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NSR database version of April 11, 2024.

Search: Author = G.Fortuna

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0418.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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