NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = F.Palumbo Found 19 matches. 2019PA11 Nucl.Phys. A983, 64 (2019) The D2 point group of the Two-Rotors Model and scissors modes of negative parity
doi: 10.1016/j.nuclphysa.2018.12.022
2019PA17 Phys.Rev. C 99, 034319 (2019) Inertia tensor and fine structure of scissors-mode resonances NUCLEAR STRUCTURE 150Nd, 156Gd, 166,168Er, 172Yb, 182,184W, 190Os; calculated relative energy splitting, and relative B(M1) strength differences using the two-rotors model (TRM) method for scissors mode. Comparison of the structure of scissors-mode resonances (SRs) in the rare-earth elements with irrotational inertia tensor on one side, and two-fluid and rigid one on the other.
doi: 10.1103/PhysRevC.99.034319
2016PA09 Phys.Rev. C 93, 034331 (2016) Entanglement in the states of the two-rotors model NUCLEAR STRUCTURE 25O; calculated energy, J and π of unbound level or resonance, width, decay energy spectrum and width for d3/2 configuration using the neutron+24O model; calibrated Woods-Saxon potential. 26O; calculated uncorrelated and correlated decay energy spectra using uncorrelated two-neutron state in 27F with the 1d3/21d3/2, 0+ configuration as a reference state, mean-square neutron-neutron distance and the core-dineutron distance, density distributions, angular density for the ground state as function of the angle between the two valence neutrons, decay energy spectra and configurations for the 0+ and 2+ states in 26O, angular correlations between the emitted neutrons from the two-neutron decay. 24O+n+n three-body model. Comparison with experimental data. 16,17,18,19,21,22,23,24O; calculated root-mean-square (rms) radii, and compared with experimental values. 26O; calculated root-mean-square (rms) radius with the three-body model calculation using the empirical rms radius of 24O. RADIOACTIVITY 26O(2n); calculated energy, decay energy spectrum, angular correlations between the emitted neutrons. 24O+n+n three-body model. Comparison with experimental data.
doi: 10.1103/PhysRevC.93.034331
2013HA16 Phys.Rev. C 88, 014305 (2013) K.Hatada, K.Hayakawa, F.Palumbo Scissors modes: The elusive breathing overtone
doi: 10.1103/PhysRevC.88.014305
2011HA32 Phys.Rev. C 84, 011302 (2011) K.Hatada, K.Hayakawa, F.Palumbo Scissors modes: The first overtone
doi: 10.1103/PhysRevC.84.011302
2005PA43 Phys.Rev. C 72, 014303 (2005) Boson dominance in nuclei
doi: 10.1103/PhysRevC.72.014303
2004BA82 Phys.Rev. C 70, 034309 (2004) M.B.Barbaro, A.Molinari, F.Palumbo, M.R.Quaglia Goldstone bosons in the pairing Hamiltonian: The path integral approach
doi: 10.1103/PhysRevC.70.034309
1999DE34 Phys.Rev. D60, 074008 (1999) Quark-Composites Approach to QCD: The nucleons
doi: 10.1103/PhysRevD.60.074008
1999PA37 Phys.Rev. D60, 074009 (1999) Quark-Composites Approach to QCD: The nucleon-pion system
doi: 10.1103/PhysRevD.60.074009
1990LO08 Phys.Rev. C42, 241 (1990) N.Lo Iudice, F.Palumbo, A.Richter, H.J.Wortche Semiclassical Description of the Scissors Mode: Possible improvements and intrinsic limitations NUCLEAR REACTIONS 164Dy(e, e'), E not given; calculated form factors. Two-rotor model. NUCLEAR STRUCTURE 164Dy; calculated normalized transition density. Two-rotor model.
doi: 10.1103/PhysRevC.42.241
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
1985PA16 Phys.Lett. 158B, 101 (1985) Splitting of the Magnetic Dipole Giant Resonance and Triaxial Deformation NUCLEAR STRUCTURE 164Dy, 174Yb; analyzed magnetic GDR splitting; deduced triaxial deformation role.
doi: 10.1016/0370-2693(85)91371-1
1985RA08 Phys.Rev. C31, 1656 (1985) C.Rangacharyulu, E.J.Ansaldo, D.Stockhausen, D.Bender, S.Muller, A.Richter, N.Lo Iudice, F.Palumbo Search for Isovector Magnetic Quadrupole Strength and Spin-Isospin Correlations in 20Ne NUCLEAR REACTIONS 20Ne(e, e'), E=39.5-59.3 MeV; measured σ(E(e')), form factors. 20Ne deduced transitions, B(M2) distribution.
doi: 10.1103/PhysRevC.31.1656
1984BO09 Phys.Lett. 137B, 27 (1984) D.Bohle, A.Richter, W.Steffen, A.E.L.Dieperink, N.Lo Iudice, F.Palumbo, O.Scholten New Magnetic Dipole Excitation Mode Studied in the Heavy Deformed Nucleus 156Gd by Inelastic Electron Scattering NUCLEAR REACTIONS 156Gd(e, e'), E=25-56 MeV; measured σ(E(e')), σ(θ), M1 transition form factor. 158Gd(e, e'), E=25 MeV; measured σ(E(e')). 156Gd deduced collective magnetic dipole excitation mode, B(λ). 158Gd deduced evidence for collective magnetic dipole excitation mode.
doi: 10.1016/0370-2693(84)91099-2
1984DE10 Phys.Rev. C29, 1496 (1984) G.De Franceschi, F.Palumbo, N.Lo Iudice Reformulation of the Two-Rotor Model NUCLEAR STRUCTURE 156Gd; calculated M1 form factor. Two-rotor model reformulation.
doi: 10.1103/PhysRevC.29.1496
1984LO05 Phys.Rev. C30, 360 (1984) M2 Collective Excitations in Light Deformed Nuclei and Their Relationship to the One Pion Exchange Potential NUCLEAR STRUCTURE 12C, 28Si, 22Ne, 24Mg, 32S; calculated B(M2) strength distribution. One-pion exchange model.
doi: 10.1103/PhysRevC.30.360
1983LO04 Lett.Nuovo Cim. 36, 91 (1983) Spin-Isospin Collective Excitations in Light Oblate Nuclei NUCLEAR STRUCTURE 12C, 28Si; calculated B(M2). Spin, isospin collective excitations, semi-classical model.
doi: 10.1007/BF02751839
1981LO04 Phys.Rev.Lett. 46, 1054 (1981) Nonstatic Spin-Isospin Order in Light Nuclei NUCLEAR STRUCTURE A=12, 28; calculated levels, B(M2). Semimicroscopic model, one pion exchange.
doi: 10.1103/PhysRevLett.46.1054
1972GA26 Phys.Lett. 40B, 621 (1972) Center of Mass Spuriosity Effects on the Charge Form Factor in Many-Body Theories NUCLEAR STRUCTURE 4He, 16O; analyzed cms spuriosity effects on charge form factor. Saxon-Woods wave functions.
doi: 10.1016/0370-2693(72)90611-9
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