NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = M.Samyn Found 19 matches. 2007GO18 Phys.Rev. C 75, 064312 (2007) S.Goriely, M.Samyn, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. VII. Simultaneous fits to masses and fission barriers NUCLEAR STRUCTURE Z > 7, N > 7; analyzed masses and fission barrier data using a new HFB mass model.
doi: 10.1103/PhysRevC.75.064312
2006GO21 Nucl.Phys. A773, 279 (2006) S.Goriely, M.Samyn, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas VI: Weakened pairing NUCLEAR STRUCTURE Z=8-120; A=16-360; analysed atomic masses. Nuclear matter properties discussed. Skyrme-Hartree-Fock-Bogoliubov approach, comparison with data and earlier models.
doi: 10.1016/j.nuclphysa.2006.05.002
2005DE44 Nucl.Phys. A758, 627c (2005) P.Demetriou, M.Samyn, S.Goriely Fission properties relevant to r-process nucleosynthesis NUCLEAR REACTIONS 231Pa, 233,234,238U, 239Pu, 248Cm(n, F), E(cm)=0-5 MeV; calculated fission σ. Comparison with data. RADIOACTIVITY 232,234,236,238,240U, 238,240,242,244,246Pu, 242,244,246,248,250Cm, 250,252Cf(SF); calculated fission T1/2.
doi: 10.1016/j.nuclphysa.2005.05.113
2005GO07 Nucl.Phys. A750, 425 (2005) S.Goriely, M.Samyn, J.M.Pearson, M.Onsi Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. IV: Neutron-matter constraint
doi: 10.1016/j.nuclphysa.2005.01.009
2005GO32 Nucl.Phys. A758, 587c (2005) S.Goriely, P.Demetriou, H.-Th.Janka, J.M.Pearson, M.Samyn The r-process nucleosynthesis: a continued challenge for nuclear physics and astrophysics
doi: 10.1016/j.nuclphysa.2005.05.107
2005GO39 Eur.Phys.J. A 25, Supplement 1, 71 (2005) S.Goriely, M.Samyn, J.M.Pearson, E.Khan Recent progress in mass predictions NUCLEAR STRUCTURE Z=8-120; A=16-340; analyzed atomic masses. Nuclear matter properties discussed. Skyrme-Hartree-Fock-Bogoliubov approach, comparison with data.
doi: 10.1140/epjad/i2005-06-022-4
2005PE17 Nucl.Phys. A758, 651c (2005) J.M.Pearson, M.Onsi, S.Goriely, M.Samyn Hartree-Fock-Bogoliubov mass formulas and the equation of state of neutron-star matter
doi: 10.1016/j.nuclphysa.2005.05.117
2005SA48 Nucl.Phys. A758, 659c (2005) Microscopic HFB Fission Barriers for r-Process Nucleosynthesis Calculations NUCLEAR STRUCTURE 240Pu; calculated potential energy surface. Z=84-100; calculated fission barrier heights. Constrained Skyrme-Hartree-Fock-Bogoliubov approach.
doi: 10.1016/j.nuclphysa.2005.05.118
2005SA56 Phys.Rev. C 72, 044316 (2005) M.Samyn, S.Goriely, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. V. Extension to fission barriers NUCLEAR STRUCTURE Z=80-130; A=198-314; calculated deformation and fission barrier parameters. Skyrme-Hartree-Fock-Bogoliubov approach, comparisons with data.
doi: 10.1103/PhysRevC.72.044316
2005WA27 Nucl.Phys. A758, 671c (2005) S.Wanajo, N.Itoh, S.Goriely, M.Samyn, Y.Ishimaru The r-process in supernovae with new microscopic mass formulae
doi: 10.1016/j.nuclphysa.2005.05.120
2004GO37 Nucl.Phys. A739, 331 (2004) Microscopic HFB + QRPA predictions of dipole strength for astrophysics applications NUCLEAR STRUCTURE 72Ge, 82Se, 94Zr, 100Mo, 124Sn, 130Te, 142Ce, 150Sm, 208Pb; calculated photoabsorption σ, dipole strength distributions. Z=8-110; calculated Maxwellian-average neutron capture rates. HFB and quasiparticle RPA models, comparison with data.
doi: 10.1016/j.nuclphysa.2004.04.105
2004SA55 Phys.Rev. C 70, 044309 (2004) M.Samyn, S.Goriely, M.Bender, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. III. Role of particle-number projection NUCLEAR STRUCTURE Z=8-120; calculated masses. 230,231,233Th, 235,236,237,238,239U, 237,238Np, 235,237,238,239,240,241,243,244Pu, 239,240,241,242,243,244Am, 241,242,243,244,245Cm, 244Bk; analyzed shape isomer energies. 32S, 208Pb; calculated charge density distributions. Skyrme-Hartree-Fock-Bogoliubov mass formulas.
doi: 10.1103/PhysRevC.70.044309
2003GO31 Phys.Rev. C 68, 054325 (2003) S.Goriely, M.Samyn, M.Bender, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. II. Role of the effective mass NUCLEAR STRUCTURE Z=8-120; calculated masses; deduced role of effective mass. 16O, 132Sn, 208Pb; calculated single-particle energy levels. Skyrme-Hartree-Fock-Bogoliubov approach, comparisons with data.
doi: 10.1103/PhysRevC.68.054325
2003SA26 Nucl.Phys. A725, 69 (2003) M.Samyn, S.Goriely, J.M.Pearson Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas I: Role of density dependence in pairing force
doi: 10.1016/S0375-9474(03)01578-1
2003SA34 Nucl.Phys. A718, 653c (2003) M.Samyn, S.Goriely, J.M.Pearson Nuclear Mass Predictions Within The Skyrme HFB Theory NUCLEAR STRUCTURE A=2-270; calculated masses. Z=34-70; calculated shell gaps. Self-consistent Skyrme HFB approach.
doi: 10.1016/S0375-9474(03)00877-7
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
2002PE19 Eur.Phys.J. A 15, 13 (2002) J.M.Pearson, S.Goriely, M.Samyn A Hartree-Fock nuclear mass formula
doi: 10.1140/epja/i2001-10215-y
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
2001SA75 Hyperfine Interactions 132, 433 (2001) M.Samyn, S.Goriely, P.-H.Heenen Towards a Skyrme-Hartree-Fock-Bogolyubov Mass Formula NUCLEAR STRUCTURE 116Se, 118Kr, 120Sr, 122Zr, 124Mo, 126Ru, 128Pd, 130Cd, 132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy; calculated two-neutron separation energies. Skyrme-Hartree-Fock-Bogolyubov formula.
doi: 10.1023/A:1011960316655
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