NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = R.Fonte Found 19 matches. 2001LA07 Nucl.Phys. A683, 566 (2001) G.Lanzano, E.De Filippo, M.Geraci, A.Pagano, S.Aiello, A.Cunsolo, R.Fonte, A.Foti, M.L.Sperduto, C.Volant, J.L.Charvet, R.Dayras, R.Legrain Light Charged Particle and Neutron Velocity Spectra in Coincidence with Projectile Fragments in the Reaction 40Ar(44 A MeV) + 27Al NUCLEAR REACTIONS 27Al(40Ar, X), E=44 MeV/nucleon; measured fragments charge distributions, light particle spectra, angular distribution, (particle)(fragment)-coin; deduced particle source features. Three-source analysis.
doi: 10.1016/S0375-9474(00)00447-4
1996KN01 Phys.Rev. C53, 347 (1996) C.N.Knott, S.Albergo, Z.Caccia, C.-X.Chen, S.Costa, H.J.Crawford, M.Cronqvist, J.Engelage, P.Ferrando, R.Fonte, L.Greiner, T.G.Guzik, A.Insolia, F.C.Jones, P.J.Lindstrom, J.W.Mitchell, R.Potenza, J.Romanski, G.V.Russo, A.Soutoul, O.Testard, C.E.Tull, C.Tuve, C.J.Waddington, W.R.Webber, J.P.Wefel, and the Transport Collaboration Interactions of Relativistic Neon to Nickel Projectiles in Hydrogen, Elemental Production Cross Sections NUCLEAR REACTIONS 1H(22Ne, X), (26Mg, X), (32S, X), (36Ar, X), (40Ar, X), (52Cr, X), (58Ni, X), (40Ca, X), E=338-894 MeV/nucleon; measured elemental production σ, relativistic collisions. Liquid hydrogen target.
doi: 10.1103/PhysRevC.53.347
1994CH21 Phys.Rev. C49, 3200 (1994) C.-X.Chen, S.Albergo, Z.Caccia, S.Costa, H.J.Crawford, M.Cronqvist, J.Engelage, P.Ferrando, R.Fonte, L.Grenier, T.G.Guzik, A.Insolia, F.C.Jones, C.N.Knott, P.J.Lindstrom, J.W.Mitchell, R.Potenza, J.Romanski, G.V.Russo, A.Soutoul, O.Testard, C.E.Tull, C.Tuve, J.C.Waddington, W.R.Webber, J.P.Wefel, X.Zhang Interactions in Hydrogen of Relativistic Neon to Nickel Projectiles: Total charge-changing cross sections NUCLEAR REACTIONS 1H(22Ne, X), (26Mg, X), (32S, X), (36Ar, X), (40Ar, X), (40Ca, X), (52Cr, X), (58Ni, X), E=400-900 MeV/nucleon; measured σ vs E, mass; deduced optical model parameters. Liquid hydrogen target.
doi: 10.1103/PhysRevC.49.3200
1994DE21 Nuovo Cim. 107A, 775 (1994) E.De Filippo, R.Fonte, G.Lanzano, A.Pagano The Response of a NE102A-BaF2 Phoswich Detector to Low-Energy Heavy Ions NUCLEAR REACTIONS 12C(16O, X), E=80 MeV; measured fragment tof spectra; deduced detector response characteristics. NE102A-BaF2 phoswich detector.
doi: 10.1007/BF02732085
1991FO05 Phys.Rev. C44, 543 (1991) Critical Energy Deposit in Heavy Ion Complete Fusion NUCLEAR REACTIONS 28Si(28Si, X), E(cm) ≤ 300 MeV; analyzed data. l-window model.
doi: 10.1103/PhysRevC.44.543
1990PA14 Phys.Lett. 240B, 317 (1990) N.H.Papadakis, N.P.Vodinas, Y.Cassagnou, R.Dayras, R.Fonte, G.Imme, R.Legrain, A.D.Panagiotou, E.G.Pollacco, G.Raciti, L.Rodriguez, F.Saint-Laurent, M.G.Saint-Laurent, N.Saunier Global Features of Intermediate Mass Fragment Cross Sections in Ne Induced Interactions NUCLEAR REACTIONS 197Au, Ag(20Ne, X), E=20-60 MeV/nucleon; measured fragment production σ vs E. Fragmentation model.
doi: 10.1016/0370-2693(90)91105-K
1989BE25 Z.Phys. A333, 393 (1989) V.Bellini, M.Bolore, J.Julien, J.M.Hisleur, A.Fallica, A.S.Figuera, R.Fonte, A.Insolia, C.Milone, G.F.Palama, G.V.Russo, M.L.Sperduto, L.Bimbot Inclusive (p, π0) Reactions at E(lab) = 200 MeV NUCLEAR REACTIONS C, 27Al, Ni, 89Y, 118,124Sn, Pb, U(p, π0X), E=200 MeV; measured inclusive pion production σ; deduced target mass dependence.
1989FO07 Nucl.Phys. A495, 43c (1989) R.Fonte, A.Insolia, G.Palama, G.V.Russo π0 Production in Heavy Ion Collisions NUCLEAR REACTIONS 27Al, 197Au(20Ne, π0X), E=200 MeV/nucleon; 27Al, 197Au(16O, π0X), E=38 MeV/nucleon; measured inclusive σ(θ).
doi: 10.1016/0375-9474(89)90305-9
1988JU02 Z.Phys. A330, 83 (1988) J.Julien, M.Bolore, H.Dabrowski, J.M.Hisleur, V.Bellini, A.S.Figuera, R.Fonte, A.Insolia, G.F.Palama, G.V.Russo, M.L.Sperduto, J.Chauvin, P.De Saintignon, D.Lebrun, D.Rebreyend Neutral Pion Production in Subthreshold Heavy Ion Collision with 16O(38 MeV/u) and 20Ne(200 MeV/u) Beams NUCLEAR REACTIONS 27Al, 197Au(16O, π0X), E=38 MeV/nucleon; 27Al(20Ne, π0X), E=200 MeV/nucleon; measured σ(θ(π)), integrated σ vs E(π).
1988NO09 Nucl.Phys. A489, 763 (1988) B.Noren, B.Jakobsson, A.Kristiansson, L.Karlsson, A.Oskarsson, M.Westenius, J.Julien, V.Bellini, R.Fonte, T.Johansson, J.Thun, C.Guet Charge Pion Production and Projectile Breakup in 85A MeV 12C-Induced Heavy-Ion Reactions NUCLEAR REACTIONS 12C, 116,124Sn(12C, π+X), (12C, π-X), E=85 MeV/nucleon; measured σ(E(π), fragment Z).
doi: 10.1016/0375-9474(88)90120-0
1985FO04 Lett.Nuovo Cim. 42, 17 (1985) Lower-l Cut-Off in Heavy-Ion Fusion Process NUCLEAR REACTIONS, ICPND 12C, 16O, 32S(27Al, X), E(cm) ≈ 50-200 MeV; 18O(12C, X), 26Mg(16O, X), E(cm) ≈ 25-100 MeV; 24Mg(32S, X), 62Ni(35Cl, X), 28Si(28Si, X), 35Cl(27Al, X), E(cm) ≈ 50-150 MeV; 208Pb(27Al, X), (26Mg, X), E(cm) ≈ 100-200 MeV; 12C(12C, X), E(cm) ≈ 10-75 MeV; 16O(16O, X), E(cm) ≈ 10-100 MeV; 116Sn(35Cl, X), E(cm) ≈ 100-200 MeV; 208Pb(48Ca, X), E(cm)=175-250 MeV; calculated fusion σ(E); deduced fusion l-window.
doi: 10.1007/BF02739470
1984FO20 Lett.Nuovo Cim. 40, 519 (1984) Influence of the Impact Parameter on the Heavy-Ion Fusion Process NUCLEAR REACTIONS 118Sn(40Ar, xn), 74Ge(84Kr, xn), E(cm) ≈ 270-330 MeV; calculated fusion σ/reaction σ vs excitation energy; deduced fusion L-window interpretation.
doi: 10.1007/BF02749383
1984FO21 Phys.Lett. 148B, 257 (1984) 1-Window Model for Complete Fusion NUCLEAR REACTIONS, ICPND 27Al(12C, X), (16O, X), (32S, X), E(cm) ≈ 25-175 MeV; 116Sn(35Cl, X), E(cm)=150-300 MeV; 62Ni(35Cl, X), E(cm)=102-302 MeV; calculated fusion σ(E). L-window model.
doi: 10.1016/0370-2693(84)90083-2
1983FO03 Lett.Nuovo Cim. 38, 237 (1983) Anomalous Behaviour of Tritons from 156 MeV 6Li Break-Up Reaction NUCLEAR REACTIONS 40Ca(6Li, t), E=156 MeV; calculated σ(Et) following 6Li breakup; deduced second step (3He, t) contribution. DWBA, breakup model.
doi: 10.1007/BF02814635
1983OE02 Phys.Rev. C27, 1677 (1983) H.Oeschler, Y.Cassagnou, R.Fonte, R.Legrain Q-value Systematics Applied to the Absorption of Mesons on Complex Nuclei NUCLEAR REACTIONS 60Ni(π+, X), (π-, X), E=60, 70, 220 MeV; 58Ni, 63Cu(K-, X), E at rest; analyzed yields vs (Q) for 54,55,56Fe, 53,54,55,56Mn, 50,51,52,53Cr, 46,48Ti; deduced nuclear temperatures, reaction mechanism. Binary separation, fragmentation model.
doi: 10.1103/PhysRevC.27.1677
1982FO07 Lett.Nuovo Cim. 34, 26 (1982) Level Density Limitation to Fusion NUCLEAR REACTIONS, ICPND 12,13C, 14,15N, 16,18O, 19F, 27Al(12C, X), 16O, 24,26Mg, 27Al, 40Ca(16O, X), 28Si(18O, X), 32S(24Mg, X), (27Al, X), 28Si(28Si, X), E not given; calculated fusion σ; deduced reaction independent nuclear temperature, fusion level density limitation.
doi: 10.1007/BF02817146
1981JU01 Phys.Rev. C23, 448 (1981) J.Julien, R.Letourneau, L.Roussel, R.Legrain, Y.Cassagnou, R.Fonte, A.Palmeri Coincidences between Neutrons and γ-Rays Emitted by Pions Stopped in 28Si NUCLEAR REACTIONS 28Si(π-, n), E at rest; 28Si(π+, p), E=70 MeV; measured nγ-, pγ-, n(X-ray)-coin; deduced σ(En), σ(Ep). 25,26Al, 26,25,24Mg, 23Na, 20,21,22Ne deduced neutron, proton multiplicities. Quasideuteron pion absorption model.
doi: 10.1103/PhysRevC.23.448
1980FO13 Phys.Lett. B96, 265 (1980) An Optimal Velocity for the Fusion between Heavy Ions NUCLEAR REACTIONS 27Al(35Cl, X), E=70-170 MeV; 26Mg(16O, X), E=30-81 MeV; 16O(16O, X), E=35-80 MeV, E(cm)=14.9-36 MeV; 19F(12C, X), E(cm)=11.6-27.1 MeV; 18O(12C, X), E(cm)=11.9-28 MeV; 16O(12C, X), E(cm)=12.9-27 MeV; 15N(12C, X), E(cm)=8.9-26.7 MeV, E=22-60 MeV; 14N(12C, X), E=27-60 MeV, 43-178 MeV; 13C(12C, X), E(cm)=7.6-24.9 MeV; 12C(12C, X), E=7.4-31.2 MeV; analyzed σ(fusion) data; deduced heavy ion fusion optimal velocity.
doi: 10.1016/0370-2693(80)90763-7
1978CA13 Lett.Nuovo Cim. 22, 536 (1978) G.Calvi, S.Cavallaro, A.S.Figuera, R.Fonte, C.Milone Some Measurements on Neutron Polarization from 3H(d, n)4He at E = 700 keV NUCLEAR REACTIONS 3H(d, n), E=700 keV; measured σ(En, θ), polarization.
doi: 10.1007/BF02789523
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