NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = F.Stancu Found 39 matches. 2018BR11 Phys.Rev. C 97, 064304 (2018) Skyrme density functional description of the double magic 78Ni nucleus NUCLEAR STRUCTURE 68,69,70,71,72,73,74,75,76,77,78Ni; calculated proton single-particle energy difference between the unoccupied 1f5/2 and occupied 1f7/2 levels, proton and neutron single particle energies around the Fermi sea with and without tensor force by Hartree-Fock calculations using the Skryme energy density functional; deduced contribution of tensor force to single-particle spectra gap, and doubly-magic character of 78Ni.
doi: 10.1103/PhysRevC.97.064304
2016ST01 Nucl.Phys. A945, 144 (2016) SU(3) Clebsch-Gordan coefficients at large Nc
doi: 10.1016/j.nuclphysa.2015.10.003
2009MA45 Nucl.Phys. A826, 161 (2009) Matrix elements of SU(6) generators for baryons with arbitrary Nc quarks in mixed symmetric states [Nc-1, 1]
doi: 10.1016/j.nuclphysa.2009.05.092
2008MA38 Nucl.Phys. A811, 291 (2008) A new look at the [70, 1-] baryon multiplet in the 1/Nc expansion
doi: 10.1016/j.nuclphysa.2008.07.006
2007BR12 Phys.Rev. C 75, 064311 (2007) Evolution of nuclear shells with the Skyrme density dependent interaction NUCLEAR STRUCTURE Z=20, Z=50, N=82; calculated proton and neutron single particle energies using Hartree-Fock method and density dependent Skyrme interaction.
doi: 10.1103/PhysRevC.75.064311
2003PA29 Nucl.Phys. A726, 327 (2003) Three-body confinement force in a realistic constituent quark model
doi: 10.1016/j.nuclphysa.2003.07.011
2003SA16 Phys.Rev. C 67, 054005 (2003) Phase shift effective range expansion from supersymmetric quantum mechanics NUCLEAR REACTIONS 1H(n, n), E=14-350 MeV; calculated phase shifts, potential features. Supersymmetric transformations, phase shift effective range expansion.
doi: 10.1103/PhysRevC.67.054005
2002BA22 Nucl.Phys. A699, 316c (2002) Nucleon-Nucleon Interaction in a Chiral Constituent Quark Model
doi: 10.1016/S0375-9474(01)01510-X
2002SA39 Phys.Rev. C66, 034001 (2002) Phase Equivalent Chains of Darboux Transformations in Scattering Theory
doi: 10.1103/PhysRevC.66.034001
2001BA14 Phys.Rev. C63, 034001 (2001) Nucleon-Nucleon Scattering in a Chiral Constituent Quark Model
doi: 10.1103/PhysRevC.63.034001
2001BA46 Nucl.Phys. A688, 915 (2001) NN Scattering Phase Shifts in a Chiral Constituent Quark Model
doi: 10.1016/S0375-9474(00)00599-6
2001ST05 Nucl.Phys. A683, 359 (2001) The Short-Range Baryon-Baryon Interaction in a Chiral Constituent Quark Model
doi: 10.1016/S0375-9474(00)00461-9
1999BA20 Phys.Rev. C59, 1756 (1999) Important Configurations for NN Processes in a Goldstone Boson Exchange Model
doi: 10.1103/PhysRevC.59.1756
1999BA98 Phys.Rev. C60, 055207 (1999) NN Interaction in a Goldstone Boson Exchange Model
doi: 10.1103/PhysRevC.60.055207
1997ST24 Phys.Rev. C56, 2779 (1997); Erratum Phys.Rev. C59, 1219 (1999) F.Stancu, S.Pepin, L.Ya.Glozman Nucleon-Nucleon Interaction in a Chiral Constituent Quark Model
doi: 10.1103/PhysRevC.56.2779
1997ST30 Z.Phys. A359, 321 (1997) Positive Parity Nonstrange Baryons Beyond 2 GeV
doi: 10.1007/s002180050408
1997WI07 Phys.Rev. C56, 486 (1997) L.Wilets, M.A.Alberg, S.Pepin, Fl.Stancu, J.Carlson, W.Koepf Quark Substructure Approach to 4He Charge Distribution NUCLEAR STRUCTURE 4He; calculated density distribution; deduced proton size vs density. Realistic nucleonic wave functions, quark substructure, chromodielectric model.
doi: 10.1103/PhysRevC.56.486
1996PE03 Phys.Rev. C53, 1368 (1996) S.Pepin, Fl.Stancu, W.Koepf, L.Wilets Nucleon-Nucleon Interaction in the Chromodielectric Soliton Model: Dynamics
doi: 10.1103/PhysRevC.53.1368
1995ST08 Z.Phys. A351, 77 (1995) Δπ Decay of Baryons in a Flux-Tube-Breaking Mechanism
doi: 10.1007/BF01292788
1994KO22 Phys.Rev. C50, 614 (1994) W.Koepf, L.Wilets, S.Pepin, Fl.Stancu The Nucleon-Nucleon Potential in the Chromodielectric Soliton Model: Statics NUCLEAR STRUCTURE 1H; calculated μ; deduced chromodielectric soliton model parameters. Self-consistent mean field calculation. Model used for NN-interaction.
doi: 10.1103/PhysRevC.50.614
1985ST25 Phys.Rev. C32, 1937 (1985) Effect of Shell Structure on the Nucleon Transfer Contribution to the Imaginary Part of the Heavy Ion Optical Potential NUCLEAR REACTIONS 40Ca(16O, 16O), E=40-214.1 MeV; 60Ni(16O, 16O), E=142 MeV; 208Pb(16O, 16O), E=129.5-312.6 MeV; 32S(32S, 32S), E=90.9 MeV; 40Ca(40Ca, 40Ca), E=143.6-240 MeV; calculated heavy ion optical potential imaginary term near strong absorption radius.
doi: 10.1103/PhysRevC.32.1937
1984SA08 Phys.Rev. C29, 1756 (1984) Density Matrix Approach to the Complex Heavy Ion Optical Potential: Exchange part NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated optical potential parameter dependence. Density matrix approach.
doi: 10.1103/PhysRevC.29.1756
1983SA14 Nucl.Phys. A404, 392 (1983) Unified Skyrme Approach to the Real and Imaginary Parts of the Heavy-Ion Optical Potential NUCLEAR STRUCTURE 16O, 40,48Ca, 56Ni, 90Zr, 208Pb; calculated binding energies, charge radii. Hartree-Fock method, Skyrme interaction. NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated optical potential real, imaginary parts vs separation distance. Skyrme approach.
doi: 10.1016/0375-9474(83)90555-9
1983SA36 Phys.Rev. C28, 2533 (1983) Complex Heavy Ion Optical Potential and the Proximity Concept NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated optical potential components vs ion-ion separation distance. Proximity approximation.
doi: 10.1103/PhysRevC.28.2533
1983TA17 Rev.Roum.Phys. 28, 857 (1983) Fl.Stancu, M.T.Magda, S.Dima, M.Macovel, E.Ivanov, R.Dumitrescu, C.Stan-Sion Energy Spectrum of Neutrons Produced by Deuterons on Thick Be Target NUCLEAR REACTIONS 9Be(d, n), E=13 MeV; measured σ(θ), σ(En). Thin, thick targets.
1982SA20 Phys.Rev. C26, 1025 (1982) Density Matrix Approach to the Complex Heavy Ion Optical Potential NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated optical potential characteristics. Density matrix expansion, complex effective interaction.
doi: 10.1103/PhysRevC.26.1025
1982ST08 Phys.Rev. C25, 2450 (1982) Nucleon Transfer Contribution to the Absorptive Potential in Heavy-Ion Scattering NUCLEAR REACTIONS 40Ca(16O, 16O), E=55.6, 103.6, 214.1 MeV; 58Ni(16O, 16O), E=45, 60, 81 MeV; 60Ni(16O, 16O), E=142 MeV; 208Pb(16O, 16O), E=129.5, 192, 312.6 MeV; 40Ca(20Ne, 20Ne), E=151 MeV; 32S(32S, X), E=90.9 MeV; 40Ca(40Ca, 40Ca), E=143.6, 186, 240 MeV; 209Bi(136Xe, 136Xe), E=940, 1130 MeV; calculated nucleon transfer contribution to absorption potential. Proximity method, Pauli blocking, barrier penetration effects.
doi: 10.1103/PhysRevC.25.2450
1981BR11 Phys.Rev. C24, 144 (1981) Time-Dependent Hartree-Fock and the One-Body Dissipation for Head-On Collisions NUCLEAR REACTIONS 139La(86Kr, X), E=360-1000 MeV; 209Bi(84Kr, X), E=500-1000 MeV; calculated interaction potential vs separation distance, classical trajectories. Head-on collisions, window formula for friction, one-body dissipation.
doi: 10.1103/PhysRevC.24.144
1981DE13 Phys.Rev. C23, 1503 (1981) Fusion Cross Section of Light Ions at Sub-Coulomb Energies NUCLEAR REACTIONS 16O(16O, X), E(cm)=4-9.76 MeV; 12C(14N, X), E(cm)=1-6.07 MeV; 12C(10B, X), E(cm)=0.25-4.22 MeV; calculated σ(fusion, E). Barrier penetration model.
doi: 10.1103/PhysRevC.23.1503
1981GN01 Nucl.Phys. A366, 520 (1981) Classical Trajectory Calculations with Time-Dependent Forces in Heavy-Ion Collisions NUCLEAR REACTIONS 139La(86Kr, X), E=505, 610, 710 MeV; calculated σ(θ); 209Bi(136Xe, X), E=1130 MeV; calculated σ(θ, E), σ(θ), energy loss, deflection function. Classical trajectory model, time-dependent forces, deep inelastic collisions.
doi: 10.1016/0375-9474(81)90525-X
1981SA33 Phys.Rev. C24, 2347 (1981) The Nucleus-Nucleus Optical Potential Derived from a Complex Skyrme-Type Interaction NUCLEAR REACTIONS 16O(16O, 16O), E=83, 322 MeV; calculated nucleus-nucleus optical potential. Complex energy function, Skyrme-type interaction.
doi: 10.1103/PhysRevC.24.2347
1979ST14 Phys.Rev.Lett. 43, 1094 (1979) Static Polarization Effects in the Nucleus-Nucleus Potential NUCLEAR REACTIONS 90Zr, 40Ca(40Ca, X), 90Zr, 208Pb(90Zr, X), 48Ca, 56Ni(208Pb, X), E not given; calculated real part of nucleus-nucleus potential. Variable surface thickness. Deduced barrier, its position for an arbitrary pair.
doi: 10.1103/PhysRevLett.43.1094
1978ST24 J.Phys.(Paris) 39, 799 (1978) The Sensitivity of the Real Part of the Nucleus-Nucleus Potential to Nuclear Densities NUCLEAR REACTIONS 48Ca(16O, 16O), E=40 MeV; 48Ca(48Ca, 48Ca), 208Pb(16O, 16O), E not given; calculated real part of nucleus-nucleus potential. Method based on energy functional of Skyrme nucleon-nucleon interaction.
doi: 10.1051/jphys:01978003908079900
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
1976ST15 Nucl.Phys. A270, 236 (1976) The Real Part of the Nucleus-Nucleus Interaction NUCLEAR REACTIONS 48Ca(16O, 16O), E=40, 60 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(76)90137-8
1975BR13 Nucl.Phys. A243, 175 (1975) Interaction Potential between Two 16O Nuclei Derived from the Skyrme Interaction NUCLEAR REACTIONS 16O(16O, 16O); calculated potential.
doi: 10.1016/0375-9474(75)90027-5
1973ST05 Nucl.Phys. A205, 561 (1973) Separable-Potential Model for the Nucleon-Nucleus Interaction NUCLEAR REACTIONS 16O(n, n); calculated σ(E).
doi: 10.1016/0375-9474(73)90706-9
1972ST02 Nucl.Phys. A179, 714 (1972) Separable Single-Particle Hamiltonian and its Local Equivalent NUCLEAR REACTIONS 3He, 11C, 15O, 39Ca(n, n), E=0.216, 4.659 MeV; calculated equivalent local potentials, damping functions.
doi: 10.1016/0375-9474(72)90614-8
1968GU11 Nuovo Cimento 58A, 503 (1968) Particle-Hole Description of Even-Parity T = 1 Levels of 12B NUCLEAR STRUCTURE 12B; calculated even-parity levels. Particle-hole model.
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