NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = G.Fortuna Found 25 matches. 2009BL05 Int.J.Mod.Phys. E18, 1960 (2009) Y.Blumenfeld, P.Butler, J.Cornell, G.Fortuna, M.Lindroos EURISOL design study: towards an ultimate ISOL facility for Europe
doi: 10.1142/S0218301309014081
2002TE05 Nucl.Phys. A701, 67c (2002) L.B.Tecchio, A.Andrighetto, R.Cherubini, P.Colautti, M.Comunian, L.Corradi, A.Dainelli, G.De Angelis, M.De Poli, A.Facco, E.Fioretto, G.Fortuna, G.Jiyu, R.Ming, G.Montagnoli, G.Moschini, A.Pisent, M.Poggi, A.M.Porcellato, D.Zafiropoulos, P.Bak, N.Kot, P.Logatchev, S.Shyankov, F.Brandolini, G.Moschini, C.Signorini, T.Clauser, G.Lamanna, V.Stagno, V.Variale Project of an Advanced ISOL Facility for Exotic Beams at LNL
doi: 10.1016/S0375-9474(01)01550-0
1999RI14 Ann.Nucl.Energy 26, 1643 (1999) M.V.Ricciardi, L.Barone-Tonghi, G.Cuttone, G.Ciavola, G.Di Bartolo, M.Menna, G.Fortuna, S.Monti, L.Tecchio Dependence of Exotic Nuclides Production on Target and Beam Features NUCLEAR REACTIONS 94Zr(p, X), E=1 GeV; 238U(p, F), E=40, 1000 MeV; calculated Rb yields. U(p, F), E=100 MeV; calculated As, Kr, Rb yields vs target thickness. U(p, F), E=60 MeV; calculated Zn, Rb, Cd, Sn, Cs isotopic yields. Hadronic transport Monte Carlo calculations.
doi: 10.1016/S0306-4549(99)00045-6
1989DE20 Phys.Rev. C40, 627 (1989) A.De Rosa, G.Inglima, E.Rosato, M.Sandoli, G.Cardella, M.Papa, G.Pappalardo, F.Rizzo, G.Fortuna, G.Montagnoli, A.M.Stefanini, A.Tivelli, C.Signorini Angular Momentum Role in Cross-Section Energy Coherence of Heavy-Ion Dissipative Collisions NUCLEAR REACTIONS 63Cu(19F, X), E=100-108 MeV; measured σ(θ) vs E for fragment Z=5-11; deduced coherence widths. Other data analyzed.
doi: 10.1103/PhysRevC.40.627
1988CA27 Nucl.Phys. A482, 235c (1988) G.Cardella, M.Papa, G.Pappalardo, F.Rizzo, A.De Rosa, G.Inglima, M.Sandoli, G.Fortuna, G.Montagnoli, A.M.Stefanini, A.Tivelli, S.Beghini, C.Signorini Experimental Indications of Selective Excitations in Dissipative Heavy Ion Collisions NUCLEAR REACTIONS 64Ni, 48Ti(28Si, X), E=120-127 MeV; measured σ(θ) vs E; deduced fluctuations role.
doi: 10.1016/0375-9474(88)90587-8
1988DE06 Phys.Rev. C37, 1042 (1988) A.De Rosa, G.Inglima, M.Romano, V.Russo, M.Sandoli, G.Cardella, G.Pappalardo, F.Rizzo, G.Fortuna, A.M.Stefanini, S.Beghini, G.Montagnoli, C.Signorini Interaction Time Evaluation in Dissipative Heavy Ion Reactions NUCLEAR REACTIONS 48Ti(28Si, X), E=120-127 MeV; measured σ(fragment θ) vs E; deduced interaction time features.
doi: 10.1103/PhysRevC.37.1042
1988SO06 Phys.Rev. C38, 537 (1988) F.Soramel, S.Lunardi, S.Beghini, M.Morando, C.Signorini, W.Meczynski, G.Fortuna, G.Montagnoli, A.M.Stefanini Nucleus 136Sm and the Transition to a Deformed Regime at N = 76-74 NUCLEAR REACTIONS 107Ag(32S, 2np), E=125-150 MeV; measured Eγ, T1/2, γγ-coin. 136Sm deduced levels, J, π, B(E2), deformation parameters.
doi: 10.1103/PhysRevC.38.537
1988ST02 Phys.Lett. 200B, 419 (1988) W.Starzecki, G.de Angelis, B.Rubio, J.Styczen, K.Zuber, H.Guven, W.Urban, W.Gast, P.Kleinheinz, S.Lunardi, F.Soramel, A.Facco, C.Signorini, M.Morando, W.Meczynski, A.M.Stefanini, G.Fortuna Prolate and Oblate 10+ Isomers in 140Sm78 and 142Gd78 NUCLEAR REACTIONS 142Nd(α, 6n), E=95 MeV; 110Cd(35Cl, 2np), E=148 MeV; measured Eγ, Iγ, γγ-coin, T1/2. 140Sm, 142Gd deduced levels, J, π, B(E2).
doi: 10.1016/0370-2693(88)90145-1
1987LU06 Z.Phys. A328, 487 (1987) S.Lunardi, P.J.Daly, F.Soramel, C.Signorini, B.Fornal, G.Fortuna, A.M.Stefanini, R.Broda, W.Meczynski, J.Blomqvist Decay of (νh11/2(n))(+10)+ and (πd5/2νh11/2(n))(25/2)+ Isomers in Even-A Sn and Odd-A Sb Nuclei NUCLEAR REACTIONS 116Cd(7Li, X), E=26-40 MeV; measured Eγ, Iγ. 120Sn deduced isomer T1/2, configuration, B(E2), decay characteristics. 116,118Sn, 119,120Sb deduced isomer decay characteristics, configuration.
1987SK07 Z.Phys. A328, 355 (1987) S.J.Skorka, A.M.Stefanini, G.Fortuna, R.Pengo, W.Meczynski, G.Montagnoli, A.Tivelli, S.Beghini, C.Signorini, P.R.Pascholati Sub-barrier fusion of 35,37Cl + 58,64Ni evidence of effects of proton transfer channels NUCLEAR REACTIONS, ICPND 58,64Ni(35Cl, X), (37Cl, X), E ≈ 57-70 MeV; measured fusion σ(E). Enriched targets.
doi: 10.1007/bf01290504
1987ST06 Phys.Lett. 185B, 15 (1987) A.M.Stefanini, G.Montagnoli, G.Fortuna, R.Menegazzo, S.Beghini, C.Signorini, A.DeRosa, G.Inglima, M.Sandoli, F.Rizzo, G.Pappalardo, G.Cardella Neutron and Proton Transfer in 32,36S + 58,64Ni around the Coulomb Barrier NUCLEAR REACTIONS, ICPND 58,64Ni(32S, 32S), (32S, 32S'), (36S, 36S), (36S, 36S'), E=94-112 MeV; measured σ(θ), transfer σ; calculated inelastic, reaction σ, fusion σ(E). Enriched targets, tof ΔE-E telescope. Coupled-channels, DWBA calculations.
doi: 10.1016/0370-2693(87)91520-6
1987ST27 Phys.Rev.Lett. 59, 2852 (1987) A.M.Stefanini, D.Bonamini, A.Tivelli, G.Montagnoli, G.Fortuna, Y.Nagashima, S.Beghini, C.Signorini, A.DeRosa, G.Inglima, M.Sandoli, G.Cardella, F.Rizzo Strong Energy Dependence of the Optical Potential for 32S + 58,64Ni near the Coulomb Barrier NUCLEAR REACTIONS 58,64Ni(32S, 32S), E=82-150 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1103/PhysRevLett.59.2852
1987TI04 Fizika(Zagreb) 19, Supplement 1, 39 (1987) A.Tivelli, A.M.Stefanini, D.Bonamini, G.Montagnoli, G.Fortuna, Y.Nagashima, S.Beghini, C.Signorini, A.De Rosa, G.Inglima, M.Sandoli, G.Cardella, F.Rizzo, G.Pappalardo Elastic Scattering of 32S + 58,64Ni around the Coulomb Barrier NUCLEAR REACTIONS 58,64Ni(32S, 32S), E=82-150 MeV; measured σ(θ); deduced model parameters. Optical model.
1986DA05 Z.Phys. A323, 245 (1986) P.J.Daly, S.Lunardi, F.Soramel, M.Morando, C.Signorini, B.Fornal, G.Fortuna, A.M.Stefanini, W.Meczynski Transition Probabilities between ν(h(n)11/2) States in Sn Isotopes NUCLEAR REACTIONS 116Cd(7Li, 2np), E=26-40 MeV; measured Eγ, Iγ. 120Sn deduced isomer T1/2, decay characteristics, levels, γ-branching, B(E2), ICC, configuration. NUCLEAR STRUCTURE 116,118,120Sn; analyzed B(E2) data; deduced neutron number dependence.
1986ST08 Nucl.Phys. A456, 509 (1986) A.M.Stefanini, G.Fortuna, R.Pengo, W.Meczynski, G.Montagnoli, L.Corradi, A.Tivelli, S.Beghini, C.Signorini, S.Lunardi, M.Morando, F.Soramel Heavy-Ion Fusion below the Coulomb Barrier: The systems 28,30Si + 58,62,64Ni and 32,34,36S + 58,64Ni NUCLEAR REACTIONS, ICPND 58,62,64Ni(28Si, X), (30Si, X), E=68.4-94 MeV; 58,64Ni(32S, X), (34S, X), (36S, X), E=79.6-152 MeV; measured evaporation residues; deduced fusion σ(E) around, below Coulomb barrier, barrier parameters, discussed influence of coupling to inelastic, transfer channels. Enriched targets, electrostatic beam separator.
doi: 10.1016/0375-9474(86)90408-2
1985BE54 Nucl.Instrum.Methods 239, 585 (1985) S.Beghini, C.Signorini, S.Lundardi, M.Morando, G.Fortuna, A.M.Stefanini, W.Meczynski, R.Pengo An Electrostatic Beam Separator for Evaporation Residue Detection NUCLEAR REACTIONS 28Si(58Ni, X), E=194 MeV; 64Ni(28Si, X), E=84 MeV; measured fragment mass spectra. Electrostatic beam separator.
doi: 10.1016/0168-9002(85)90040-3
1985DE36 Phys.Lett. 160B, 239 (1985) A.De Rosa, G.Inglima, V.Russo, M.Sandoli, G.Fortuna, G.Montagnoli, C.Signorini, A.M.Stefanini, G.Cardella, G.Pappalardo, F.Rizzo Fluctuations in the Excitation Functions of Dissipative Heavy Ion Collisions NUCLEAR REACTIONS 60Ni(28Si, X), E=120-126.75 MeV; measured fragment production σ(θ) vs E for Z=10-16; deduced dinuclear intermediate state formation. Dissipative collisions.
doi: 10.1016/0370-2693(85)91318-8
1985LU06 Z.Phys. A321, 177 (1985) S.Lunardi, F.Scarlassara, F.Soramel, S.Beghini, M.Morando, C.Signorini, W.Meczynski, W.Starzecki, G.Fortuna, A.M.Stefanini Excited States in the Neutron Deficient Nuclei 138Sm and 139Eu NUCLEAR REACTIONS 108Pd, 109Ag, 110,112Cd(32S, xnyp), E=120-170 MeV; measured σ(E), Eγ, Iγ, γ(θ), γγ(t). 110Cd(32S, 2np), (32S, 2n2p), E=130, 143 MeV; measured γ-spectra, Doppler shift recoil distance. 138Sm, 139Eu deduced levels, J, π, γ-branching, T1/2, yrast band, B(E2).
doi: 10.1007/BF01411962
1985ST24 Phys.Lett. 162B, 66 (1985) A.M.Stefanini, G.Fortuna, R.Pengo, L.Corradi, G.Montagnoli, W.Meczynski, R.Rohe, S.Beghini, C.Signorini, S.Lunardi, F.Soramel, M.Morando Influence of Different Reaction Channels on the Subbarier Fusion of 32,36S with 58,64Ni NUCLEAR REACTIONS, ICPND 58,64Ni(32S, X), E(cm) ≈ 52-76 MeV; measured fusion σ(E); deduced barrier parameters. Coupled-channels analysis.
doi: 10.1016/0370-2693(85)91062-7
1984LU07 ATOMKI Kozlem. 26, 39 (1984) S.Lunardi, S.Beghini, M.Morando, C.Signorini, G.Fortuna, W.Meczynski, W.Starzecki, A.M.Stefanini Study of Neutron-Poor Nuclei in the Sm-Gd Region NUCLEAR REACTIONS 108Pd(32S, xn), (32S, X), 109Ag, 108,110,112Cd(32S, xnyp), E=126-170 MeV; measured γ(θ), γγ(t), σ(Eγ, E). 138,140Sm, 139Eu deduced levels, J, π, configuration.
1984ST23 Phys.Rev. C30, 2088 (1984) A.M.Stefanini, G.Fortuna, A.Tivelli, W.Meczynski, S.Beghini, C.Signorini, S.Lunardi, M.Morando Sub-Barrier Fusion of 28,30Si with 58,62,64Ni NUCLEAR REACTIONS, ICPND 58,62,64Ni(28Si, X), (30Si, X), E(cm) ≈ 47-64 MeV; measured fusion σ(E); deduced isotopic effects. Channel coupling model.
doi: 10.1103/PhysRevC.30.2088
1982CH08 Lett.Nuovo Cim. 33, 159 (1982) I.Chiodi, S.Lunardi, M.Morando, C.Signorini, G.Fortuna, W.Starzecki, A.M.Stefanini, G.Korschinek, H.Morinaga, E.Nolte, W.Schollmeier Multinucleon Transfer in the Interaction of 58Ni with 124Sn around the Coulomb Barrier NUCLEAR REACTIONS 124Sn(58Ni, X), E=249 MeV; measured σ(fragment E, mass); deduced multi-nucleon transfer, kinematic effects.
doi: 10.1007/BF02725528
1978FO09 Nucl.Phys. A299, 479 (1978) G.Fortuna, S.Lunardi, M.Morando, C.Signorini Shell Model and Collective High Spin States in Odd-A 1f7/2 Nuclei: 45,47Ti, 47,49V and 51Mn NUCLEAR REACTIONS 40Ca(14N, n2pγ), (12C, 3pγ), 50Cr(3He, npγ), 35Cl(16O, npαγ), 27Al(24Mg, npαγ), 44Ca(7Li, 3npγ), 24Mg(32S, 3pαγ), E=10-110 MeV; measured Eγ, Iγ, γ(θ), γγ(E). 45,47Ti, 47,49V, 51Mn deduced levels, J, π, δ, γ-branching. Ge(Li) detectors, enriched targets.
doi: 10.1016/0375-9474(78)90384-6
1976FO22 Nuovo Cim. 34A, 321 (1976) G.Fortuna, R.B.Huber, W.Kutschera, M.Morando, H.Morinaga, R.A.Ricci, C.Signorini High-Spin States in 48Ti and 46Ti NUCLEAR REACTIONS 44Ca(7Li, 2npγ), (7Li, 2nγ), (7Li, 3nγ), (7Li, 2nαγ), (7Li, 3npγ), E=10-35 MeV; 48Ca(3He, 3nγ), E=10-22 MeV; 27Al(24Mg, 3pγ), E=72 MeV; 40Ca(12C, 2pγ), (12C, 3pγ), (12C, n3pγ), (12C, 2pαγ), (12C, n2pγ), (12C, pαγ), (12C, npαγ), (12C, 4pγ), E=20-62 MeV; measured σ(E, Eγ), γγ-coin. 48,46Ti deduced levels, J, π.
doi: 10.1007/BF02786995
1976MO26 Phys.Lett. 64B, 140 (1976) M.Morando, A.Stranieri, G.Fortuna, C.Signorini A Kπ = 4- Rotational Band in 48V NUCLEAR REACTIONS 48Ti(p, n), E=6.15 MeV; measured γ linear polarization. 27Al(24Mg, n2pγ); measured σ(Eγ), γγ-coin. 35Cl(16O, n2pγ), E=35-80 MeV; measured σ(E, Eγ). 48V deduced levels, K, J, π.
doi: 10.1016/0370-2693(76)90314-2
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