NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = S.Stringari Found 36 matches. 1990LE14 Phys.Rev. C42, 416 (1990) W.Leidemann, E.Lipparini, S.Stringari Asymmetry in Inclusive Polarized Electron Scattering from Polarized Nuclei: Sum rule approach NUCLEAR REACTIONS 3He, 7Li, 9Be, 2H(polarized e, e'), E not given; calculated average asymmetry. Polarized electrons, polarized nuclei, sum rule approach.
doi: 10.1103/PhysRevC.42.416
1990ST17 Nucl.Phys. A516, 33 (1990) S.Stringari, M.Traini, O.Bohigas Momentum Distribution in Heavy Nuclei NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb, 4He; calculated nucleon momentum distribution. Local density approximation.
doi: 10.1016/0375-9474(90)90046-O
1989LI14 Phys.Rev. C40, R19 (1989) Electron Scattering Sum Rules in Polarized Nuclei NUCLEAR REACTIONS 3He, 2H(polarized e, e'), E not given; calculated sum rules; deduced nucleon form factor role.
doi: 10.1103/PhysRevC.40.R19
1988LI13 Nucl.Phys. A482, 205c (1988) Surface and Temperature Effects in Isovector Giant Resonances NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 140Ce, 208Pb; calculated giant resonance excitation; deduced surface, temperature effects role, sum rules. Liquid droplet model.
doi: 10.1016/0375-9474(88)90585-4
1988LI24 Phys.Lett. 212B, 6 (1988) E.Lipparini, S.Stringari, R.Leonardi Isospin Effects and Dynamic Correlations in Inclusive Muon Capture in N ≠ Z Nuclei NUCLEAR STRUCTURE 40,48Ca, 60Ni, 90Zr, 140Ce, 208Pb; calculated μ- capture rate. ATOMIC PHYSICS, Mesic-Atoms 40,48Ca, 60Ni, 90Zr, 140Ce, 208Pb(μ-, X), E at rest; calculated muon capture rate.
doi: 10.1016/0370-2693(88)91225-7
1987BO38 Phys.Lett. 197B, 497 (1987) J.D.Bowman, E.Lipparini, S.Stringari Isovector Monopole Excitation Energies NUCLEAR STRUCTURE A=20-220; calculated isovector dipole, monopole levels. Hydrodyamical model.
doi: 10.1016/0370-2693(87)91041-0
1987CH11 Phys.Lett. 189B, 375 (1987) Ph.Chomaz, Nguyen Van Giai, S.Stringari Lifetimes of Monopole Resonances in Time-Dependent Hartree-Fock Theory NUCLEAR STRUCTURE 16O, 40Ca; calculated monopole resonance particle decay T1/2, transition strength distribution. TDHF approach.
doi: 10.1016/0370-2693(87)90643-5
1987LE10 Phys.Rev. C35, 1439 (1987) R.Leonardi, E.Lipparini, S.Stringari Peculiarity of the Charge-Exchange Quadrupole Excitation in Nuclei NUCLEAR STRUCTURE 90Zr; calculated isovector quadrupole strength distribution.
doi: 10.1103/PhysRevC.35.1439
1987LI13 Phys.Rev.Lett. 59, 982 (1987) Hydrodynamic Model in Isospin Channels NUCLEAR STRUCTURE 60Ni, 90Zr, 120Sn, 140Ce, 208Pb; calculated GDR isospin splitting. 48Ca, 60Ni, 90Zr, 120Sn, 208Pb; calculated total transition strengths. Steinwedel-Jensen hydrodynamic model.
doi: 10.1103/PhysRevLett.59.982
1987LI31 Phys.Rev. C36, 2697 (1987) Coupling between the Isoscalar and Isovector Monopole Resonances in N ≠ Z Nuclei NUCLEAR STRUCTURE 40Ca, 90Zr, 140Ce, 208Pb; calculated isovector, isoscalar monopole resonances, energy weighted sum rules.
doi: 10.1103/PhysRevC.36.2697
1987LI33 J.Phys.(Paris), Colloq.C-2, 27 (1987) Charge Exchange Excitations in N ≠ Z Nuclei: Vlasov and hydrodynamic equations NUCLEAR STRUCTURE 40,48Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb; calculated GDR isospin splitting, strengths. Time dependent Hartree-Fock theory. NUCLEAR REACTIONS 40,48Ca, 60Ni, 90Zr, 140Ce, 208Pb(μ-, γ), E at rest; calculated capture rates.
1987ST24 Nucl.Phys. A473, 61 (1987) Macroscopic Models for Charge Exchange Reactions in N not Equal to Z Nuclei NUCLEAR STRUCTURE 48Ca, 60Ni, 90Zr, 120Sn, 208Pb; calculated levels, giant resonance isospin splitting, charge exchange dipole mode total transition strengths. Time-dependent Hartree-Fock.
doi: 10.1016/0375-9474(87)90155-2
1986LI06 Nucl.Phys. A455, 294 (1986) On the Equivalence between the Landau-Migdal and the Bohr-Mottelson Interactions NUCLEAR STRUCTURE 48Ca, 90Zr, 208Pb; calculated Gamow-Teller, M1 transition strengths; deduced Landau-Migdal, Bohr-Mottelson interaction equivalence.
doi: 10.1016/0375-9474(86)90019-9
1985LI18 Phys.Lett. 160B, 221 (1985) E.Lipparini, S.Stringari, A.Richter Variational Approach to Magnetic Dipole Core Polarization: Applications to moments and transitions NUCLEAR STRUCTURE A=48-209; calculated core polarization corrections to μ, B(M1). Variational approach.
doi: 10.1016/0370-2693(85)91314-0
1985LO12 Phys.Lett. 161B, 18 (1985) N.Lo Iudice, E.Lipparini, S.Stringari, F.Palumbo, A.Richter Effect of Triaxial Deformations on the Splitting of the M1 Isovector Rotational State NUCLEAR STRUCTURE 164Dy, 174Yb; calculated isovector rotational states, M1 transition strength fragmentation. Sum rule approach.
doi: 10.1016/0370-2693(85)90599-4
1985ST11 Nuovo Cim. 87A, 231 (1985) Fluid-Dynamic Models from the Boltzmann Equations NUCLEAR STRUCTURE A=20-240; calculated isoscalar quadrupole giant resonance energy. A=20-220; calculated octupole giant resonance energy. Fluid dynamical models, Boltzmann equations.
doi: 10.1007/BF02902348
1984ST03 Phys.Rev. C29, 1482 (1984) Long Range Dipole Correlations and Electron Scattering Sum Rules NUCLEAR STRUCTURE 12C, 40Ca; calculated longitudinal, transverse sum rule strength vs momentum transfer. RPA, Schematic model. NUCLEAR REACTIONS 12C(e, e'), E not given; calculated total σ(inelastic) vs momentum transfer; deduced dipole correlations role. RPA, schematic model.
doi: 10.1103/PhysRevC.29.1482
1983LI12 Phys.Lett. 130B, 139 (1983) Isovector M1 Rotational States in Deformed Nuclei NUCLEAR STRUCTURE A ≈ 180; calculated isovector rotational state B(M1). Sum rule approach, comparison with other models.
doi: 10.1016/0370-2693(83)91028-6
1983ST12 Prog.Theor.Phys.(Kyoto), Suppl. 74/75, 367 (1983) Symmetry Energy and Isovector Collective Motions NUCLEAR STRUCTURE 16O, 40Ca, 140Ce, 208Pb; calculated GDR energy. Self-consistent RPA, macroscopic hydrodynamical models.
doi: 10.1143/PTPS.74.367
1982DA03 Nucl.Phys. A376, 81 (1982) M.Dal Ri, S.Stringari, O.Bohigas Effects of Short Range Correlations on One- and Two-Body Properties of Nuclei NUCLEAR STRUCTURE 4He; calculated two-body density, momentum distribution, elastic, inelastic form factors; deduced short range correlation effects. Jastrow formalism, low-order approximation.
doi: 10.1016/0375-9474(82)90534-6
1982LE27 Phys.Rev. C26, 2636 (1982) R.Leonardi, E.Lipparini, S.Stringari Microscopic Model for the Isospin Fragmentation of the Dipole Mode NUCLEAR STRUCTURE 90Zr, 116,120,124Sn, 208Pb; calculated isospin splitting. RPA, schematic force.
doi: 10.1103/PhysRevC.26.2636
1982LI07 Phys.Lett. 112B, 421 (1982) Volume and Surface Symmetry Energy Coeffecients from Photoabsorption Cross Sections NUCLEAR STRUCTURE 16O, 40Ca, 140Ce, 208Pb; analyzed GDR data; deduced volume, surface symmetry energy parameters. Hydrodynamic model.
doi: 10.1016/0370-2693(82)90839-5
1982OR07 Phys.Lett. 119B, 21 (1982) G.Orlandini, S.Stringari, M.Traini Isoscalar Transition Density for the Low-Lying Dipole States NUCLEAR STRUCTURE 16O, 40Ca; calculated isoscalar dipole state EWSR, transition density. Microscopic model, center of mass motion.
doi: 10.1016/0370-2693(82)90234-9
1982ST04 Phys.Lett. 108B, 232 (1982) Sum Rules for Compression Modes NUCLEAR STRUCTURE 208Pb; calculated T=0, giant monopole, dipole resonance transition density. Sum rule approach.
doi: 10.1016/0370-2693(82)91182-0
1982ST14 Phys.Lett. 117B, 141 (1982) Hydrodynamical Approach to the Difference between Neutron and Proton Radii NUCLEAR STRUCTURE 40,48Ca, 90Zr, 208Pb; calculated neutron, proton radii differences. Hydrodynamical model.
doi: 10.1016/0370-2693(82)90533-0
1981LI03 Phys.Lett. 99B, 183 (1981) Surface Symmetry Energy and the Dipole Giant Resonance NUCLEAR STRUCTURE A=16-208; calculated GDR energy vs mass; deduced surface symmetry energy effects. RPA, sum rule approach, Woods-Saxon shape for potentials, isovector densities.
doi: 10.1016/0370-2693(81)91103-5
1981ST10 Phys.Lett. 103B, 5 (1981) Effects of Velocity Dependent Potentials in the Low-Lying Octupole Vibration NUCLEAR STRUCTURE A=16-250; calculated octupole energy, fragmentation; deduced spin-orbit interaction, effective mass effects. Schematic RPA model.
doi: 10.1016/0370-2693(81)90181-7
1980CH25 Phys.Lett. B95, 344 (1980) P.Christillin, E.Lipparini, S.Stringari, M.Traini Inclusive Radiative Pion and Muon Capture in N=Z Nuclei NUCLEAR REACTIONS 16O, 40Ca(π-, γ), (μ-, γ), E at rest; calculated excitation energy, total capture rate; deduced dependence on captured particle orbit. Sum rule method.
doi: 10.1016/0370-2693(80)90165-3
1980ST14 Phys.Rev. C22, 884 (1980) Variational Approach to the Moment of Inertia NUCLEAR STRUCTURE 20Ne; calculated irrotational, rigid moments of inertia. Cranked Hartree-Fock method.
doi: 10.1103/PhysRevC.22.884
1979LI10 Phys.Lett. 84B, 1 (1979) Spin Oscillations and the M1 Magnetic Form Factor NUCLEAR STRUCTURE 90Zr; calculated electroexcitation, M1 transverse form factor vs momentum transfer; discussed nuclear deformation induced by external magnetic field.
doi: 10.1016/0370-2693(79)90634-8
1979ST20 Phys.Lett. 88B, 1 (1979) Damping of Monopole Vibrations in Time-Dependent Hartree-Fock Theory NUCLEAR STRUCTURE 16O, 40Ca; calculated monopole modes; deduced damping due to particle emission. time-dependent Hartree-Fock calculations, time dependent Schrodinger equation.
doi: 10.1016/0370-2693(79)90099-6
1979TR03 Nucl.Phys. A318, 162 (1979) M.Traini, E.Lipparini, G.Orlandini, S.Stringari Magnetic Susceptibility and M1 Transitions in 208Pb NUCLEAR STRUCTURE 208Pb; calculated energy-weighted, inverse energy-weighted sum rules; deduced M1 strengths, excitation energies.
doi: 10.1016/0375-9474(79)90477-9
1977LI17 Lett.Nuovo Cim. 19, 171 (1977) E.Lipparini, S.Stringari, M.Traini Skyrme's Interaction and Corrections to Gyromagnetic Factors NUCLEAR STRUCTURE 15N, 17O, 39K, 41Ca; calculated corrections to g using Skyrme interaction.
1977LI21 Nucl.Phys. A293, 29 (1977) E.Lipparini, S.Stringari, M.Traini Magnetic Moments and the Skyrme Interaction NUCLEAR MOMENTS 27Al, 29Si, 55Co, 57Ni, 89Y, 91Zr, 207Pb, 209Bi; calculated μ.
doi: 10.1016/0375-9474(77)90474-2
1976LI26 Nuovo Cim. 34A, 48 (1976) E.Lipparini, S.Stringari, M.Traini Sum Rule Approach to Radiative Pion Capture in Nuclei NUCLEAR REACTIONS 4He, 6Li, 10B, 12C, 14N, 16O(π, γ); calculated capture rates.
doi: 10.1007/BF02813879
1976ST13 Nucl.Phys. A269, 87 (1976) S.Stringari, R.Leonardi, D.M.Brink Spin Stability and Magnetic Polarizability with Skyrme's Interaction NUCLEAR STRUCTURE 12C, 28Si, 56Ni; calculated spin polarizability. Skyrme effective interaction.
doi: 10.1016/0375-9474(76)90398-5
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