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NSR database version of May 23, 2024.

Search: Author = R.Fonte

Found 19 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1230.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1991FO05      Phys.Rev. C44, 543 (1991)

R.Fonte, A.Insolia

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1985FO04      Lett.Nuovo Cim. 42, 17 (1985)

R.Fonte, A.Insolia

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
Citations: PlumX Metrics


1984FO20      Lett.Nuovo Cim. 40, 519 (1984)

R.Fonte, A.Insolia

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
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1984FO21      Phys.Lett. 148B, 257 (1984)

R.Fonte, A.Insolia

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
Citations: PlumX Metrics


1983FO03      Lett.Nuovo Cim. 38, 237 (1983)

R.Fonte

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1982FO07      Lett.Nuovo Cim. 34, 26 (1982)

R.Fonte, A.Insolia

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1980FO13      Phys.Lett. B96, 265 (1980)

R.Fonte, H.Oeschler

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
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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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