NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = S.Fracasso Found 8 matches. 2016ST13 Phys.Rev. C 93, 054617 (2016) P.D.Stevenson, E.B.Suckling, S.Fracasso, M.C.Barton, A.S.Umar Skyrme tensor force in heavy ion collisions NUCLEAR REACTIONS 16O(16O, X), E(cm)=100 MeV; calculated contributions from terms involving time-odd densities and currents to the total energy as the sum of isoscalar and isovector contributions, energy contributions from (pseudo)scalar-, vector- and (pseudo)tensor-decomposed form of spin-current tensor J. Symmetry-unrestricted Time-dependent Hartree-Fock (TDHF) energy density functional calculations with full version of Skyrme force, including terms arising only from the Skyrme tensor force. Discussed role of Skyrme tensor force in dynamic processes in nuclei.
doi: 10.1103/PhysRevC.93.054617
2012FR06 Phys.Rev. C 86, 044303 (2012) S.Fracasso, E.B.Suckling, P.D.Stevenson Unrestricted Skyrme-tensor time-dependent Hartree-Fock model and its application to the nuclear response from spherical to triaxial nuclei NUCLEAR STRUCTURE 16O, 24Mg, 28Si, 120Sn, 178Os, 190W, 238U; calculated transition strength distributions of isovector giant dipole resonances using the Skyrme energy density functional (EDF) in the three dimensional time-dependent Hartree-Fock. Comparison with predictions from the (quasi)-particle random-phase approximation and experimental data.
doi: 10.1103/PhysRevC.86.044303
2012ST23 J.Phys.:Conf.Ser. 381, 012105 (2012) P.D.Stevenson, S.Fracasso, E.B.Suckling The tensor-kinetic field in nuclear collisions
doi: 10.1088/1742-6596/381/1/012105
2007CO06 Phys.Lett. B 646, 227 (2007) G.Colo, H.Sagawa, S.Fracasso, P.F.Bortignon Spin-orbit splitting and the tensor component of the Skyrme interaction NUCLEAR STRUCTURE 106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er; calculated single-particle energy differences. Skyrme effective interaction with tensor term. Comparison with data.
doi: 10.1016/j.physletb.2007.01.033
2007CO24 Nucl.Phys. A788, 173c (2007) G.Colo, P.F.Bortignon, S.Fracasso, N.Van Giai What can we learn from recent non-relativistic mean field calculations? NUCLEAR STRUCTURE 120,132Sn, 208Pb; calculated low-lying states level energy, B(E2), GDR. Fully self-consistent quasi-particle RPA model, comparisons with Gogny forces, relativistic mean field Lagrangians and data.
doi: 10.1016/j.nuclphysa.2007.01.079
2007FR15 Phys.Atomic Nuclei 70, 1415 (2007) Microscopic calculations of charge-exchange nuclear modes NUCLEAR STRUCTURE 90Zr, 114,118,120,124Sn, 208Pb; calculated IAS and GTR energies and GT strength distributions using nonrelativistic spherical QRPA and HF-BCS approach.
doi: 10.1134/S1063778807080157
2007FR20 Phys.Rev. C 76, 044307 (2007) Spin-isospin nuclear response using the existing microscopic Skyrme functionals NUCLEAR STRUCTURE 90Zr, 208Pb, 114,118,120,124Sn; calculated excitation energies, Gamow-Teller strengths. Used non-relativistic Skyrme energy functionals, QRPA.
doi: 10.1103/PhysRevC.76.044307
2005FR35 Phys.Rev. C 72, 064310 (2005) Fully self-consistent charge-exchange quasiparticle random-phase approximation and its application to isobaric analog resonances NUCLEAR STRUCTURE 104,106,108,110,112,114,116,118,120,122,124,126,128,130,132Sn; calculated pair gap energies, IAR energies. 120In; calculated giant monopole resonance strength function. Fully self-consistent charge-exchange quasiparticle RPA.
doi: 10.1103/PhysRevC.72.064310
Back to query form |