUCLEAR STRUCTURE Z=8-88, A=16-222; calculated masses, neutron separation, β-decay energies. Extended Thomas-Fermi method, shell effects.
doi: 10.1016/0375-9474(86)90283-6
1986TO01 J.Phys.(London) G12, 33 (1986) Hartree-Fock Against Droplet Model of Nuclear Core Densities: A revised verdict NUCLEAR STRUCTURE 16O, 40Ca, 60Ni, 80Kr, 90Zr, 120Te, 140Nd, 200Hg; calculated bulk densities. 16O, 28Si, 40,48Ca, 56Fe, 58Ni, 90Zr, 118,132Sn, 138Ba, 146Gd, 208Pb; calculated bulk densities, dilation parameters.
doi: 10.1088/0305-4616/12/1/011
1986TO16 Z.Phys. A325, 405 (1986) F.Tondeur, D.Berdichevsky, M.Farine Nuclear Matter Saturation Density: From finite nuclei to infinite matter NUCLEAR STRUCTURE 16O, 40Ca, 58Ni, 208Pb; calculated average core charge densities, matter density, charge radii. Skyrme functional, Hartree-Fock calculations.
1985BE35 Z.Phys. A322, 141 (1985) Nuclear Core Densities, Isotope Shifts, and the Parametrization of the Droplet Model NUCLEAR STRUCTURE 58Ni, 90Zr; calculated charge distribution, rms charge radius. 208Pb; calculated rms charge radius, charge, matter distributions. A=40-80, 100-220; calculated bulk charge densities. 124Sn; calculated charge distribution. 138Ba, 116Sn; calculated rms charge radii. Z=28, 50, 82, 126; calculated isotope shifts; deduced core density parameters. Droplet model.
doi: 10.1007/BF01412027
1985TO16 Nucl.Phys. A442, 460 (1985) Fission Barriers and the Parametrisation of Skyrme Forces NUCLEAR STRUCTURE 240Pu; calculated fission barrier effective interaction parameter dependence. Hartree-Fock plus BCS, Skyrme forces.
doi: 10.1016/S0375-9474(85)80026-9
1984TO05 Nucl.Phys. A420, 297 (1984) F.Tondeur, M.Brack, M.Farine, J.M.Pearson Static Nuclear Properties and the Parametrisation of Skyrme Forces NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; calculated binding energies, rms radii. 32S, 56Fe, 72Ge, 100Ru, 110Cd, 118,132Sn, 138Ba, 146Gd; calculated binding energies. 240Pu; calculated fission barriers. Trial Skyrme forces.
doi: 10.1016/0375-9474(84)90444-5
1983TO02 Nucl.Phys. A394, 462 (1983) F.Tondeur, J.M.Pearson, M.Farine The Anomalies of the Droplet Model NUCLEAR STRUCTURE A ≈ 10-260; calculated surface stiffness vs mass. Droplet model.
doi: 10.1016/0375-9474(83)90118-5
1983TO04 Phys.Lett. 123B, 139 (1983) A Skyrme Functional for Hartree-Fock Calculations of Nuclear Masses and Density Distributions NUCLEAR STRUCTURE 16O, 48Ca, 56Fe, 118,132Sn, 138Ba, 146Gd; calculated binding energies, charge radii. 40Ca, 58Ni, 90Zr, 208Pb; calculated binding energies, charge radii, charge distributions.
doi: 10.1016/0370-2693(83)90408-2
1982TO07 Nucl.Phys. A383, 32 (1982) Average Trends of Nuclear Densities from a Self-Consitent Model with a Generalised Strutinsky-Type Smoothing NUCLEAR STRUCTURE A=16-300; calculated mass, neutron, proton core densities, droplet, liquid drop model radii vs mass. Self-consistent model, generalized Strutinsky smoothing.
doi: 10.1016/0375-9474(82)90075-6
1981TO07 Nucl.Phys. A359, 278 (1981) The Subshell Closure at N=56 and the Deformation of Neutron-Rich Isotopes from Ge to Zr NUCLEAR STRUCTURE 90,96Zr, 91Br; calculated neutron single particle levels; 88,90,92,94,96,98,100Zr; calculated pairing energy; 92,94,96,98Zr; calculated two-neutron separation energies; 100Zr; calculated deformation energy; deduced N=56 subshell closure. Microscopic energy density method.
doi: 10.1016/0375-9474(81)90237-2
1980TO01 Nucl.Phys. A338, 77 (1980) Self-Consistent Study of the Proton Shell Effects Near 146Gd NUCLEAR STRUCTURE 146,150,152Gd; calculated levels, deformation energy curves, α-decay energy differences; deduced subshell effect at Z=64. Self-consistent energy density mass formula.
doi: 10.1016/0375-9474(80)90122-0
1980TO09 Z.Phys. A297, 61 (1980) Shell Structure and Stability of Nuclei with 270 < A < 500 and the Possible Existence of Primordial Superheavy Nuclei NUCLEAR STRUCTURE A=270-500; calculated Eα, α-decay T1/2, nuclear densities, single particle potentials. Self-consistent energy density method. Superheavy nuclei.
doi: 10.1007/BF01414246
1979TO02 Nucl.Phys. A315, 353 (1979) Pairing with a Delta Interaction in the Energy Density Nuclear Mass Formula NUCLEAR STRUCTURE 56Fe, 108Pd, 150Sm, 196Pt; calculated variations of average pairing strength in (N, Z) plane δ-interaction, self-consistent energy density formalism. Extrapolation to deformed, superheavy nuclei.
doi: 10.1016/0375-9474(79)90616-X
1978TO06 Nucl.Phys. A303, 185 (1978) An Energy Density Nuclear Mass Formula. I. Self-Consistent Calculation for Spherical Nuclei NUCLEAR STRUCTURE 208Pb; calculated levels. 16O, 24,26Mg, 28Si, 32S, 40Ar, 40,48Ca, 48Ti, 52Cr, 54,56,58Fe, 58,60,62,64Ni, 64,66,68,70Zn, 88Sr, 90,92,94,96Zr, 92,94,96,98,100Mo, 110,112,114,116Cd, 112,114,116,118,120,122,124Sn, 138Ba, 142,144,146,148Nd, 148Sm, 206,208Pb; calculated nuclear charge radii.
doi: 10.1016/0375-9474(78)90050-7
1978TO10 Nucl.Phys. A311, 51 (1978) An Energy Density Nuclear Mass Formula (II). Approximate Method for Deformed Nuclei NUCLEAR STRUCTURE Z=54-96; calculated binding energies, quadrupole moments. Strutinsky prescription with modified smoothing method for energy density mass formula.
doi: 10.1016/0375-9474(78)90501-8
1972TO20 J.Phys.(Paris) 33, 825 (1972) Extension de la Prescription de Strutinski a des Puits de Potentiel Finis
doi: 10.1051/jphys:019720033010082500
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