NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = A.Fahli Found 12 matches. 2003BE75 Acta Phys.Hung.N.S. 18, 297 (2003) C.Beck, M.Rousseau, P.Papka, A.Sanchez i Zafra, C.Bhattacharya, V.Rauch, P.Bednarczyk, S.Courtin, O.Dorvaux, F.Haas, A.Nourreddine, I.Piqueras, J.Robin, L.El Bakali, C.Enaux, E.Galmar, S.Szilner, O.Stezowski, A.Prevost, S.Thummerer, W.von Oertzen, A.Hachem, E.Martin, A.Fahli, A.Morsad, A.Szanto de Toledo, S.J.Sanders Search for Cluster Emission and Extremely Deformed Shapes Using Charged-Particle Spectroscopy NUCLEAR REACTIONS 12C, 28Si(28Si, X), E=180 MeV; 12C(27Al, X), E=150 MeV; 12C(31P, X), E=112 MeV; 12C(32S, X), E=140 MeV; measured Eα, Ep, angular correlations between light charged particles and evaporation residues; deduced highly deformed configurations, cluster emission features. Other reactions discussed.
doi: 10.1556/APH.18.2003.2-4.30
2002HA05 Nucl.Instrum.Methods Phys.Res. B187, 164 (2002) A.Hakim, A.Fahli, M.Toulemonde, D.Lelievre Stopping Powers of Al, Havar, Ni, Ti and Ta Media for 9.67 MeV/u 58Ni and 9.5 MeV/u 18O Ions NUCLEAR REACTIONS 27Al, Ti, Ni, Ta(58Ni, 58Ni'), E=9.67 MeV/nucleon; 27Al, Ti, Ni, Ta(18O, 18O'), E=9.5 MeV/nucleon; measured energy loss vs target thickness; deduced stopping powers. Comparison with previous results, model predictions.
doi: 10.1016/S0168-583X(01)00930-2
1995HA42 Appl.Radiat.Isot. 46, 425 (1995) A.Hakim, A.Fahli, M.Ohta, G.Guillaume, J.P.Coffin, P.Fintz, F.Jundt, A.Malki, F.Rami, B.Rastegar, P.Wagner, M.Zahar Prompt and Delayed Charged-Particle Emissions in Low Impact Parameter Collision of 40Ar(1100 MeV) and 24Mg NUCLEAR REACTIONS, ICPND 24Mg(40Ar, X), E=1100 MeV; measured σ(θ(light charged particle), θ(fragment), E), d-, t-, p-, α-yield ratios. Two-moving source model analysis.
doi: 10.1016/0969-8043(95)00036-4
1994HA54 Nuovo Cim. 107A, 1587 (1994) A.Hakim, A.Fahli, M.Ohta, G.Guillaume, J.P.Coffin, P.Fintz, J.Jundt, A.Malki, F.Rami, B.Rastegar, P.Wagner, M.Zahar Prompt and Thermal Light-Charged-Particle Emissions in the Central 40Ar(1100 MeV) + 24Mg Reactions NUCLEAR REACTIONS 24Mg(40Ar, X), E=1100 MeV; measured (light charged particle)(evaporation residue)-coin; deduced thermal, preequilibrium emission regions separation, model parameters. 64Zn deduced energy, temperature.
doi: 10.1007/BF02780693
1988GO12 Phys.Rev. C38, 135 (1988) M.Gonin, J.P.Coffin, G.Guillaume, F.Jundt, P.Wagner, P.Fintz, B.Heusch, A.Malki, A.Fahli, S.Kox, F.Merchez, J.Mistretta Preequilibrium Emission and Incomplete Fusion of Low and Medium Mass Heavy Ion Systems NUCLEAR REACTIONS 45Sc(40Ar, X), 24Mg(40Ar, X), 13C(40Ar, X), E=1100 MeV; measured fragment velocity, light particle (p, d, t, α) energy, σ(θ), σ(E, A); deduced projectile linear momentum transfer, compound nucleus excitation energy, temperature, entrance channel asymmetry dependence, incomplete fusion, pre-equilibrium emission properties.
doi: 10.1103/PhysRevC.38.135
1987FA02 Z.Phys. A326, 169 (1987) A.Fahli, J.P.Coffin, G.Guillaume, B.Heusch, F.Jundt, F.Rami, P.Wagner, P.Fintz, A.J.Cole, S.Kox, Y.Schutz, N.Cindro Light Charged Particle Emission in 40Ar Induced Reactions on 68Zn at 14.6, 19.6 and 35 MeV/Nucleon NUCLEAR REACTIONS 68Zn(40Ar, X), E=14.6, 19.6, 35 MeV/nucleon; measured σ(fragment θ), σ(fragment θ, E), for X=p, d, t, 3,4He, 6,7Li. Enriched target, telescope system. Preequilibrium emission, moving source, coalescence models.
1987RA10 Z.Phys. A327, 207 (1987) F.Rami, A.Fahli, J.P.Coffin, G.Guillaume, B.Heusch, F.Jundt, P.Wagner, P.Fintz, S.Kox, Y.Schutz, M.C.Mermaz Origin of Projectile-Like Fragments from 40Ar + 68Zn Collisions between 15 and 35 MeV/Nucleon: Direct transfer of nucleons and projectile fragmentation NUCLEAR REACTIONS 68Zn(40Ar, X), E=14.6, 19.6, 27.6, 35 MeV/nucleon; measured σ(fragment θ, E), σ(fragment θ), σ(fragment Z); deduced fragment velocities, linear momentum distribution widths. Enriched target, tof, ΔE-E telescope.
1986FA05 Phys.Rev. C34, 161 (1986) A.Fahli, J.P.Coffin, G.Guillaume, B.Heusch, F.Jundt, F.Rami, P.Wagner, P.Fintz, A.J.Cole, S.Kox, Y.Schutz Incomplete Fusion in the 40Ar + 68Zn Reaction: Trends and limits NUCLEAR REACTIONS 68Zn(40Ar, X), E=14.6, 19.6, 27.6, 35 MeV/nucleon; measured σ(fragment θ), fragment mass vs velocity; deduced fusion σ(E), reaction mechanism.
doi: 10.1103/PhysRevC.34.161
1985ME08 Phys.Rev. C31, 1972 (1985) M.C.Mermaz, F.Rami, J.P.Coffin, G.Guillaume, B.Heusch, P.Wagner, A.Fahli, P.Fintz Direct Surface Transfer Reactions Induced by a 1102 MeV 40Ar Beam on 68Zn Target Nucleus NUCLEAR REACTIONS 68Zn(40Ar, X), E=1102 MeV; measured σ(fragment θ, E) for X=42,41Ca, 36,37Cl, 39K; deduced level densities, diffraction model parameters.
doi: 10.1103/PhysRevC.31.1972
1985RA23 Nucl.Phys. A444, 325 (1985) F.Rami, J.P.Coffin, G.Guillaume, B.Heusch, P.Wagner, A.Fahli, P.Fintz Study of the 40Ar + 68Zn Reaction at 27.6 MeV/Nucleon NUCLEAR REACTIONS 68Zn(40Ar, X), E=1102 MeV; measured fragment σ(θ), σ(E, Z, A); deduced reaction σ, dominant reaction mechanisms. Time-of-flight, telescope spectrometers, solid-state detectors. Enriched target.
doi: 10.1016/0375-9474(85)90353-7
1984CO14 Phys.Rev. C30, 539 (1984) J.P.Coffin, G.Guillaume, A.Fahli, F.Rami, B.Heusch, P.Wagner, P.Engelstein, P.Fintz, N.Cindro Transitional Dissipative Mechanism in the 32S + 59Co Reaction NUCLEAR REACTIONS 59Co(32S, X), (32S, F), E=128, 143, 158, 178, 198 MeV; measured fission, evaporation residue fragment energy, mass distributions, σ(E), σ(fragment θ, A); deduced fusion σ, fission mechanism.
doi: 10.1103/PhysRevC.30.539
1984RA12 Z.Phys. A318, 239 (1984) F.Rami, J.P.Coffin, G.Guillaume, B.Heusch, P.Wagner, A.Fahli, P.Fintz Few Nucleon Transfer Versus Fragmentation in the Production of Projectile-Like Fragments in the 40Ar + 68Zn Reaction at 27.6 MeV/Nucleon NUCLEAR REACTIONS 68Zn(40Ar, X), E=27.6 MeV/nucleon; measured fragment velocity, momentum width, isotope distributions; deduced fragmentation process, nucleon transfer, damped collision roles.
doi: 10.1007/BF01413475
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