NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = F.Catara Found 75 matches. 2019LA21 Eur.Phys.J. A 55, 235 (2019) E.G.Lanza, L.Pellegri, M.V.Andres, F.Catara, A.Vitturi Low-lying dipole and quadrupole states
doi: 10.1140/epja/i2019-12797-y
2018MA36 Phys.Lett. B 782, 112 (2018) N.S.Martorana, G.Cardella, E.G.Lanza, L.Acosta, M.V.Andres, L.Auditore, F.Catara, E.De Filippo, S.De Luca, D.Dell'Aquila, B.Gnoffo, G.Lanzalone, I.Lombardo, C.Maiolino, S.Norella, A.Pagano, E.V.Pagano, M.Papa, S.Pirrone, G.Politi, L.Quattrocchi, F.Rizzo, P.Russotto, D.Santonocito, A.Trifiro, M.Trimarchi, M.Vigilante, A.Vitturi First measurement of the isoscalar excitation above the neutron emission threshold of the Pygmy Dipole Resonance in 68Ni NUCLEAR REACTIONS 12C(68Ni, γ), E=28 MeV/nucleon; measured reaction products, Eγ, Iγ. 68Ni; deduced σ(E), σ(θ), γ-ray decay of the pygmy resonance.
doi: 10.1016/j.physletb.2018.05.019
2018MA46 Acta Phys.Pol. B49, 475 (2018) N.S.Martorana, G.Cardella, E.G.Lanza, L.Acosta, M.V.Andres, L.Auditore, F.Catara, E.De Filippo, S.De Luca, D.Dell'Aquila, B.Gnoffo, G.Lanzalone, I.Lombardo, C.Maiolino, S.Norella, A.Pagano, E.V.Pagano, M.Papa, S.Pirrone, G.Politi, L.Quattrocchi, F.Rizzo, P.Russotto, D.Santonocito, A.Trifiro, M.Trimarchi, M.Vigilante, A.Vitturi Experimental Study of the Pygmy Dipole Resonance in the 68Ni Nucleus NUCLEAR REACTIONS 9Be(70Zn, x), E=40 MeV/nucleon; measured fragmentation products, mainly 66,67,68Ni; 12C(p, x), E=24 MeV; measured protons, γ-rays; deduced Q-value spectrum, deduced total Doppler-corrected γ-ray energy spectrum in coincidence with 66,67,68Ni detected with CsI(Tl) of CHIMERA in coincidence with inelastic and with elastic channels, not normalized σ(θ), yield of Pygmy Dipole Resonance (PDR) obtained using subtraction of other channels. NEWCHIM-CHIMERA Collaboration standard tagging system, which allows event-by-event measurement of the isotopic composition.
doi: 10.5506/aphyspolb.49.475
2016GA04 Phys.Rev. C 93, 024309 (2016) D.Gambacurta, F.Catara, M.Grasso, M.Sambataro, M.V.Andres, E.G.Lanza Nuclear excitations as coupled one and two random-phase-approximation modes NUCLEAR STRUCTURE 16O; calculated low-lying levels and giant resonances (dipole, quadrupole and octupole), J, π, monopole (E0), dipole (E1), isoscalar quadrupole (E2), and isoscalar octupole (E3) response functions. Double random-phase approximation (DRPA) method to include two -particle two-hole (2p-2h) configurations and by coupling them with the 1p-1h ones and among themselves. Comparison with experimental values.
doi: 10.1103/PhysRevC.93.024309
2012GA31 Phys.Rev. C 86, 021304 (2012) D.Gambacurta, M.Grasso, V.De Donno, G.Co, F.Catara Second random-phase approximation with the Gogny force: First applications NUCLEAR STRUCTURE 16O; calculated isoscalar monopole discrete strength distribution B(E0), isoscalar monopole response, proton and neutron transition densities. Random-phase approximation (RPA), second RPA (SRPA) with finite-range Gogny interaction. Discussed effects of particle-hole couplings in Gogny-SRPA calculations.
doi: 10.1103/PhysRevC.86.021304
2011GA02 J.Phys.(London) G38, 035103 (2011) D.Gambacurta, M.Grasso, F.Catara Residual interaction in second random-phase approximation with density-dependent forces: rearrangement terms
doi: 10.1088/0954-3899/38/3/035103
2011GA39 Phys.Rev. C 84, 034301 (2011) D.Gambacurta, M.Grasso, F.Catara Low-lying dipole response in the stable 40, 48Ca nuclei with the second random-phase approximation NUCLEAR STRUCTURE 40,48Ca; calculated isoscalar and isovector B(E1) strength distributions in 5-10 MeV excitation region, EWSR, neutron and proton transition densities. Random-phase approximation (RPA) and second random-phase approximation (SRPA) with Skyrme interaction SGII with inclusion of 2p2h configurations. Pygmy resonances. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.034301
2011LA22 Phys.Rev. C 84, 064602 (2011) E.G.Lanza, A.Vitturi, M.V.Andres, F.Catara, D.Gambacurta Excitations of pygmy dipole resonances in exotic and stable nuclei via Coulomb and nuclear fields NUCLEAR REACTIONS 132Sn(α, α'), (40Ca, 40Ca'), (48Ca, 48Ca'), E=30, 60, 100 MeV; 208Pb(17O, 17O'), E=20, 50 MeV; calculated form factors for PDR states and GDR, partial wave cross sections, differential cross sections. 100Sn, 120Sn, 132Sn, 208Pb; calculated isovector strength distributions B(E1), RPA transition strengths for low-lying states. Hartree-Fock plus RPA random phase approximation (RPA), with Skyrme interaction.
doi: 10.1103/PhysRevC.84.064602
2010GA07 Phys.Rev. C 81, 054312 (2010) D.Gambacurta, M.Grasso, F.Catara Collective nuclear excitations with Skyrme-second random-phase approximation NUCLEAR STRUCTURE 16O; calculated isoscalar and isovector strength distributions for monopole 0+, dipole 1- and quadrupole 2+ states, B(E0), B(E1), B(E2), transition densities using second random phase approximation using second random-phase approximation (SRPA) calculations with a Skyrme force. Comparison between RPA and SRPA calculations.
doi: 10.1103/PhysRevC.81.054312
2010VI02 Pramana 75, 73 (2010) A.Vitturi, E.G.Lanza, M.V.Andres, F.Catara, D.Gambacurta Excitation of pygmy dipole resonance in neutron-rich nuclei via Coulomb and nuclear fields NUCLEAR REACTIONS 208Pb(132Sn, 132Sn'), E=6, 10, 20, 50 MeV/nucleon; 4He, 40,48Ca(132Sn, 132Sn'), E=10 MeV/nucleon; 132Sn; calculated σ(θ), σ(E), transition densities of dipole state, B(E1), form factors.
doi: 10.1007/s12043-010-0066-z
2009GA22 Phys.Rev. C 80, 014303 (2009) D.Gambacurta, F.Catara, M.Grasso Self-consistent extension of random-phase approximation enlarged beyond particle-hole configurations
doi: 10.1103/PhysRevC.80.014303
2009LA11 Phys.Rev. C 79, 054615 (2009) E.G.Lanza, F.Catara, D.Gambacurta, M.V.Andres, Ph.Chomaz Multiphonon excitations and pygmy resonances in tin isotopes NUCLEAR REACTIONS 100,120,132Sn(γ, γ'), E not given; calculated proton and neutron densities, isoscalar strength distributions for monopole, quadrupole and octupole states, isovector strength distributions for dipole states, transition probabilities, transition densities for low-lying dipole state for pygmy dipole resonance and giant dipole resonance. Microscopic RPA and boson expansion calculations. 120,132Sn(208Pb, X), E=500 MeV/nucleon; calculated relativistic Coulomb inelastic cross sections using coupled-channel method.
doi: 10.1103/PhysRevC.79.054615
2007LA28 Nucl.Phys. A788, 112c (2007) E.G.Lanza, M.V.Andres, F.Catara, Ph.Chomaz, M.Fallot, J.A.Scarpaci Triple Giant Resonance Excitations: A Microscopic Approach NUCLEAR REACTIONS 40Ca(40Ca, 40Ca'), E=25, 50, 100 MeV/nucleon; 208Pb(208Pb, 208Pb'), E=641 MeV/nucleon; calculated σ(E), one-, two-, and three-phonon components, giant resonance excitation. Microscopic extended RPA with anharmonicity.
doi: 10.1016/j.nuclphysa.2007.01.056
2006GA02 Phys.Rev. C 73, 014310 (2006) D.Gambacurta, M.Sambataro, F.Catara Solvable many-level pairing model in a boson formalism
doi: 10.1103/PhysRevC.73.014310
2006GA09 Phys.Rev. C 73, 024319 (2006) D.Gambacurta, M.Grasso, F.Catara, M.Sambataro Extension of the second random-phase approximation
doi: 10.1103/PhysRevC.73.024319
2006LA30 Phys.Rev.C 74, 064614 (2006) E.G.Lanza, F.Catara, M.V.Andres, Ph.Chomaz, M.Fallot, J.A.Scarpaci Microscopic calculations of double and triple giant resonance excitations in heavy ion collisions NUCLEAR REACTIONS 40Ca(40Ca, 40Ca'), E=50 MeV/nucleon; 208Pb(208Pb, 208Pb'), E=641 MeV/nucleon; calculated σ(E), one-, two-, and three-phonon components, giant resonance excitation. Microscopic extended RPA with anharmonicity, effects of four phonon states estimated.
doi: 10.1103/PhysRevC.74.064614
2003FA17 Nucl.Phys. A729, 699 (2003) M.Fallot, Ph.Chomaz, M.V.Andres, F.Catara, E.G.Lanza, J.A.Scarpaci Anharmonic vibrations in nuclei NUCLEAR STRUCTURE 40Ca, 208Pb; calculated two- and three-phonon states configurations, strength distributions, mixing features, giant resonance effects.
doi: 10.1016/j.nuclphysa.2003.10.001
2002AN01 Phys.Rev. C65, 014608 (2002) M.V.Andres, F.Catara, E.G.Lanza, Ph.Chomaz, M.Fallot, J.A.Scarpaci Microscopic Description of Coulomb and Nuclear Excitation of Multiphonon States in 40Ca + 40Ca Collisions NUCLEAR REACTIONS 40Ca(40Ca, X), E=50 MeV/nucleon; calculated inelastic σ(E), population of one- and two-phonon states; deduced role of anharmonicities and nonlinearities. RPA approach.
doi: 10.1103/PhysRevC.65.014608
2002GR30 Phys.Rev. C 66, 064303 (2002) M.Grasso, F.Catara, M.Sambataro Boson-mapping-based extension of the random-phase approximation in a three-level Lipkin model
doi: 10.1103/PhysRevC.66.064303
2001GR03 Phys.Rev. C63, 014317 (2001) Extension of Random-Phase Approximation Preserving Energy Weighted Sum Rules: An application to a 3-level Lipkin model
doi: 10.1103/PhysRevC.63.014317
2000KW01 Acta Phys.Pol. B31, 2029 (2000) E.Kwasniewicz, F.Catara, M.Sambataro Description of A = 22 Nuclei in the Collective Pair Approximation NUCLEAR STRUCTURE A=22; calculated levels, J. Collective pair approximation.
2000VO17 Fiz.Elem.Chastits At.Yadra 31, 905 (2000); Phys.Part.Nucl. 31, 452 (2000) V.V.Voronov, D.Karadjov, F.Catara, A.P.Severyukhin Ground State Correlations Beyond the Random Phase Approximation and Collective Excitations NUCLEAR STRUCTURE 64Zn; calculated transition densities. 68Zn; calculated ground state quasiparticle distribution, transition densities, B(E2) for vibrational states. Fermionic approach, extended RPA.
1999AN51 Phys.Lett. 470B, 6 (1999) M.V.Andres, E.G.Lanza, P.Van Isacker, C.Volpe, F.Catara Excitation of Multiple Giant Dipole Resonances: From spherical to deformed nuclei NUCLEAR STRUCTURE 148,150,152,154Sm, 238U; calculated multiple GDR B(E1) distributions. Interacting boson model. NUCLEAR REACTIONS 208Pb(238U, 238U'), E=0.5 GeV/nucleon; 148,150,152,154Sm(208Pb, 208Pb'), E=0.5 GeV/nucleon; calculated Coulomb excitation σ(E); deduced multiple GDR, deformation effects.
doi: 10.1016/S0370-2693(99)01220-4
1999LA33 Nucl.Phys. (Supplement) A654, 792c (1999) E.G.Lanza, M.V.Andres, F.Catara, Ph.Chomaz, C.Volpe Microscopic Description of Multiphonon States Excitation in Heavy Ion Collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E=50, 641 MeV/nucleon; calculated GDR, double-GDR excitation σ and σ(E). Comparison with data. Microscopic approach.
doi: 10.1016/S0375-9474(00)88548-6
1999VO04 Nucl.Phys. A647, 246 (1999) C.Volpe, Ph.Chomaz, M.V.Andres, F.Catara, E.G.Lanza Boson Expansion Methods Applied to a Two-Level Model in the Study of Multiple Giant Resonances
doi: 10.1016/S0375-9474(99)00016-0
1998KA60 Nucl.Phys. A643, 259 (1998) D.Karadjov, V.V.Voronov, F.Catara, M.Grinberg, A.P.Severyukhin Effects of the Ground State Correlations on the Structure of Vibrational States NUCLEAR STRUCTURE 68Zn; calculated vibrational states energies, up-transition B(λ), transition charge density; deduced ground state correlations effects. Extended RPA.
doi: 10.1016/S0375-9474(98)00563-6
1998LA17 Nucl.Phys. A636, 452 (1998) E.G.Lanza, M.V.Andres, F.Catara, Ph.Chomaz, C.Volpe Microscopic Description of Coulomb and Nuclear Excitation of Multiphonon States in Heavy Ion Collisions NUCLEAR REACTIONS 208Pb(208Pb, 208Pb'), E=50 MeV/nucleon; calculated inelastic σ(Ex, L) ; deduced nuclear, Coulomb contributions, role of anharmonicities, nonlinearities.
doi: 10.1016/S0375-9474(98)00222-X
1997CA06 Nucl.Phys. A614, 86 (1997) F.Catara, E.G.Lanza, M.A.Nagarajan, A.Vitturi Collective Transition Densities in Neutron-Rich Nuclei NUCLEAR STRUCTURE 28O, 60Ca; calculated nucleon ground state densities, isoscalar, isovector transition strength distribution, RPA transition densities. 40Ca, 208Pb; calculated isoscalar, isovector transition strength distribution for RPA quadrupole states.
doi: 10.1016/S0375-9474(96)00457-5
1997CA51 Nucl.Phys. A624, 449 (1997) F.Catara, E.G.Lanza, M.A.Nagarajan, A.Vitturi Effect of Large Neutron Excess on the Dipole Response in the Region of the Giant Dipole Resonance NUCLEAR STRUCTURE 16,28O, 40,48,60,70Ca; calculated dipole response; 28O, 60,70Ca; calculated transition densities; deduced neutron excess effects. Hartree-Fock plus RPA, Skyrme interaction.
doi: 10.1016/S0375-9474(97)00485-5
1997KW02 Acta Phys.Pol. B28, 1249 (1997) E.Kwasniewicz, F.Catara, M.Sambataro The Structure of 1s0d- 1p0f-Shell Nuclei in the Collective Pair Approximation NUCLEAR STRUCTURE 20Ne; calculated levels; deduced shell model truncation effects. Collective pair approximation.
1997KW03 J.Phys.(London) G23, 911 (1997) E.Kwasniewicz, F.Catara, M.Sambataro Structure of Odd-A 1s0d- and 1p0f-Shell Nuclei in the Collective Pair Approximation NUCLEAR STRUCTURE A=19; A=21; A=43; calculated levels. Collective pair approximation, shell model comparison.
doi: 10.1088/0954-3899/23/8/006
1997LA07 Nucl.Phys. A613, 445 (1997) E.G.Lanza, M.V.Andres, F.Catara, Ph.Chomaz, C.Volpe Role of Anharmonicities and Nonlinearities in Heavy Ion Collisions a Microscopic Approach NUCLEAR REACTIONS 208Pb, 40Ca(208Pb, 208Pb'), E=0.641, 1 GeV/nucleon; calculated Coulomb excitation σ vs excitation energy, relativistic energies. Microscopic approach beyond RPA, anharmonicities, nonlinearities. NUCLEAR STRUCTURE 40Ca, 208Pb; calculated 1- giant resonances; deduced anharmonicities, nonlinearities role. Microscopic approach beyond RPA.
doi: 10.1016/S0375-9474(96)00444-7
1996CA21 Nucl.Phys. A602, 181 (1996) F.Catara, C.H.Dasso, A.Vitturi Low-Lying Component in Strength Distributions of Weakly Bound Neutron-Rich Nuclei
doi: 10.1016/0375-9474(96)00112-1
1996VO08 Nucl.Phys. A599, 347c (1996) C.Volpe, Ph.Chomaz, M.V.Andres, F.Catara, E.G.Lanza Are Giant Resonances Harmonic Vibrations ( Question ) NUCLEAR REACTIONS 208Pb(136Xe, 136Xe'), E=700 MeV/nucleon; calculated one-, two-phonon states excitation in projectile by Coulomb excitation; deduced small anharmonicities, nonlinearities role.
doi: 10.1016/0375-9474(96)00077-2
1995BA60 Yad.Fiz. 58, No 4, 604 (1995); Phys.Atomic Nuclei 58, 548 (1995) E.B.Balbutsev, A.V.Unzhakova, M.V.Andres, F.Catara, E.G.Lanza Role of Low-Lying Isoscalar Dipole Modes in the Polarization Potential NUCLEAR REACTIONS 208Pb(208Pb, 208Pb'), E=2-8 GeV; calculated GDR, GQR other multipolarities contribution to real, imaginary part of local polarization potential. Wigner function moments method.
1995SA26 Phys.Rev. C51, 3066 (1995) Extended Random-Phase Approximation in a Boson Formalism with Pauli Principle
doi: 10.1103/PhysRevC.51.3066
1995VO04 Nucl.Phys. A589, 521 (1995) C.Volpe, F.Catara, Ph.Chomaz, M.V.Andres, E.G.Lanza Anharmonicities and Non-Linearities in the Excitation of Double Giant Resonances NUCLEAR REACTIONS 208Pb(136Xe, X), E=700 MeV/nucleon; analyzed data; deduced anharmonicities, nonlinearities role in GDR excitation. Quantum anharmonic oscillator.
doi: 10.1016/0375-9474(95)00195-7
1994CA28 Nucl.Phys. A579, 1 (1994) F.Catara, N.Dinh Dang, M.Sambataro Ground-State Correlations Beyond RPA NUCLEAR STRUCTURE 208Pb, 146Gd; calculated levels, B(λ), EWSR. Ground state correlations beyond RPA.
doi: 10.1016/0375-9474(94)90790-0
1994KA33 J.Phys.(London) G20, 1431 (1994) D.Karadjov, V.V.Voronov, F.Catara Effect of Ground State Correlations on the Charge Transition Densities of Vibrational States NUCLEAR STRUCTURE 64,66,68,70Zn; calculated transition charge density. Ground state correlations beyond RPA.
doi: 10.1088/0954-3899/20/9/012
1993AN01 Phys.Rev. C47, 902 (1993) M.V.Andres, F.Catara, E.G.Lanza Reply to ' Comment on ' Dynamical Polarization Potential Due to the Excitation of Collective States ' ' NUCLEAR REACTIONS 40Ca(16O, 16O), E < 600 MeV; calculated dynamical polarization potential parameters vs E; deduced form factors role.
doi: 10.1103/PhysRevC.47.902
1993KA14 Phys.Lett. 306B, 197 (1993) D.Karadzhov, V.V.Voronov, F.Catara Ground State Correlations and Charge Transition Densities NUCLEAR STRUCTURE 64Zn; calculated ground state quasiparticle distribution, transition charge density; deduced ground state correlations features.
doi: 10.1016/0370-2693(93)90067-R
1992CA06 Phys.Lett. 277B, 1 (1992) F.Catara, Ph.Chomaz, N.Van Giai Electromagnetic Decay of Two-Phonon States NUCLEAR STRUCTURE 40Ca; calculated dipole, quadrupole state energies, transition rates, EWSR percentages. Boson expansion approach, RPA. NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E=50 MeV/nucleon; calculated one-, two-phonon states excitation probability, GDR, GQR excitations. Boson expansion approach, RPA.
doi: 10.1016/0370-2693(92)90946-2
1992CA22 Phys.Rev. C46, 754 (1992) Quark Distributions in Nuclei NUCLEAR STRUCTURE 4He, 16O, 40Ca; calculated quark distribution; deduced short range correlations role in quark density.
doi: 10.1103/PhysRevC.46.754
1991AN20 Phys.Rev. C44, 2709 (1991) M.V.Andres, F.Catara, E.G.Lanza Dynamical Polarization Potential Due to the Excitation of Collective States NUCLEAR REACTIONS 40Ca(16O, 16O), E=104 MeV; 40Ca(40Ca, 40Ca), E=143 MeV; calculated σ(θ); deduced potential parameters energy dependence. Dynamical polarization potential, Feshbach formalism.
doi: 10.1103/PhysRevC.44.2709
1991GA25 Europhys.Lett. 16, 711 (1991) Y.Y.Gao, F.Catara, M.Sambataro, A.Vitturi Study of Negative-Parity States in Near-Closed-Shell Nuclei in the Collective-Pair Approximation Including Particle-Hole Excitations NUCLEAR STRUCTURE 18O; calculated levels; deduced (particle-particle)-, (particle-hole)- degrees of freedom role in octupole states. Collective pair approximation.
1989AN01 Phys.Rev. C39, 99 (1989) M.V.Andres, F.Catara, Ph.Chomaz, E.G.Lanza Random-Phase-Approximation-Based Dynamical Polarization Potential NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E(cm)=55.45-888 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.39.99
1989CA09 Nucl.Phys. A494, 301 (1989) F.Catara, M.Di Toro, A.Ferriolo Dynamical Deformations in Nucleon Momentum Distributions of Colliding Ions NUCLEAR REACTIONS 40Ca(40Ca, X), E=10-40 MeV/nucleon; calculated average phonon excitation number vs time, nucleon momentum distribution; deduced dynamical distortions enhancement.
doi: 10.1016/0375-9474(89)90025-0
1989CA10 Nucl.Phys. A495, 115c (1989) Dynamical Polarization Effects in Heavy Ion Collisions NUCLEAR REACTIONS 40Ca(40Ca, 40Ca), E(cm)=800 meV; calculated σ(θ); deduced model parameters. RPA, collective vibrational modes.
doi: 10.1016/0375-9474(89)90312-6
1989CA16 J.Phys.(London) G15, L191 (1989) F.Catara, C.H.Dasso, A.Vitturi Test for Static Octupole Deformations in the Actinide Region through Subbarrier Fusion Processes NUCLEAR REACTIONS, ICPND 144Ba(16O, X), E(cm)=45-65 MeV; 224Ra(16O, X), E(cm)=70-90 MeV; calculated fusion σ(E). 218,220,222,224,226,228,230Ra(16O, X), E(cm)=72 MeV; calculated fusion σ enhancement factor; deduced octupole deformations role.
doi: 10.1088/0954-3899/15/9/003
1989CA27 Phys.Lett. 233B, 6 (1989) F.Catara, Ph.Chomaz, N.Van Giai High-Lying Two-Phonon States in 40Ca NUCLEAR STRUCTURE 40Ca; calculated two-phonon spectra. RPA, boson expansion.
doi: 10.1016/0370-2693(89)90606-0
1989CH29 Europhys.Lett. 9, 125 (1989) Ph.Chomaz, Y.Blumenfeld, M.V.Andres, F.Catara, E.G.Lanza Importance of Giant-Resonance Excitation for the Surface Properties of the Heavy-Ion Optical Potential NUCLEAR STRUCTURE 40Ca, 90Zr, 208Pb; calculated response functions. RPA. NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(40Ca, 40Ca), E=33 MeV/nucleon; calculated transmission factor vs l. RPA based heavy-ion potential.
doi: 10.1209/0295-5075/9/2/006
1988AN12 J.Phys.(London) G14, 1331 (1988) M.V.Andres, F.Catara, Ph.Chomaz, E.G.Lanza Polarisation Potential and Sub-Barrier Fusion in a Multiphonon Excitation Model NUCLEAR REACTIONS, ICPND 40Ca(40Ca, X), E(cm) ≈ 50-70 MeV; 48Ca(40Ca, X), E(cm)=48-68 MeV; calculated fusion σ(E). Adiabatic polarization potential.
doi: 10.1088/0305-4616/14/10/009
1988LO05 Europhys.Lett. 6, 125 (1988) P.Lotti, E.Maglione, F.Catara, A.Insolia Surface Clustering and Two-Nucleon Pick-Up in Samarium Isotopes NUCLEAR STRUCTURE 148,156Sm; calculated two-neutron pickup form factors.
doi: 10.1209/0295-5075/6/2/006
1987CA22 Nucl.Phys. A471, 661 (1987) F.Catara, Ph.Chomaz, A.Vitturi Heavy-Ion Inelastic Scattering in a Multiphonon Excitation Model NUCLEAR REACTIONS 40Ca(40Ca, 40Ca'), E=10-44 MeV/nucleon; calculated σ(θ(40Ca), E(40Ca)). Multi-phonon excitation model.
doi: 10.1016/0375-9474(87)90105-9
1986CA02 Nucl.Phys. A451, 299 (1986) Interplay between Particle-Hole Excitation and Nucleon Transfer in Deep-Inelastic Collisions NUCLEAR REACTIONS 197Au(58Ni, X), 209Bi(56Fe, X), E not given; calculated projectile-like fragment neutron, proton average shifts, relative distance vs time; deduced particle-hole excitation, nucleon transfer interplay. Independent particle model, deep inelastic collisions.
doi: 10.1016/0375-9474(86)90416-1
1986CA12 Nucl.Phys. A455, 158 (1986) Non-Linear Effects and Multiphonon Excitations in Grazing Collisions NUCLEAR REACTIONS 40Ca(40Ca, 40Ca'), E=30 MeV/nucleon; calculated elementary mode coupling induced nonlinear effects; deduced target GQR multiple excitations role. Semi-classical description.
doi: 10.1016/0375-9474(86)90349-0
1985TA12 Nucl.Phys. A442, 369 (1985) Polarization Effects in Nucleus-Nucleus Collisions (II). Elastic and Inelastic Cross Sections NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=25 MeV; calculated σ(θ); deduced polarization effects role. Coupled-channels, perturbed stationary state approach.
doi: 10.1016/0375-9474(85)90150-2
1984CA04 Phys.Rev. C29, 1091 (1984) F.Catara, A.Insolia, E.Maglione, A.Vitturi Relation between Pairing Correlations and Two-Particle Space Correlations NUCLEAR STRUCTURE 206Pb; calculated level wave function radial probability distributions. Pairing, two-particle space correlations.
doi: 10.1103/PhysRevC.29.1091
1984CA12 Phys.Rev. C29, 1916 (1984) F.Catara, A.Insolia, E.Maglione, A.Vitturi Description of the Even Samarium Isotopes in the Collective Pair Approximation NUCLEAR STRUCTURE 146,148,150,152,154Sm; calculated ground state characteristics, neutron, proton effective gaps, collective pair microscopic structure, emptiness factors, β2, diffusivity. Collective pair approximation.
doi: 10.1103/PhysRevC.29.1916
1984CA21 Nucl.Phys. A424, 184 (1984) F.Catara, A.Insolia, E.Maglione, A.Vitturi, R.A.Broglia Comparative Study of the Selectivity Displayed by (6Li, d) and (16O, 12C) Reactions NUCLEAR REACTIONS 56Fe(6Li, d), E=34 MeV; 54Fe(16O, 12C), E=50 MeV; calculated σ(θ). 58,60Ni deduced selective 0+ state population. DWBA, finite-range form factors.
doi: 10.1016/0375-9474(84)90134-9
1984CA28 Nucl.Phys. A427, 568 (1984) Polarization Effects in Nucleus-Nucleus Collisions (I). Distortion of Nuclear Intrinsic States NUCLEAR REACTIONS 12C(12C, 12C'), E not given; calculated folding potential parameters, equal density contour plots, B(E2) vs inter-ion distance. Polarization effects, rotating frame.
doi: 10.1016/0375-9474(84)90231-8
1984CA36 Phys.Lett. 149B, 41 (1984) F.Catara, A.Insolia, E.Maglione, A.Vitturi Two-and Four-Particle Surface Clusterization in Heavy Deformed Nuclei NUCLEAR STRUCTURE 232Th; calculated α, di-nucleon cluster probability distribution. Pairing correlation, Nilsson basis.
doi: 10.1016/0370-2693(84)91547-8
1983BA18 Lett.Nuovo Cim. 36, 359 (1983) M.Baldo, F.Catara, E.G.Lanza, U.Lombardo, L.Lo Monaco Pairing Correlation Effects on the Mass Transfer in Deep Inelastic Collisions between Heavy Ions NUCLEAR REACTIONS 40Ca(40Ca, X), (42Ca, X), (44Ca, X), (46Ca, X), (48Ca, X), 42Ca(42Ca, X), 44Ca(44Ca, X), 46Ca(46Ca, X), 48Ca(48Ca, X), E=6.4 MeV/nucleon; calculated transferred nucleon average number, width. Deep inelastic collisions, mass transfer, pairing correlation.
doi: 10.1007/BF02747126
1983CA16 Nucl.Phys. A404, 167 (1983) F.Catara, L.Ferreira, A.Insolia, E.Maglione, A.Vitturi, R.A.Broglia Value of the Absolute Cross Section for the Reaction 40Ca(16O, 12C)44Ti NUCLEAR REACTIONS 40Ca(16O, 12C), E=42 MeV; calculated absolute σ(θ). Finite-range DWBA, recoil effects, transfer connected state shell model description.
doi: 10.1016/0375-9474(83)90420-7
1982BA71 Nucl.Phys. A391, 249 (1982) M.Baldo, F.Catara, E.G.Lanza, U.Lombardo, L.Lo Monaco Independent Particle Description of Mass and Charge Transfer in Deep Inelastic Collisions NUCLEAR REACTIONS 48Ca(40Ca, X), E(cm)=128, 150 MeV; 209Bi(84Kr, X), E=714 MeV; calculated mean transferred nucleon number vs interaction time. Classical approach, time-dependent single-particle model.
doi: 10.1016/0375-9474(82)90231-7
1981CA15 Nucl.Phys. A372, 237 (1981) F.Catara, L.Ferreira, A.Insolia, A.Vitturi, R.A.Broglia Probing the Pairing Vibrational Modes of the Zr Isotopes in Two- and Four-Nucleon Transfer Reactions NUCLEAR STRUCTURE 90,92,94,96Zr, 94,96,98,100Mo; calculated levels, wave functions. Pairing vibrational model. NUCLEAR REACTIONS 90,92,94Zr(t, p), 94,96,98,100Mo(d, 6Li), 94,92Mo(6Li, 8B), E not given; calculated σ(relative), two-nucleon transfer spectroscopic amplitudes, four-particle transfer form factors. DWBA, pairing vibrational model.
doi: 10.1016/0375-9474(81)90099-3
1981IN02 Z.Phys. A301, 209 (1981) A.Insolia, M.Baldo, F.Catara, A.Vitturi Microscopic Analysis of the 12C(6Li, d)16O Reaction NUCLEAR REACTIONS 12C(6Li, d), E=28, 34 MeV; analyzed σ(θ). Zero-range DWBA, microscopic four-nucleon transfer.
doi: 10.1007/BF01416295
1980CA26 Nuovo Cim. 60A, 98 (1980) F.Catara, M.Consoli, A.Insolia, L.Lo Monaco π-Nucleus Elastic Scattering around the Δ(3, 3) Resonance NUCLEAR REACTIONS 12C(π, π), E=150-280 MeV; calculated σ(θ). Microscopic pion-nucleus optical model, isobar degrees of freedom.
doi: 10.1007/BF02776558
1979CA06 Nucl.Phys. A320, 373 (1979) A Selfconsistent Description of 6Li in Terms of Four-Body and Two-Body Substructures NUCLEAR STRUCTURE 6Li; calculated gs energy, elastic electron scattering form factors. Microscopic shell model with 2p-2n, 1p-1n substuctures, bare nucleon-nucleon interaction.
doi: 10.1016/0375-9474(79)90195-7
1977CA02 Nucl.Phys. A276, 433 (1977) F.Catara, M.Consoli, A.Insolia, L.Pappalardo, S.Pappalardo An Approach to the Nuclear Many-Body Problem Including Virtual Mesons (I). HF Approximation in Finite Nuclei NUCLEAR STRUCTURE 12C, 16O; calculated single-nucleon self-energy. Hartree-Fock approximation.
doi: 10.1016/0375-9474(77)90537-1
1976CA08 Nucl.Phys. A261, 282 (1976) F.Catara, A.Insolia, U.Lombardo Pairing and Quartering Correlations in Nuclei NUCLEAR STRUCTURE 44,46,48,50Ti, 48,50,52Cr, 52,54Fe, 56Ni; calculated quasi-hole energies.
doi: 10.1016/0375-9474(76)90571-6
1973CA32 Nucl.Phys. A215, 85 (1973) A Variational Determination of Few-Nucleon Substructures in Nuclei NUCLEAR STRUCTURE 20Ne, 24Mg; calculated levels, J, π, level-width.
doi: 10.1016/0375-9474(73)90103-6
1972AG02 Nucl.Phys. A184, 458 (1972) A.Agodi, M.Baldo, F.Catara, M.Di Toro, R.Parisi An Approach to Nuclear Theory Including Shell-Model Conditions and Particle Correlations NUCLEAR REACTIONS 15N(n, n), (n, n'), 16O(γ, n), calculated σ(E), scattering amplitudes; deduced correlation effects.
doi: 10.1016/0375-9474(72)90421-6
1971AG02 Nucl.Phys. A171, 199 (1971) An Approach to Nuclear Theory Including 'Shell-Model' Conditions and Particle Correlations NUCLEAR STRUCTURE 16O; calculated p-H states. Correlated, uncorrelated ground state wave functions.
doi: 10.1016/0375-9474(71)90371-X
1968CA08 Nucl.Phys. A111, 577 (1968) Electric Levels and Transition Rates in 12C, 16O and 28Si NUCLEAR STRUCTURE 16O, 28Si, 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(68)90241-8
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