NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = M.E.Brandan Found 51 matches. 2001BR17 Nucl.Phys. A688, 659 (2001) M.E.Brandan, A.Menchaca-Rocha, L.Trache, H.L.Clark, A.Azhari, C.A.Gagliardi, Y.-W.Lui, R.E.Tribble, R.L.Varner, J.R.Beene, G.R.Satchler Refractive Elastic Scattering of 16O by 12C at 300 MeV NUCLEAR REACTIONS 12C(16O, 16O), (16O, 12C), E=300 MeV; measured σ(θ); deduced optical model parameters, potential characteristics. Airy structure, nuclear rainbow.
doi: 10.1016/S0375-9474(00)00588-1
2001GO39 Nucl.Phys. A693, 603 (2001) The Dispersion Relation Applied to the Radial Shape and Energy Dependence of the 16O-16O Potential at Intermediate Energies NUCLEAR REACTIONS 16O(16O, 16O), E=145-704 MeV; calculated σ(θ), dispersive contribution.
doi: 10.1016/S0375-9474(01)00801-6
2001SZ05 Phys.Rev. C64, 064614 (2001) S.Szilner, M.P.Nicoli, Z.Basrak, R.M.Freeman, F.Haas, A.Morsad, M.E.Brandan, G.R.Satchler Refractive Elastic Scattering of Carbon and Oxygen Nuclei: The mean field analysis and Airy structures NUCLEAR REACTIONS 12C(16O, 16O), E=62-124 MeV; 12C(18O, 18O), E=66-120 MeV; measured σ(θ); deduced potential features. Optical model analysis, Airy structures.
doi: 10.1103/PhysRevC.64.064614
2000NI03 Phys.Rev. C61, 034609 (2000) M.P.Nicoli, F.Haas, R.M.Freeman, S.Szilner, Z.Basrak, A.Morsad, G.R.Satchler, M.E.Brandan Detailed Study and Mean Field Interpretation of 16O + 12C Elastic Scattering at Seven Medium Energies NUCLEAR REACTIONS 12C(16O, 16O), E=62-124 MeV; measured σ(θ); deduced parameters. Optical model analysis, Woods-Saxon and folding-model potentials. Comparison with potentials at higher energies and for similar systems.
doi: 10.1103/PhysRevC.61.034609
1999NI08 Phys.Rev. C60, 064608 (1999) M.P.Nicoli, F.Haas, R.M.Freeman, N.Aissaoui, C.Beck, A.Elanique, R.Nouicer, A.Morsad, S.Szilner, Z.Basrak, M.E.Brandan, G.R.Satchler Elastic Scattering of 16O + 16O at Energies E/A between 5 and 8 MeV NUCLEAR REACTIONS 16O(16O, 16O), E=75-124 MeV; measured σ(θ); deduced phenomenological and microscopic potentials. Optical model, interpretation in terms of Airy minima and the dispersion relation.
doi: 10.1103/PhysRevC.60.064608
1999NI14 Nucl.Phys. (Supplement) A654, 882c (1999) M.P.Nicoli, F.Haas, R.M.Freeman, N.Aissaoui, C.Beck, A.Elanique, R.Nouicer, A.Morsad, S.Szilner, Z.Basrak, M.E.Brandan Refractive Effects in the Elastic Scattering of Light Heavy Ions between 5 and 10 MeV/n: The 16O + 16O reaction NUCLEAR REACTIONS 16O(16O, 16O), E=75-124 MeV; measured σ(θ); deduced refractive effects. Optical model analysis.
doi: 10.1016/S0375-9474(00)88565-6
1998KO29 Nucl.Phys. A637, 175 (1998) Y.Kondo, M.E.Brandan, G.R.Satchler Shape Resonances and Deep Optical Potentials: A mean-field description of 12C + 12C Scattering at low energies NUCLEAR REACTIONS 12C(12C, 12C), E(cm) < 725 MeV; analyzed σ(E), σ(θ), shape resonances; deduced optical potential features.
doi: 10.1016/S0375-9474(98)00212-7
1997BR04 Phys.Rev. C55, 1353 (1997) M.E.Brandan, H.Chehime, K.W.McVoy Limits to the Validity of the Glauber Approximation for Heavy-Ion Scatering, and a Possible Assessment of In-Medium NN Pauli Blocking NUCLEAR REACTIONS 12C(12C, 12C), E=360, 1016 MeV; 12C(16O, 16O), E=608, 1503 MeV; 16O(16O, 16O), E=350 MeV; calculated phase shifts; deduced Glauber approximation validity limitations, in-medium NN-Pauli blocking assessement related features.
doi: 10.1103/PhysRevC.55.1353
1997BR05 Phys.Rev. C55, 1362 (1997) Remarkable Optical-Potential Systematics for Lighter Heavy Ions NUCLEAR REACTIONS 90Zr(α, α), E=20 MeV/nucleon; 16O(16O, 16O), E=22 MeV/nucleon; 12C(12C, 12C), E=13 MeV/nucleon; 58Ni(7Li, 7Li), E=35 MeV/nucleon; 12C(16O, 16O), E=38 MeV/nucleon; 12C(20Ne, 20Ne), E=20 MeV/nucleon; analyzed σ(θ), other aspects; deduced model parameters, reaction suppression regions, related features.
doi: 10.1103/PhysRevC.55.1362
1997BR30 Phys.Rep. 285, 143 (1997) The Interaction between Light Heavy-Ions and What It Tells Us NUCLEAR REACTIONS 12C(12C, 12C), E=79-1016 MeV; 16O(16O, 16O), E=124-704 MeV; compiled, analyzed σ(θ); deduced optical model features, parameters, folding model importance. Other reactions discussed.
doi: 10.1016/S0370-1573(96)00048-8
1997CA49 Phys.Rev. C56, 2700 (1997) J.M.Casandjian, R.Lichtenthaler, W.Mittig, A.Lepine-Szily, A.C.C.Villari, G.Auger, R.Beunard, L.Bianchi, M.E.Brandan, J.L.Ciffre, A.Cunsolo, A.Foti, A.Menchaca-Rocha, N.A.Orr, E.Plagnol, R.H.Siemssen, J.P.Wieleczko Atomic Effects in Heavy-Ion Elastic Scattering NUCLEAR REACTIONS 208Pb(208Pb, 208Pb), E=786.7, 1029.9 MeV; Ag(208Pb, 208Pb), E=873.4, 1029.9, 1129.7 MeV; measured σ(θ); deduced atomic effects. Monte Carlo simulation analysis.
doi: 10.1103/PhysRevC.56.2700
1996GA06 Appl.Radiat.Isot. 47, 111 (1996) Influence of Annealing on TLD-100 Response to 5.3 MeV α-Particles RADIOACTIVITY 241Am(α); 60Co(β-); measured air-annealed chips glow curves; deduced effect of annealing on TLD-100 dosemeters response.
doi: 10.1016/0969-8043(95)00256-1
1995GE10 Phys.Rev.Lett. 75, 3082 (1995) C.J.Gelderloos, J.M.Alexander, N.N.Ajitanand, E.Bauge, A.Elmaani, T.Ethvignot, L.Kowalski, R.A.Lacey, M.E.Brandan, A.Giorni, D.Heuer, S.Kox, A.Lleres, A.Menchaca-Rocha, F.Merchez, D.Rebreyend, J.B.Viano, B.Chambon, B.Cheynis, D.Drain, C.Pastor Time Relationships between Direct Particle Emission and Fragmentation: A probe for nuclear expansion prior to fragment freeze-out NUCLEAR REACTIONS Ag(40Ar, X), E=34 MeV/nucleon; measured intermediate mass fragment emission time relative to 2H, 3He; deduced prior fragment freeze-out expansion features.
doi: 10.1103/PhysRevLett.75.3082
1995GE12 Phys.Rev. C52, R2834 (1995) C.J.Gelderloos, R.Sun, N.N.Ajitanand, J.M.Alexander, E.Bauge, A.Elmaani, T.Ethvignot, R.A.Lacey, M.E.Brandan, A.Giorni, D.Heuer, S.Kox, A.Lleres, A.Menchaca-Rocha, F.Merchez, D.Rebreyend, J.B.Viano, B.Chambon, B.Cheynis, D.Drain, C.Pastor Emission Times for Energy Selected 1,2,3H Ejectiles from Central Collisions: 1360 MeV 40Ar + Ag NUCLEAR REACTIONS Ag(40Ar, X), E=1.36 GeV; measured (fragment)(fragment) relative momentum, velocity difference correlations for 1,2,3H ejectiles; deduced emission times, mechanism.
doi: 10.1103/PhysRevC.52.R2834
1995HE07 Nucl.Phys. A583, 537c (1995) D.Heuer, A.Chabane, M.E.Brandan, M.Charvet, A.J.Cole, P.Desesquelles, A.Giorni, A.Lleres, A.Menchaca-Rocha, J.B.Viano, D.Benchekroun, B.Cheynis, A.Demeyer, E.Gerlic, D.Guinet, M.Stern, L.Vagneron Blast Expansion in 32S + 27Al at 37.5 MeV/nucleon NUCLEAR REACTIONS 27Al(32S, X), E=37.5 MeV/nucleon; measured fragment charge distributions; deduced multi-fragmentation, decay mechansim.
doi: 10.1016/0375-9474(94)00716-Z
1995LE06 Nucl.Phys. A583, 263c (1995) A.Lepine-Szily, J.M.Casandjian, W.Mittig, A.C.C.Villari, R.Lichtenthaler Filho, G.Auger, L.Bianchi, R.Beunard, M.E.Brandan, J.L.Ciffre, A.Cunsolo, A.Foti, L.Gaudard, A.Menchaca-Rocha, N.A.Orr, E.Plagnol, Y.Schutz, R.H.Siemssen, J.P.Wieleczko The High Precision Measurement of 208Pb + 208Pb Mott Scattering at Energies Under the Coulomb Barrier: The observation of new atomic effects NUCLEAR REACTIONS 208Pb, 238U(208Pb, 208Pb), E ≈ 5 MeV/nucleon; measured Mott, elastic scattering; deduced new atomic effects related features.
doi: 10.1016/0375-9474(94)00670-I
1995LO02 Nucl.Phys. A581, 373 (1995) Y.Lou, M.Gonin, R.Wada, K.Hagel, J.Li, B.Xiao, M.Gui, D.Utley, R.Tezkratt, L.Cooke, T.Botting, B.Hurst, D.O'Kelly, G.Mouchaty, R.P.Schmitt, W.Turmel, J.B.Natowitz, D.Fabris, G.Nebbia, G.Viesti, J.Ruiz, R.Burch, F.Gramegna, M.Poggi, G.Prete, M.E.Brandan, A.Menchaca-Rocha Light-Particle Evaporation as a Function of Neutron Excess for Medium-Mass Compound Nuclei with E(x) ≈ 2 MeV/u NUCLEAR REACTIONS 92,100Mo(63Cu, F), E=10 MeV/nucleon; 144,148,154Sm(20Ne, F), E=20 MeV/nucleon; measured fission (fragment)α-coin, proton, neutron, α-multiplicities, mass, total kinetic energy, linear momentum transfer distributions; deduced dynamic fission role. Statistical model analysis.
doi: 10.1016/0375-9474(94)00482-3
1994HE27 Phys.Rev. C50, 1943 (1994) D.Heuer, A.Chabane, M.E.Brandan, M.Charvet, A.J.Cole, P.Desesquelles, A.Giorni, A.Lleres, A.Menchaca-Rocha, J.B.Viano, D.Benchekroun, B.Cheynis, A.Demeyer, E.Gerlic, D.Guinet, M.Stern, L.Vagneron Explosive Multifragmentation in the 32S + 27Al Reaction at 37.5 MeV/nucleon NUCLEAR REACTIONS 27Al(32S, X), E=37.5 MeV/nucleon; measured largest charge, inclusive charge distribution; deduced multi-fragmentation mechanism. Statistical decay model.
doi: 10.1103/PhysRevC.50.1943
1993BR11 Phys.Rev. C48, 1147 (1993) M.E.Brandan, J.R.Alfaro, A.Menchaca-Rocha, J.Gomez del Campo, G.R.Satchler, P.H.Stelson, H.J.Kim, D.Shapira Elastic Scattering of 58Ni + 27Al at Near-Barrier Energies NUCLEAR REACTIONS 27Al(58Ni, 58Ni), E=155-220 MeV; measured σ(E, θ); deduced optical model parameters, potential volume integrals. Phenomenological folding model, dispersion relations analyses.
doi: 10.1103/PhysRevC.48.1147
1993BR19 Nucl.Instrum.Methods Phys.Res. A334, 461 (1993) M.E.Brandan, A.J.Cole, P.Desesquelles, A.Giorni, D.Heuer, A.Lleres, A.Menchaca-Rocha, K.Michaelian Effect of the Detector Response on Measurements Performed with Heavy-Ion 4π Detectors NUCLEAR REACTIONS 27Al(32S, X), E=37.5 MeV/nucleon; 40Ca(40Ca, X), E=35 MeV/nucleon; calculated, simulated fragment velocity, total parallel momentum vs Z, multiplicities, charge distributions. Microscopic approach, Monte Carlo techniques. Heavy-ion 4π detectors investigated.
doi: 10.1016/0168-9002(93)90809-V
1993CO04 Phys.Rev. C47, 1251 (1993) A.J.Cole, M.E.Brandan, P.Desesquelles, A.Giorni, D.Heuer, A.Lleres, A.Menchaca-Rocha, J.B.Viano, B.Chambon, B.Cheynis, D.Drain, C.Pastor Recoil Effects in Sequential Emission and Coulomb Dissociation NUCLEAR REACTIONS Cu(40Ca, X), E=35 MeV/nucleon; analyzed reconstructed projectile like fragments charge partition from decay data; deduced no evidence for decay mechanism evolution.
doi: 10.1103/PhysRevC.47.1251
1993LL01 Phys.Rev. C48, 2753 (1993) A.Lleres, A.Giorni, H.Elhage, M.E.Brandan, A.J.Cole, P.Desesquelles, D.Heuer, A.Menchaca-Rocha, J.B.Viano, F.Benrachi, B.Chambon, B.Cheynis, D.Drain, C.Pastor Multidetector Study of Primary Projectilelike Fragments in the Reaction 40Ca + (nat)Cu at 35 MeV/nucleon NUCLEAR REACTIONS Cu(40Ca, X), E=35 MeV/nucleon; measured projectile-like fragment charges, velocities, emission angles; deduced fragment excitation energy distribution, angular momentum. Statistical binary decay model.
doi: 10.1103/PhysRevC.48.2753
1992BR15 Phys.Lett. 281B, 185 (1992) M.E.Brandan, K.W.McVoy, G.R.Satchler Analysis of an Unusual Potential Ambiguity for 16O + 16O Scattering NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; analyzed σ(θ).
doi: 10.1016/0370-2693(92)91126-T
1992MC07 Nucl.Phys. A542, 295 (1992) The 90° Excitation Function for Elastic 12C + 12C Scattering The Importance of Airy Elephants NUCLEAR REACTIONS 12C(12C, 12C), E=70-140 MeV; analyzed σ(E, θ=90°), σ(θ); deduced potentials.
doi: 10.1016/0375-9474(92)90218-9
1992ME02 Phys.Rev. C45, 1189 (1992) A.Menchaca-Rocha, E.Garcia-Solis, E.Belmont-Moreno, M.E.Brandan, M.Buenerd, J.Chauvin, P.DeSaintignon, G.Duhamel, D.Lebrun, P.Martin, G.Perrin, J.Y.Hostachy Low-Energy Intermediate Mass Fragments in the 16O + 12C Reaction at 38 MeV/Nucleon NUCLEAR REACTIONS 12C(16O, X), E=708 MeV; measured σ(fragment θ, E) for X=6Li, 12C, σ(θ) for Z=3-9; deduced reaction residues yield mechanism. Cascade model.
doi: 10.1103/PhysRevC.45.1189
1991BR04 Phys.Rev. C43, 1140 (1991) Rainbow-Shift Mechanism Behind Discrete Optical-Potential Ambiguities NUCLEAR REACTIONS 58Ni(6Li, 6Li), E=210 MeV; calculated σ(θ). 12C(12C, 12C), E=78 MeV; 90Zr(d, d), E=11.8 MeV; calculated σ(θ) related quanties; deduced low partial waves role.
doi: 10.1103/PhysRevC.43.1140
1991BR08 Phys.Lett. 256B, 311 (1991) Optical Potential Ambiguities and 16O + 16O at 350 MeV NUCLEAR REACTIONS 16O(16O, 16O), E=350 MeV; calculated σ(θ); deduced optical potential ambiguities. General optical model.
doi: 10.1016/0370-2693(91)91767-P
1990BR05 Phys.Rev. C41, 1520 (1990) M.E.Brandan, M.Rodriguez-Villafuerte, A.Ayala 12C + 12C Elastic Scattering Analysis Above E/A = 6 MeV using Deep Real Potentials NUCLEAR REACTIONS, ICPND 12C(12C, 12C), E=70.7-1440 MeV; analyzed data; deduced optical model parameters, reaction σ. Folding, phenomenological optical model analyses.
doi: 10.1103/PhysRevC.41.1520
1990BR21 Phys.Rev. C42, 2236 (1990) M.E.Brandan, S.E.Soberano, E.Belmont-Moreno, A.Menchaca-Rocha, M.Gonin, R.Wada, J.B.Natowitz Nuclear Refraction in 14N + 12C Elastic Scattering at E/A = 20 MeV NUCLEAR REACTIONS 12C(14N, 14N), E=280 MeV; measured σ(θ); deduced model parameters. Optical model, phenomenological, folding model potentials.
doi: 10.1103/PhysRevC.42.2236
1990ME07 Phys.Rev. C41, 2654 (1990) A.Menchaca-Rocha, E.Belmont-Moreno, M.E.Brandan, A.Martinez, D.Abriola, M.Elgue, A.Etchegoyen, M.C.Etchegoyen, J.O.Fernandez-Niello, D.E.DiGregorio, M.diTada, A.O.Macchiavelli, A.J.Pacheco, J.E.Testoni Search for a Valence-Neutron-Induced Enhancement in the Sub-Barrier Fusion of 32S + 12,13C NUCLEAR REACTIONS, ICPND 32S(12C, X), (13C, X), E=47-72 MeV; measured evaporation residues σ(θ); deduced fusion σ. Schematic coupled channel calculations.
doi: 10.1103/PhysRevC.41.2654
1988BR04 Phys.Rev.Lett. 60, 784 (1988) Unambiguous Imaginary Potential in the Optical-Model Description of Light Heavy-Ion Elastic Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=140-1016 MeV; 12C(16O, 16O), E=608-1503 MeV; calculated σ(θ); deduced optical model parameters.
doi: 10.1103/PhysRevLett.60.784
1988BR20 Phys.Rev. C38, 673 (1988) M.E.Brandan, S.H.Fricke, K.W.McVoy Resolution of Potential Ambiguities through Farside Angular Structure: Data summary NUCLEAR REACTIONS 12C(12C, 12C), E=240, 158.8 MeV; 12C(16O, 16O), E=608 MeV; measured σ(θ); deduced model parameters. Semi-classical analysis, nearside, farside decomposition.
doi: 10.1103/PhysRevC.38.673
1988BR29 Nucl.Phys. A487, 477 (1988) Folding Model Analysis of 12,13C + 12C and 16O + 12C Scattering at Intermediate Energies Using a Density-Dependent Interaction NUCLEAR REACTIONS 12C(12C, 12C), E=0.14-1.016 GeV; 12C(16O, 16O), E=0.14-1.503 GeV; 12C(13C, 13C), E=9-120 MeV/nucleon; analyzed data; deduced model parameters. Folding potential, density-, energy dependent interactions.
doi: 10.1016/0375-9474(88)90625-2
1988FR14 Phys.Rev. C38, 682 (1988) S.H.Fricke, M.E.Brandan, K.W.McVoy Resolution of Potential Ambiguities through Farside Angular Structure: Semiclassical analysis NUCLEAR REACTIONS 12C(12C, 12C), E=158.8, 240 MeV; 12C(16O, 16O), E=608 MeV; calculated σ(θ); deduced model parameters. Semi-classical analysis, near, farside decomposition.
doi: 10.1103/PhysRevC.38.682
1988KO27 Nucl.Phys. A487, 457 (1988) A.M.Kobos, M.E.Brandan, G.R.Satchler Further Optical Model Studies of 16O Scattering at E/A = 94 MeV NUCLEAR REACTIONS 12C(16O, 16O), E=94 MeV/nucleon; 28Si(16O, 16O), E=1.47 GeV; analyzed data; deduced model parameters. Optical model.
doi: 10.1016/0375-9474(88)90624-0
1988PE01 Nucl.Instrum.Methods Phys.Res. A263, 480 (1988) J.J.Perez-Padilla, M.E.Brandan A Simple Expression to Improve the 12C(n, px) Reaction Description in Neutron Efficiency Codes NUCLEAR REACTIONS 12C(n, pX), E=27, 40, 61 MeV; calculated σ(θ, Ep); deduced direct reaction component.
doi: 10.1016/0168-9002(88)90989-8
1987MA20 Phys.Rev. C35, 2125 (1987) Z.Majka, M.E.Brandan, D.Fabris, K.Hagel, A.Menchaca-Rocha, J.B.Natowitz, G.Nebbia, G.Prete, B.Sterling, G.Viesti Production and Deexcitation of Highly Deformed 67Ga NUCLEAR REACTIONS 63Cu(α, α), (α, p), 55Mn(12C, α), (12C, p), 51V(16O, α), (16O, p), E ≈ 130 MeV; 27Al(40Ar, α), (40Ar, p), E=240 MeV; measured σ(Eα, θα), σ(Ep, θp). 67Ga deduced p-, α-emission characteristics. ΔE-E, ionization chamber telescopes. Statistical model analyses.
doi: 10.1103/PhysRevC.35.2125
1986BR25 Phys.Rev. C34, 1484 (1986) M.E.Brandan, A.Menchaca-Rocha, M.Buenerd, J.Chauvin, P.DeSaintignon, G.Duhamel, D.Lebrun, P.Martin, G.Perrin, J.Y.Hostachy Elastic and Inelastic 16O + 12C Scattering at 38 MeV/Nucleon NUCLEAR REACTIONS 12C(16O, 16O), (16O, 16O'), E=608 MeV; measured σ(θ); deduced reaction σ. Magnetic spectrometer. Optical model, DWBA analyses.
doi: 10.1103/PhysRevC.34.1484
1986BR26 J.Phys.(London) G12, 391 (1986) M.E.Brandan, A.Menchaca-Rocha, A.Szanto de Toledo, N.Carlin Filho, E.M.Szanto, M.M.Coimbra Detection of 8Be Nuclei from the Reaction 16O + 27Al at 65 MeV NUCLEAR REACTIONS 27Al(16O, 8Be), E=65 MeV; measured σ(E(8Be)), ejectile production σ. ΔE-E telescope. Two-body kinematic calculations.
doi: 10.1088/0305-4616/12/5/006
1983BR01 J.Phys.(London) G9, 197 (1983) 12C - 12C Total and Reaction Cross Sections between 6 and 85 MeV/A from an Optical-Model Analysis NUCLEAR REACTIONS 12C(12C, 12C), E=6-85 MeV/nucleon; analyzed σ(θ); deduced σ(total), σ(reaction). Optical model.
doi: 10.1088/0305-4616/9/2/012
1983ME04 Phys.Lett. 121B, 111 (1983) A.Menchaca-Rocha, M.E.Brandan, A.Dacal, A.Galindo, J.Mahoney, M.Murphy, W.D.M.Rae Incomplete Momentum Transfer Components in 16O + 12C Fusion at 20 MeV/A NUCLEAR REACTIONS 12C(16O, X), E=20 MeV/nucleon; measured σ(fragment E), fragment relative yield vs Z; deduced incomplete momentum transfer in fusion.
doi: 10.1016/0370-2693(83)90896-1
1983ME10 J.Phys.(London) G9, L181 (1983) A.Menchaca-Rocha, M.E.Brandan, R.Legrain, A.Dacal, A.Galindo Target Dependence of 16O-Induced Reactions at 20 MeV/A NUCLEAR REACTIONS 12C, 60Ni(16O, X), E=315 MeV; measured σ(fragment θ, E), quasielastic fragment production σ for X=C, N, full yields for X=B, Be vs target mass.
doi: 10.1088/0305-4616/9/8/007
1983ME22 Phys.Lett. 131B, 31 (1983) A.Menchaca-Rocha, M.E.Brandan, M.Buenerd, J.Chauvin, D.Lebrun, P.Martin, P.de Saintignon, J.C.Gondrand, I.Dorion, A.Lounis Measurement of Reactions Induced by 30 MeV/A 12C NUCLEAR REACTIONS 12C, 58Ni(12C, α), (12C, 9Be), (12C, X), 197Au(12C, X), E=30 MeV/nucleon; measured σ(θ, Eα), σ(θ, E(9Be)), σ(fragment θ) for X=10C, 10B, 7Be, 6,7Li. Coalescence model analysis.
doi: 10.1016/0370-2693(83)91085-7
1982BR20 Phys.Rev.Lett. 49, 1132 (1982) Nuclear Rainbow Scattering in 12C- 12C above 160 MeV NUCLEAR REACTIONS 12C(12C, 12C), E=161.1, 288.6, 1030 MeV; analyzed data; deduced rainbow scattering characteristics. Optical, semi-classical model analyses.
doi: 10.1103/PhysRevLett.49.1132
1982ME12 Phys.Rev. C26, 1764 (1982) Friction and Geometry in 16O-Induced Reactions NUCLEAR REACTIONS 12C, 27Al, 60Ni, 208Pb(16O, X), E=100-315 MeV; analyzed data; deduced mass flow rate, frictional coefficient target mass, energy dependence. One-body energy dissipation.
doi: 10.1103/PhysRevC.26.1764
1981BR05 Phys.Rev. C23, 1272 (1981) Total Reaction Cross Section for 16O - 12C at E(cm)=60, 93, and 135 MeV NUCLEAR REACTIONS 12C(16O, 16O), E=140, 218, 315 MeV; measured σ(E, θ); deduced total σ(reaction). Optical model analysis.
doi: 10.1103/PhysRevC.23.1272
1981CO22 Phys.Rev.Lett. 47, 1705 (1981) A.J.Cole, W.D.M.Rae, M.E.Brandan, A.Dacal, B.G.Harvey, R.Legrain, M.J.Murphy, R.G.Stokstad 12C + 12C Reaction Cross Section between 70 and 290 MeV Obtained from Elastic Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=120-290 MeV; measured σ(θ) vs momentum transfer; deduced σ(total), σ(reaction).
doi: 10.1103/PhysRevLett.47.1705
1981ME15 Phys.Rev. C24, 2777 (1981) Unification for the Angular Distributions Observed in 16O-Induced Reactions NUCLEAR REACTIONS 12C, 27Al, 60Ni, 208Pb(16O, X), E=100-315 MeV; measured σ(θ) for X=B, C, N, O, F; deduced interaction times, friction coefficients. Friction model.
doi: 10.1103/PhysRevC.24.2777
1977BR27 Nucl.Phys. A287, 205 (1977); Erratum Nucl.Phys. A306, 536 (1978) Vector Analyzing Power and Cross Section for (d, t) and (d, 3He) Reactions on 64Zn at E = 13 MeV NUCLEAR REACTIONS 64Zn(polarized d, d), E=13.0 MeV; measured vector analyzing power iT11(θ), cross section σ(θ); deduced optical-model parameters. 64Zn(polarized d, t), (polarized d, 3He), E=13.0 MeV; measured iT11(θ), σ(θ). 63Zn, 63Cu levels deduced J, π, S. Enriched target.
doi: 10.1016/0375-9474(77)90491-2
1977BR28 Nucl.Phys. A287, 213 (1977) Tensor Analyzing Powers in 64Zn(d, t)63Zn and 64Zn(d, 3He)63Cu at E = 13 MeV NUCLEAR REACTIONS 64Zn(polarized d, t), (polarized d, 3He), E=13.0 MeV; measured A(θ). Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(77)90492-4
1976BR17 Nucl.Phys. A263, 189 (1976) M.E.Brandan, G.R.Plattner, W.Haeberli A Test of p-4He Phase Shifts between 2 and 9 MeV NUCLEAR REACTIONS 4He(polarized p, p), E=3.47-8.94 MeV; measured A(E, θ). 4He(p, p), E=2.24-5.90 MeV; measured σ(168.8°)/σ(104.4°). Phase-shift analysis.
doi: 10.1016/0375-9474(76)90167-6
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