NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = G.R.Satchler Found 189 matches. Showing 1 to 100. [Next]2002KH01 Phys.Rev. C65, 024611 (2002) D.T.Khoa, G.R.Satchler, D.T.Nguyen Do 1.37 GeV α Particles Find Nuclei Attractive or Repulsive ? NUCLEAR REACTIONS 12C, 40Ca(α, α), E=1370 MeV; analyzed σ(θ); deduced optical potential features.
doi: 10.1103/PhysRevC.65.024611
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
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
2000KH06 Nucl.Phys. A668, 3 (2000) Generalized Folding Model for Elastic and Inelastic Nucleus-Nucleus Scattering using Realistic Density Dependent Nucleon-Nucleon Interaction NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=112, 121.6, 240, 300 MeV; 58,60Ni(α, α), (α, α'), E=172.5 MeV; calculated σ(θ), σ(E, θ). Generalized double-folding model. Comparison with data, other models.
doi: 10.1016/S0375-9474(99)00680-6
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
2000OG06 Phys.Rev. C62, 044601 (2000) A.A.Ogloblin, Yu.A.Glukhov, W.H.Trzaska, A.S.Demyanova, S.A.Goncharov, R.Julin, S.V.Klebnikov, M.Mutterer, M.V.Rozhkov, V.P.Rudakov, G.P.Tiorin, D.T.Khoa, G.R.Satchler New Measurement of the Refractive, Elastic 16O + 12C Scattering at 132, 170, 200, 230, and 260 MeV Incident Energies NUCLEAR REACTIONS 12C(16O, 16O), E=132, 170, 200, 230, 260 MeV; measured σ(θ); deduced rainbow scattering features, optical model parameters.
doi: 10.1103/PhysRevC.62.044601
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
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
1998OG02 Phys.Rev. C57, 1797 (1998) A.A.Ogloblin, D.T.Khoa, Y.Kondo, Yu.A.Glukhov, A.S.Demyanova, M.V.Rozhkov, G.R.Satchler, S.A.Goncharov Pronounced Airy Structure in Elastic 16O + 12C Scattering at E(lab) = 132 MeV NUCLEAR REACTIONS 12C(16O, 16O), E=132 MeV; measured σ(θ); deduced Airy minimum, refractive scattering features. Optical model analysis.
doi: 10.1103/PhysRevC.57.1797
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
1997KH04 Phys.Rev. C56, 954 (1997) D.T.Khoa, G.R.Satchler, W.von Oertzen Nuclear Incompressibility and Density Dependent NN Interactions in the Folding Model for Nucleus-Nucleus Potentials NUCLEAR REACTIONS 58Ni, 12C(α, α), E=104-172.5 MeV; 40Ca(α, α), E=80-141.7 MeV; 90Zr(α, α), E=79.5-141.7 MeV; 208Pb(α, α), E=104-139 MeV; 16O(16O, 16O), E=250, 350, 480 MeV; 12C(12C, 12C), E=126.7, 300, 1016, 1503 MeV; analyzed σ(θ); deduced optical model parameters, density dependence, incompressibility. M3Y effective interaction.
doi: 10.1103/PhysRevC.56.954
1997SA03 Phys.Rev. C55, 285 (1997) Missing Monopole Strength in 58Ni and Uncertainties in the Analysis of α-Particle Scattering NUCLEAR REACTIONS 58Ni(α, α'), E=140-340 MeV; calculated σ(θ) vs E. 58Ni deduced multipole transition strengths, dependence on model parameters. Folding model.
doi: 10.1103/PhysRevC.55.285
1996BE02 Nucl.Phys. A596, 137 (1996) J.R.Beene, D.J.Horen, G.R.Satchler Critical Comparison of Folded Potential and Deformed Potential Models of Heavy-Ion Inelastic Scattering NUCLEAR REACTIONS 208Pb(17O, X), E=22, 84 MeV/nucleon; 208Pb(86Kr, X), E=43 MeV/nucleon; 90Zr(17O, X), E=84 MeV/nucleon; 208Pb(12C, X), E=8 MeV/nucleon; 90Zr(α, X), E=35.4 MeV; calculated σ ratio vs multipolarity. 208Pb(17O, 17O'), E=22 MeV/nucleon; analyzed σ(θ); deduced deformed, folded potentials critical comparison.
doi: 10.1016/0375-9474(95)00385-1
1996HO11 Nucl.Phys. A600, 193 (1996) D.J.Horen, G.R.Satchler, S.A.Fayans, E.L.Trykov Microscopic Description of the Excitation of Some States in the 90,92,94,96Zr Isotopes NUCLEAR STRUCTURE 90,92,94,96Zr; calculated neutron, proton transition densities, charge distributions. Realistic self-consistent finite Fermi systems. NUCLEAR REACTIONS 90,92,94,96Zr(6Li, 6Li'), E=70 MeV; 90,92,94,96Zr(α, α'), E=35.4 MeV; 90Zr(17O, 17O'), E=84 MeV/nucleon; analyzed σ(θ). Realistic self-consistent finite Fermi systems.
doi: 10.1016/0375-9474(96)00032-2
1996JO24 Ann.Phys.(New York) 248, 134 (1996) Characteristics of Local Pion-Nucleus Potentials that are Equivalent to Kisslinger-Type Potentials NUCLEAR REACTIONS 208Pb(π+, π+), (π-, π-), E=20-291 MeV; 16O(π-, π-), E=50, 162 MeV; calculated equivalent local potentials. 16O(π+, π+), E=262 MeV; calculated σ(θ). Krell-Ericson transformation based local equivalents for nonlocal Kisslinger-type potentials.
doi: 10.1006/aphy.1996.0054
1995BE12 Phys.Lett. 344B, 67 (1995) J.R.Beene, D.J.Horen, G.R.Satchler On the ' Hindrance ' of 3- Excitations Induced by Nuclear Scattering NUCLEAR REACTIONS 60Ni, 90Zr, 120Sn, 208Pb(17O, 17O'), E=84 MeV/nucleon; calculated σ ratio, σ(θ), hadronic, hadronic+Coulomb excitation; deduced folding, deformed optical models comparison.
doi: 10.1016/0370-2693(94)01537-M
1995HO14 Phys.Rev. C52, 1554 (1995) D.J.Horen, J.R.Beene, G.R.Satchler Folded Potential Analysis of the Excitation of Giant Resonances by Heavy Ions NUCLEAR STRUCTURE 60Ni, 90Zr, 118,120,124Sn, 208Pb; calculated giant quadrupole resonance, B(λ), density distribution parameters, giant monopole resonance sum rule limits. Folded potential model. NUCLEAR REACTIONS 90Zr, 120Sn, 208Pb, 60Ni(17O, 17O'), E=84 MeV/nucleon; analyzed σ(θ) for giant resonance excitation. Folded potential model.
doi: 10.1103/PhysRevC.52.1554
1995KH03 Phys.Rev. C51, 2069 (1995) D.T.Khoa, G.R.Satchler, W.von Oertzen Folding Analysis of the Elastic 6Li + 12C Scattering: Knock-on exchange effects, energy dependence, and dynamical polarization potential NUCLEAR REACTIONS 12C(6Li, 6Li), E=99-318 MeV; analyzed σ(θ). Folded potential, density-dependent interactions.
doi: 10.1103/PhysRevC.51.2069
1995KH11 Phys.Lett. 358B, 14 (1995) D.T.Khoa, G.R.Satchler, W.von Oertzen Realistic Scenario for the Quasielastic Scattering of 11Li, 11C + 12C at E/A ≈ 60 MeV NUCLEAR REACTIONS 12C(11C, 11C), (11C, 11C'), (11Li, 11Li), (11Li, 11Li'), E=56.3-87 MeV/nucleon; analyzed total, elastic, inelastic σ(θ) data; deduced model parameters. Semi-Microscopic optical model.
doi: 10.1016/0370-2693(95)00999-2
1995LU01 Phys.Rev. C51, 635 (1995) B.J.Lund, N.P.T.Bateman, S.Utku, D.J.Horen, G.R.Satchler Isospin Character of Transitions to the 2+1 and 3-1 States of 90,92,94,96Zr NUCLEAR REACTIONS 90,92,94,96Zr(α, α), (α, α'), E=35.4 MeV; measured σ(θ); deduced model parameters. 90,92,94,96Zr levels deduced B(λ), deformation length, transition densities, isospin mixing features. Deformed optical, folding model analyses.
doi: 10.1103/PhysRevC.51.635
1995MC01 Nucl.Phys. A581, 665 (1995) Hints of a Nearside Nuclear Rainbow in Pion Scattering from 208Pb at 291 MeV ( Question ) NUCLEAR REACTIONS 208Pb(π+, π+), E=291 MeV; calculated σ(θ); deduced strong absorption role. Optical model.
doi: 10.1016/0375-9474(94)00468-3
1994HU04 Nucl.Phys. A567, 165 (1994) Halos and Rainbows: The elastic scattering of light ' exotic ' nuclei NUCLEAR REACTIONS 12C(11Li, 11Li), (11C, 11C), E=60 MeV/nucleon; calculated σ(θ); deduced halo, rainbow characteristics. Exotic nuclei, complex optical potential.
doi: 10.1016/0375-9474(94)90732-3
1994SA10 Phys.Rev. C49, 2254 (1994) Comment on ' Elastic Scattering of 318 MeV 6Li from 12C and 28Si: Unique phenomenological and folding-model potentials ' and the validity of the M3Y effective interaction NUCLEAR REACTIONS 12C(6Li, 6Li), E=210, 318 MeV; analyzed σ(θ) analyses; deduced optical potential, validity of M3Y folding interaction.
doi: 10.1103/PhysRevC.49.2254
1994SA16 Phys.Rev. C49, 3350 (1994) Comment on ' Evidence for a Nuclear Halo from 11Li Elastic Scattering Measured at 637 MeV Incident Energy on a 12C Target ' NUCLEAR REACTIONS 12C(11C, 11C), (11Li, 11Li), E ≈ 60 MeV/nucleon; analyzed σ(θ); deduced effects causing mechanisms difference.
doi: 10.1103/PhysRevC.49.3350
1994SA23 Phys.Rev. C50, 317 (1994) Examination of a ' Properly Deformed Folding Potential ' for the Analysis of Nuclear Inelastic Scattering and Comparison with True Folded Potentials NUCLEAR REACTIONS 208Pb(α, α'), E=139 MeV; calculated transition potentials; deduced explicit folding procedure necessity.
doi: 10.1103/PhysRevC.50.317
1994SA24 Nucl.Phys. A574, 575 (1994) Further Analysis of 16O + 12C Elastic Scattering at E/A = 38 MeV: How unambiguous are the potentials and phase shifts ( Question ) NUCLEAR REACTIONS 12C(16O, 16O), E=38 MeV/nucleon; analyzed σ(θ); deduced different potentials, associated phase shifts give comparable fits to data.
doi: 10.1016/0375-9474(94)90245-3
1994SA37 Nucl.Phys. A579, 241 (1994) A Simple Effective Interaction for Peripheral Heavy-Ion Collisions at Intermediate Energies NUCLEAR REACTIONS 90,92,94,96Zr(6Li, 6Li), 40Ca, 90Zr, 208Pb(12C, 12C), 40Ca, 90Zr, 208Pb(16O, 16O), 60Ni, 90,92,94,96Zr, 112,118,120,124Sn, 208Pb(17O, 17O), 120Sn, 208Pb(40Ar, 40Ar), E=10-100 MeV/nucleon; analyzed σ(θ) data; deduced nucleon-nucleon effective interaction. Folded model analysis.
doi: 10.1016/0375-9474(94)90804-4
1994VA36 Phys.Lett. 341B, 123 (1994) Where are Pion Inelastic Interactions with Nuclei Localized ( Question ) NUCLEAR REACTIONS 208Pb(π+, π+'), (π-, π-'), E=162 MeV; calculated σ(θ); deduced transition density dependence, localization features.
doi: 10.1016/0370-2693(94)90299-2
1993BE48 Phys.Rev. C48, 3128 (1993) J.R.Beene, D.J.Horen, G.R.Satchler Examination of Inconsistencies between the Deformed Potential Model and Folding Models for Analysis of Inelastic Hadron Scattering
doi: 10.1103/PhysRevC.48.3128
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
1993HO02 Phys.Rev. C47, 629 (1993) D.J.Horen, R.L.Auble, J.Gomez del Campo, G.R.Satchler, R.L.Varner, J.R.Beene, B.Lund, V.R.Brown, P.L.Anthony, V.A.Madsen Systematics of Isospin Character of Transitions to the 2+1 and 3-1 States in 90,92,94,96Zr NUCLEAR REACTIONS 90,92,94,96Zr(6Li, 6Li), (6Li, 6Li'), E=70 MeV; measured σ(θ); deduced model parameters. 90,92,94,96Zr levels deduced B(λ), neutron, proton matrix element ratio. Deformed optical model, folding model analyses.
doi: 10.1103/PhysRevC.47.629
1993HO19 Phys.Rev. C48, R2131 (1993) D.J.Horen, R.L.Auble, G.R.Satchler, J.R.Beene, I.Y.Lee, C.Y.Wu, D.Cline, M.Devlin, R.Ibbotson, M.W.Simon Lifetime of the 3-1 State and Octupole Collectivity in 96Zr NUCLEAR REACTIONS 96Zr(32S, 32S'), E=105; measured Eγ, Iγ, γ(32S)-coin. 96Zr(6Li, 6Li'), E=70 MeV; analyzed σ(θ). 96Zr level deduced T1/2, B(λ). Model comparisons.
doi: 10.1103/PhysRevC.48.R2131
1993HO22 Phys.Lett. 316B, 463 (1993) D.J.Horen, J.R.Beene, G.R.Satchler A Critique of the ' Implicit Folding Procedure ' for Analyzing Inelastic Hadron Scattering Measurements NUCLEAR STRUCTURE 208Pb, 86Kr, 90Zr; analyzed inelastic hadron scattering data analyses; deduced explicit folding procedure suitability.
doi: 10.1016/0370-2693(93)91028-L
1993MA36 Nucl.Phys. A560, 5 (1993) Temporal Nonlocality of Nuclear and Atomic Mean Fields NUCLEAR REACTIONS 208Pb(n, n), E=-10 to 60 MeV; calculated optical potential components behavior, system self energy; deduced temporary nonlocality features. Complex mean field.
doi: 10.1016/0375-9474(93)90079-D
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
1992HO12 Phys.Lett. 296B, 18 (1992) D.J.Horen, R.L.Auble, J.Gomez del Campo, R.L.Varner, J.R.Beene, G.R.Satchler, B.Lund, V.R.Brown, P.L.Anthony, V.A.Madsen Different Effects of Valence Neutrons on the Isospin Character of Transitions to the First 2+ and 3- States of 90,92,94,96Zr NUCLEAR REACTIONS 90,92,94,96Zr(6Li, 6Li'), E=70 MeV; measured σ(θ). 90,92,94,96Zr levels deduced neutron, proton matrix element ratio.
doi: 10.1016/0370-2693(92)90797-8
1992KO14 Phys.Rev.Lett. 69, 2631 (1992) J.J.Kolata, M.Zahar, R.Smith, K.Lamkin, M.Belbot, R.Tighe, B.M.Sherrill, N.A.Orr, J.S.Winfield, J.A.Winger, S.J.Yennello, G.R.Satchler, A.H.Wuosmaa Quasielastic Scattering of 11Li and 11C from 12C at 60 MeV/Nucleon NUCLEAR REACTIONS 12C(11Li, X), (11C, X), E=60 MeV/nucleon; measured quasielastic σ(θ); deduced enhanced refraction need for 11Li projectile. Coupled-channels approach.
doi: 10.1103/PhysRevLett.69.2631
1992SA02 Phys.Rev. C45, 2027 (1992) G.R.Satchler, M.K.Singham, M.B.Johnson Comment on ' Pion Scattering from 39K and 58Ni ' and Virtual Excitation Effects on Elastic Scattering NUCLEAR REACTIONS 58Ni(π+, π+), (π+, π+'), E=162 MeV; calculated σ(θ); deduced weak virtual excitation effects. Coupled-channels, phenomenological, microscopic interaction models.
doi: 10.1103/PhysRevC.45.2027
1992SA05 Nucl.Phys. A540, 533 (1992) Local Potential Model for Pion-Nucleus Scattering and π+/π- Excitation Ratios NUCLEAR REACTIONS 208Pb(π+, π+), (π-, π-), E=116-291 MeV; 40Ca, 58Ni, 90Zr, 118Sn(π+, π+), (π-, π-), E=163 MeV; 48Ca(π+, π+), (π-, π-), E=180 MeV; analyzed σ(θ). Local potential model, Woods-Saxon shape.
doi: 10.1016/0375-9474(92)90173-H
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
1991HO13 Phys.Rev. C44, 128 (1991) D.J.Horen, R.L.Auble, J.R.Beene, F.E.Bertrand, M.L.Halbert, G.R.Satchler, M.Thoennessen, R.L.Varner, V.R.Brown, P.L.Anthony, V.A.Madsen Isospin Character of Transitions to Bound States in 204,206,208Pb using Inelastic Scattering of 17O Ions NUCLEAR REACTIONS 204,206,208Pb(17O, 17O'), E=375 MeV; measured σ(θ); deduced optical model parameters. 204,206,208Pb levels deduced B(λ), neutron, proton matrix element ratio. Enriched targets. DWBA analysis. NUCLEAR STRUCTURE 204,206,208Pb; calculated B(λ), neutron, proton matrix element ratio. RPA method.
doi: 10.1103/PhysRevC.44.128
1991HO20 Phys.Rev. C44, 2385 (1991) D.J.Horen, F.E.Bertrand, J.R.Beene, G.R.Satchler, W.Mittig, A.C.C.Villari, Y.Schutz, Z.Wenlong, E.Plagnol, A.Gillibert Isospin Character of the Giant Quadrupole Transition in 124Sn NUCLEAR REACTIONS 124Sn(17O, 17O'), E=1428 MeV; measured σ(E, θ); deduced optical model parameters. 124Sn deduced Mn/Mp for GQR, B(λ), giant monopole resonance. Enriched target, DWA analysis.
doi: 10.1103/PhysRevC.44.2385
1991RO01 Phys.Lett. 254B, 25 (1991) N.Rowley, G.R.Satchler, P.H.Stelson On the ' Distribution of Barriers ' Interpretation of Heavy-Ion Fusion NUCLEAR REACTIONS 154Sm(16O, X), E(cm) ≈ 55-65 MeV; analyzed data; deduced potential barriers distribution features.
doi: 10.1016/0370-2693(91)90389-8
1991SA02 Nucl.Phys. A522, 621 (1991) G.R.Satchler, K.W.McVoy, M.S.Hussein Exploratory Studies of the Elastic Scattering of 11Li + 12C NUCLEAR REACTIONS 11Li, 12C(12C, 12C), E=85 MeV/nucleon; calculated σ(θ). Hartree-Fock densities, folding model.
doi: 10.1016/0375-9474(91)90085-K
1990HO20 Phys.Rev. C42, 2412 (1990) D.J.Horen, F.E.Bertrand, J.R.Beene, G.R.Satchler, W.Mittig, A.C.C.Villari, Y.Schutz, Z.Wenlong, E.Plagnol, A.Gillibert Isospin Character of the ' Isoscalar ' Giant Quadrupole Resonance in 118Sn NUCLEAR REACTIONS 118Sn(17O, 17O'), E=84 MeV/nucleon; measured σ(θ). 118Sn deduced resonances, J, π, neutron, proton matrix element ratio, B(λ), giant resonances Γ.
doi: 10.1103/PhysRevC.42.2412
1990JA12 Nucl.Phys. A518, 583 (1990) L.Jarczyk, B.Kamys, A.Magiera, R.Siudak, A.Strzalkowski, B.Styczen, J.Hebenstreit, W.Oelert, P.von Rossen, H.Seyfarth, G.R.Satchler Scattering of 344.5 MeV 12C Ions on 11B, 12C, 27Al, 58Ni, 90Zr and 197Au Nuclei NUCLEAR REACTIONS 11B, 12C, 27Al, 58Ni, 90Zr, 197Au(12C, 12C), 12C(12C, 12C'), E=344.5 MeV; measured σ(θ). Optical model and coupled-channels analysis.
doi: 10.1016/0375-9474(90)90148-F
1990SA08 Phys.Rev. C41, 1869 (1990) G.R.Satchler, M.A.Nagarajan, J.S.Lilley, I.J.Thompson Comment on ' Simultaneous Analyses of Elastic Scattering and Fusion Cross Sections for the 32S + 58,64Ni Systems at Energies Near the Coulomb Barrier ' NUCLEAR REACTIONS 64Ni(32S, 32S), E=88 MeV; calculated σ(θ); deduced model parameters. Extension of Udagawa et al model.
doi: 10.1103/PhysRevC.41.1869
1990TA14 Nucl.Phys. A514, 120 (1990) E.M.Takagui, G.R.Satchler, H.Takai, K.Koide, O.Dietzsch Elastic and Inelastic Scattering of 16O by 92Zr at Energies Near the Coulomb Barrier NUCLEAR REACTIONS, ICPND 92Zr(16O, 16O), (16O, 16O'), E=56 MeV; measured σ(θ), σ(E). 90Zr levels deduced B(λ). Enriched target. Coupled-channels calculations.
doi: 10.1016/0375-9474(90)90334-I
1989FR08 Nucl.Phys. A500, 399 (1989) S.H.Fricke, P.J.Hatchell, K.W.McVoy, G.R.Satchler Coulomb-Nuclear Interference in Elastic Heavy-Ion Scattering NUCLEAR REACTIONS 208Pb(12C, 12C), E=0.096-2.4 GeV; 60Ni(16O, 16O), E=150 MeV; 12C(13C, 13C), E=25 MeV; calculated σ(θ); deduced model parameters, scattering mechanism.
doi: 10.1016/0375-9474(89)90431-4
1989SA06 Nucl.Phys. A491, 413 (1989) Relation between M(n), M(p) and Hadronic Excitation Strengths when there is Strong Absorption: The (A)Zr(α, α') reactions NUCLEAR REACTIONS 90,92,96Zr(α, α'), E=35.4 MeV; analyzed σ(θ). 90,92,96Zr levels deduced neutron, proton matrix element ratio variations.
doi: 10.1016/0375-9474(89)90576-9
1989SA44 Nucl.Phys. A505, 103 (1989) Transfer Reactions and Optical Potential Ambiguities for Light Heavy-Ion Systems NUCLEAR REACTIONS 12C(12C, 12C), E=20-30 MeV/nucleon; 12C(12C, 13C), E=20-85 MeV/nucleon; calculated σ(θ); deduced potential parameters.
doi: 10.1016/0375-9474(89)90418-1
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
1988BU15 Phys.Rev. C38, 1680 (1988) B.L.Burks, M.A.G.Fernandes, G.R.Satchler, D.J.Horen, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen Optical Model and Coupled-Channels Analyses of the Elastic and Inelastic Scattering of 18O from 28Si at 352 MeV NUCLEAR REACTIONS 28Si(18O, 18O), (18O, 18O'), E=351.7 MeV; measured σ(θ). Optical model, coupled-channels analyses.
doi: 10.1103/PhysRevC.38.1680
1988EL02 Nucl.Phys. A481, 542 (1988) Further Studies of Density-Dependent Interactions for the Excitation of Collective States NUCLEAR REACTIONS 208Pb(α, α'), E=172 MeV; 50Ti(α, α'), E=104 MeV; calculated σ(θ). 208Pb(p, p'), E=65 MeV; calculated potential features, S-matrix elements. Density dependent interactions.
doi: 10.1016/0375-9474(88)90344-2
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
1987BE03 Phys.Rev.Lett. 58, 455 (1987) M.Beckerman, R.L.Auble, F.E.Bertrand, J.L.Blankenship, B.L.Burks, C.W.Glover, R.O.Sayer, G.R.Satchler, D.Shapira, R.L.Varner Quasielastic Transfer of a Neutron between 58Ni and 208Pb at Bombarding Energies of 598 and 1011 MeV NUCLEAR REACTIONS 208Pb(58Ni, 59Ni), (58Ni, 57Ni), E=598, 1011 MeV; measured σ(E(59Ni)), σ(E(57Ni)), σ(θ). Enriched targets, tof. DWBA analyses.
doi: 10.1103/PhysRevLett.58.455
1987BE23 Phys.Rev. C36, 657 (1987) M.Beckerman, R.L.Auble, F.E.Bertrand, J.L.Blankenship, B.L.Burks, M.A.G.Fernandes, C.W.Glover, E.E.Gross, D.J.Horen, R.O.Sayer, G.R.Satchler, D.Shapira, Y.Sugiyama, R.L.Varner Elastic and Inelastic Scattering of 58Ni + 208Pb at Bombarding Energies from 598 to 1011 MeV NUCLEAR REACTIONS 208Pb(58Ni, 58Ni), (58Ni, 58Ni'), E=598-1011 MeV; measured σ(E), σ(θ). 208Pb, 58Ni levels deduced B(E2), Coulomb deformation constants. Optical model, DWBA, coupled-channels calculations.
doi: 10.1103/PhysRevC.36.657
1987HO18 Z.Phys. A328, 189 (1987) D.J.Horen, M.A.G.Fernandes, G.R.Satchler, B.L.Burks, R.L.Auble, F.E.Bertrand, E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira Transfer Reactions at High Energy and Ambiguities in Heavy-Ion Potentials NUCLEAR REACTIONS 28Si(16O, 16O), E=56, 351.7 MeV; calculated σ(θ); deduced optical potential parameters. 28Si(18O, 17O), E=352 MeV; 28Si(18O, 19F), E=352 MeV; analyzed data; deduced model parameters. 29Si, 29Al levels deduced spectroscopic factors.
1987SA38 Ann.Phys.(New York) 178, 110 (1987) G.R.Satchler, M.A.Nagarajan, J.S.Lilley, I.J.Thompson Heavy-Ion Fusion: Channel-coupling effects, the barrier penetration model, and the threshold anomaly for heavy-ion potentials NUCLEAR REACTIONS 208Pb(16O, X)(16O, 16O), (16O, 16O'), E=80, 102 MeV; 90Zr(46Ti, X), (46Ti, 46Ti), (46Ti, 46Ti'), E(cm)=105 MeV; calculated elastic, absorption, fusion, total σ. Channel-coupling effects, barrier penetration model.
doi: 10.1016/S0003-4916(87)80015-5
1987SA39 Nucl.Phys. A472, 215 (1987) Isospin and Macroscopic Models for the Excitation of Giant Resonances and Other Collective States NUCLEAR REACTIONS 116Sn(α, α'), E=129 MeV; 208Pb(α, α'), E=172 MeV; calculated σ(θ). Isospin, macroscopic models.
doi: 10.1016/0375-9474(87)90208-9
1986FE03 Phys.Rev. C33, 1971 (1986) M.A.G.Fernandes, B.l.Burks, D.J.Horen, G.R.Satchler, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, D.Shapira, T.P.Sjoreen One-Nucleon-Transfer Reactions Induced by 352-MeV 18O on 28Si NUCLEAR REACTIONS 28Si(18O, 17O), (18O, 19F), E=352 MeV; measured σ(θ); deduced model parameters. 29Si, 27Al levels deduced single-nucleon transfer spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.33.1971
1986HO27 Phys.Lett. 181B, 38 (1986) D.J.Horen, B.L.Burks, M.A.G.Fernandes, R.L.Auble, F.E.Bertrand, J.L.Blankenship, J.L.C.Ford, Jr., E.E.Gross, D.C.Hensley, R.O.Sayer, G.R.Satchler, D.Shapira, T.P.Sjoreen, F.Petrovich Investigation of the One-Step Direct Contribution to the 28Si(18O, 18F)28Al Reaction at 19.6 MeV/Nucleon NUCLEAR REACTIONS, MECPD 28Si(18O, 18F), E=352 MeV; measured σ(E(18F)), σ(θ); deduced reaction mechanism. Magnetic spectrometer system, particle identification ionization chamber. Microscopic DWIA calculations.
doi: 10.1016/0370-2693(86)91250-5
1986MA04 Nucl.Phys. A449, 354 (1986) Causality and the Threshold Anomaly of the Nucleus-Nucleus Potential NUCLEAR REACTIONS 40Ca(16O, 16O), E=38-214 MeV; 208Pb(16O, 16O), E=60-240 MeV; calculated potential volume integrals; deduced threshold anomaly causality principle relationship.
doi: 10.1016/0375-9474(86)90009-6
1986MA35 Nucl.Phys. A456, 134 (1986) Radial and Energy Dependence of the Dispersive Contributions to the α + 16O and α + 40Ca Potentials near the Threshold Anomaly NUCLEAR REACTIONS 16O(α, α), E=20-80 MeV; 40Ca(α, α), E=58-72 MeV; calculated nucleus-nucleus potential characteristics; deduced dispersion contributions radial, energy dependences.
doi: 10.1016/0375-9474(86)90370-2
1986MC07 Nucl.Phys. A455, 118 (1986) K.W.McVoy, H.M.Khalil, M.M.Shalaby, G.R.Satchler Asymmetric Deflection Functions and the Extinction of Rainbows: A comparison of α-particle scattering from 40 and 44Ca NUCLEAR REACTIONS 12C(12C, 12C), E=288.6 MeV; calculated deflection function, σ(θ). 40Ca(α, α), E=46-62 MeV; 44Ca(α, α), E=49.5-100 MeV; calculated σ(θ), deflection function; deduced nuclear rainbow evidence.
doi: 10.1016/0375-9474(86)90346-5
1986NA06 Phys.Lett. 173B, 29 (1986) Comments on the Barrier Penetration Model for Heavy-Ion Fusion NUCLEAR REACTIONS 208Pb(16O, X), E=80 MeV; calculated fusion σ vs l. Barrier penetration model.
doi: 10.1016/0370-2693(86)91224-4
1985EL02 Nucl.Phys. A438, 525 (1985) A Density-Dependent Interaction in the Folding Model for Heavy-Ion Potentials NUCLEAR REACTIONS 40Ca(12C, 12C), E=45, 51 MeV; 208Pb(12C, 12C), E=96 MeV; 90Zr(12C, 12C), E=98 MeV; 40Ca(16O, 16O), E=74.4 MeV; 60Ni(16O, 16O), E=61.4, 141.7 MeV; 208Pb(16O, 16O), E=78-312.6 MeV; 60Ni, 120Sn, 208Pb(40Ar, 40Ar), E=1.76 GeV; 40Ca(40Ca, 40Ca), E=143.6 MeV; analyzed data; deduced interaction, optical potential parameters. Folding model, density dependent interactions.
doi: 10.1016/0375-9474(85)90391-4
1985EL06 Nucl.Phys. A441, 157 (1985) Some Optical-Model Analyses of the Elastic Scattering of 40Ar at 1760 MeV NUCLEAR REACTIONS 60Ni, 120Sn, 208Pb(40Ar, 40Ar), E=1760 MeV; analyzed σ(θ); deduced real potential energy dependence. Woods-Saxon, folding model potentials.
doi: 10.1016/0375-9474(85)90173-3
1985NA01 Phys.Rev.Lett. 54, 1136 (1985) M.A.Nagarajan, C.C.Mahaux, G.R.Satchler Dispersion Relation and the Low-Energy Behavior of the Heavy-Ion Optical Potential NUCLEAR REACTIONS 208Pb(16O, 16O), E=80-220 MeV; calculated potential parameter energy dependence.
doi: 10.1103/PhysRevLett.54.1136
1985SH21 Nucl.Phys. A442, 469 (1985) Optical Potential Ambiguities and Fusion Cross Sections for Heavy Ions NUCLEAR REACTIONS, ICPND 26Mg(32S, 32S), E(cm) ≈ 18-32 MeV; calculated absorption σ(E); deduced imaginary potential role.
doi: 10.1016/S0375-9474(85)80027-0
1984EL09 Phys.Lett. 146B, 389 (1984) One Effect of using Relativistic Kinematics in the Analysis of Heavy-Ion Elastic Scattering NUCLEAR REACTIONS 208Pb, 120Sn, 60Ni(40Ar, 40Ar), E=1760 MeV; 208Pb(12C, 12C), E=86 MeV/nucleon; calculated ion-ion potential laboratory to center-of-mass motion system transformation dependence. Optical model, semi-classical description.
doi: 10.1016/0370-2693(84)90145-X
1984FU10 Nucl.Phys. A427, 545 (1984) C.B.Fulmer, G.R.Satchler, K.A.Erb, D.C.Hensley, R.L.Auble, J.R.Ball, F.E.Bertrand, E.E.Gross Elastic and Inelastic Scattering of 158 MeV 9Be Ions NUCLEAR REACTIONS 12C, 16O, 26Mg, 27Al, 40Ca, 60Ni, 197Au(9Be, 9Be); 12C, 26Mg, 60Ni(9Be, 9Be'), E=158 MeV; measured σ(θ); deduced optical potential parameters. Distorted wave calculations.
doi: 10.1016/0375-9474(84)90230-6
1984GU22 Nucl.Phys. A430, 485 (1984) M.W.Guidry, R.E.Neese, C.R.Bingham, L.L.Riedinger, J.A.Vrba, I.Y.Lee, N.R.Johnson, G.R.Satchler, P.A.Butler, R.Donangelo, J.O.Rasmussen, D.L.Hillis, H.H.Kluge Heavy-Ion Inelastic Scattering from Deformed Nuclei NUCLEAR REACTIONS 162Dy(16O, 16O'), E=50-68 MeV; 232Th(86Kr, 86Kr'), E=350-450 MeV; 160Gd(40Ar, 40Ar'), E=100-170 MeV; 162Dy(40Ar, 40Ar'), E=120-170 MeV; 180Hf(40Ar, 40Ar'), E=135-175 MeV; 156Gd, 164Dy(40Ar, 40Ar'), E=120-160 MeV; measured γ(particle)-coin, σ(E); deduced ion-ion potentials. Gamma spectroscopy. Classical limit.
doi: 10.1016/0375-9474(84)90050-2
1984KO15 Phys.Rev. C30, 403 (1984) Potential Models and Resonances in the 16O + 28Si System NUCLEAR REACTIONS 28Si(16O, 16O), E=29.4-45 MeV; analyzed σ(E, θ); deduced optical model potential, phase shifts, no resonances.
doi: 10.1103/PhysRevC.30.403
1984KO20 Nucl.Phys. A425, 205 (1984) A.M.Kobos, B.A.Brown, R.Lindsay, G.R.Satchler Folding-Model Analysis of Elastic and Inelastic α-Particle Scattering using a Density-Dependent Force NUCLEAR REACTIONS 40Ca(α, α), E=29, 100 MeV; 90Zr(α, α), E=40, 59.1, 79.5, 99.5, 118 MeV; 208Pb(α, α'), E=25, 139 MeV; 58Ni(α, α'), E=139 MeV; 46,48,50Ti(α, α'), E=140 MeV; calculated σ(θ). Folding model analysis.
doi: 10.1016/0375-9474(84)90073-3
1984KO30 Nucl.Phys. A427, 589 (1984) A Global Optical Potential Analysis of 16O + 28Si Elastic Scattering NUCLEAR REACTIONS 28Si(16O, 16O), E(cm)=18-35 MeV; calculated σ(θ), σ(E); deduced potential parameters, scattering amplitude components. Global optical model.
doi: 10.1016/0375-9474(84)90232-X
1984MA17 Z.Phys. A316, 35 (1984) A.D.MacKellar, G.R.Satchler, C.-Y.Wong An Exploratory Study of Antiproton-Nucleus Scattering NUCLEAR REACTIONS 16O(p-bar, p-bar), E=45, 175 MeV; calculated σ(θ).12C(p-bar, p-bar), E=50-200 MeV; calculated reaction σ(E).208Pb(p-bar, p-bar), E=70 MeV; calculated reaction σ vs real, imaginary potential parameters. Antiproton-atom data derived potentials.
doi: 10.1007/BF01415658
1984MC06 Nucl.Phys. A417, 157 (1984) Nuclear Rainbows and Heavy-Ion Scattering NUCLEAR REACTIONS 12C(12C, 12C), E ≈ 200 MeV; 90Zr(α, α), E=79.5 MeV; calculated σ(θ); deduced nuclear rainbow effect. Semi-classical, strong absorption interpretation.
doi: 10.1016/0375-9474(84)90328-2
1984SA04 Phys.Lett. 134B, 7 (1984) Comment on J-Dependence in (α, d) Transfer Reactions NUCLEAR REACTIONS 208Pb(α, d), E not given; calculated σ(θ); deduced simultaneous, sequential transfer interference J-dependence. Second-order DWBA amplitudes.
doi: 10.1016/0370-2693(84)90972-9
1984WO01 Phys.Rev. C29, 574 (1984) C.-Y.Wong, A.K.Kerman, G.R.Satchler, A.D.MacKellar Ambiguity in Antiproton-Nucleus Potentials from Antiprotonic-Atom Data NUCLEAR REACTIONS 12C(p-bar, p-bar), E=70 MeV; calculated σ(θ); deduced potential ambiguities. Optical potentials from p-bar atomic data.
doi: 10.1103/PhysRevC.29.574
1983CA15 Nucl.Phys. A403, 93 (1983) B.Castel, G.R.Satchler, L.Zamick, I.P.Johnstone Core-Polarization and Open-Shell Effects in E6 Transitions NUCLEAR STRUCTURE 50,52Cr, 52Fe; analyzed E6 decay negative proton polarization charge; deduced quadrupole deformation role. Collective model core polarization, open shell approaches.
doi: 10.1016/0375-9474(83)90190-2
1983GO13 Phys.Rev. C28, 952 (1983) J.Gomez del Campo, G.R.Satchler Nucleus-Nucleus Potential at Close Contact from Fusion at ' High ' Energies NUCLEAR REACTIONS 14N, 16,17O(10B, X), 16O(11B, X), 14,15N, 27Al(12C, X), 27Al, 40Ca(16O, X), 27Al, 20Ne(20Ne, X), 40Ca(40Ca, X), E not given; compiled σ(fusion) data analyses; deduced critical radius, potential corelation.
doi: 10.1103/PhysRevC.28.952
1983GR10 Nucl.Phys. A401, 362 (1983) E.E.Gross, J.R.Beene, K.A.Erb, M.P.Fewell, D.Shapira, M.J.Rhoades-Brown, G.R.Satchler, C.E.Thorn Elastic and Inelastic Scattering of 120 MeV 18O from 208Pb and the Spin Alignment of the 2+ State of 18O NUCLEAR REACTIONS 208Pb(18O, 18O), (18O, 18O'), E=120 MeV; measured σ(E(18O), θ), Doppler broadened line shapes. 18O deduced substate population, excited state hexadecapole moment. Enriched target. Coupled-channels analysis.
doi: 10.1016/0375-9474(83)90533-X
1983KO06 Nucl.Phys. A395, 248 (1983) A.M.Kobos, G.R.Satchler, R.S.Mackintosh An Optical Potential Description of 16O + 28Si Elastic Scattering NUCLEAR REACTIONS 28Si(16O, 16O), E(cm)=21.1-34.8 MeV; analyzed σ(θ); deduced optical model, potential parameters. Double folded potential, model independent correction term.
doi: 10.1016/0375-9474(83)90099-4
1983SA03 Nucl.Phys. A394, 349 (1983) ' Wine-Bottle ' Optical Potentials and the Inelastic Scattering of Protons near 200 MeV NUCLEAR REACTIONS 208Pb(p, p), (p, p')E=200 MeV; 40Ca(p, p), (p, p'), E=181 MeV; calculated σ(θ); deduced equivalent potential parameters. Woods-Saxon plus derivative term.
doi: 10.1016/0375-9474(83)90108-2
1983SA20 Phys.Lett. 128B, 147 (1983) G.R.Satchler, C.B.Fulmer, R.L.Auble, J.B.Ball, F.E.Bertrand, K.A.Erb, E.E.Gross, D.C.Hensley Refractive Effects in 9Be Scattering and Nuclear Rainbow Ghosts NUCLEAR REACTIONS 12C, 16O(9Be, 9Be), E=158 MeV; measured σ(θ); deduced optical model parameters, nuclear rainbow, refractive effects. Optical model.
doi: 10.1016/0370-2693(83)90378-7
1983SA33 Nucl.Phys. A411, 144 (1983) Properties of the Transition Amplitude for Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 208Pb(α, d), E not given; calculated σ(θ). 210Bi levels deduced population J-dependence. Two-nucleon transfer, additional angular momemntum transfer sources.
doi: 10.1016/0375-9474(83)90512-2
1982FU09 Nucl.Phys. A385, 83 (1982) C.B.Fulmer, S.Mukhopadhyay, G.R.Satchler, R.L.Auble, J.B.Ball, F.E.Bertrand, E.E.Gross, D.C.Hensley Elastic and Inelastic Scattering of 79.5 MeV 11B and 87.5 MeV 10B Ions NUCLEAR REACTIONS 24,25,26Mg, 27Al, 59Co, 60Ni, 197Au(11B, 11B), 24,26Mg(11B, 11B'), E=79.5 MeV; 24,25Mg, 60Ni(10B, 10B), 24Mg, 60Ni(10B, 10B'), E=87.5 MeV; measured σ(θ); deduced optical model parameters. 26Mg(11B, 11B), (11B, 10B), (11B, 12B), (11B, 13C), (11B, 12C), (11B, 11C), (11B, 9Be), (11B, 10Be), (11B, 7Be), (11B, 7Li), (11B, 6Li), (11B, 8Li), E=79.6 MeV; measured σ(θ) vs reaction product E.
doi: 10.1016/0375-9474(82)90491-2
1982KO19 Nucl.Phys. A384, 65 (1982) A.M.Kobos, B.A.Brown, P.E.Hodgson, G.R.Satchler, A.Budzanowski Folding Model Analysis of α-Particle Elastic Scattering with a Semirealistic Density-Dependent Effective Interaction NUCLEAR REACTIONS 40Ca, 46,48,50Ti, 58Ni, 90Zr, 208Pb(α, α), E=140 MeV; 58,60,62,64Ni(α, α), E=172 MeV: analyzed σ(θ). Folding model, density-dependent effective interaction.
doi: 10.1016/0375-9474(82)90305-0
1982NA22 Phys.Rev.Lett. 49, 1899 (1982) D-State Effects and J Dependence in (α, d) Reactions NUCLEAR REACTIONS, ICPND 208Pb(α, d), E=48 MeV; calculated angle integrated σ; deduced α-particle D-state effects. DWBA analysis.
doi: 10.1103/PhysRevLett.49.1899
1982NE04 Nucl.Phys. A385, 349 (1982) G.A.Needham, F.P.Brady, D.H.Fitzgerald, J.L.Romero, J.L.Ullmann, J.W.Watson, C.Zanelli, N.S.P.King, G.R.Satchler Excitation of Analog Isovector Giant Resonances via the (n, p) Reaction on 14N and 16O at 60 MeV NUCLEAR REACTIONS 14N, 16O(n, p), E=60 MeV; measured σ(θ). 14C, 16N deduced GDR analog excitation. Natural targets. DWBA analysis.
doi: 10.1016/0375-9474(82)90092-6
1982WO02 Z.Phys. A305, 179 (1982) R.Wolf, O.Tanimura, U.Mosel, G.R.Satchler Influence of Strongly Coupled Inelastic Excitations on the Optical Potential for 12C + 12C NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E(cm)=37.12, 46.9, 63.35 MeV; calculated σ(θ); deduced local equivalent, nonlocal heavy ion potentials. Exact Green's function, coupled inelastic excitations, Fesbach projection formalism.
doi: 10.1007/BF01415027
1981BR01 J.Phys.(London) G7, 43 (1981) The Role of the Attractive Nuclear Potential in Determining Reaction Cross Sections NUCLEAR REACTIONS 40Ca(α, X), E=0.03-1.37 GeV; 12C(12C, X), E=0.07-10.44 GeV; calculated σ(reaction, E), transmission coefficients; deduced role of attractive nuclear potential. Woods-Saxon, Woods-Saxon squared potentials.
doi: 10.1088/0305-4616/7/1/009
1981EC01 Phys.Rev. C23, 228 (1981) J.S.Eck, T.R.Ophel, P.D.Clark, D.C.Weisser, G.R.Satchler Elastic and Inelastic Scattering Measurements for the 24Mg + 208Pb and 28Si + 208Pb Systems NUCLEAR REACTIONS 208Pb(24Mg, 24Mg), (24Mg, 24Mg'), E=145 MeV; 206Pb(28Si, 28Si), (28Si, 28Si'), E=162 MeV; measured σ(θ). 208,206Pb level deduced deformation β2. Optical model, coupled-channel analyses.
doi: 10.1103/PhysRevC.23.228
1981FU04 Nucl.Phys. A356, 235 (1981) C.B.Fulmer, G.R.Satchler, E.E.Gross, F.E.Bertrand, C.D.Goodman, D.C.Hensley, J.R.Wu, N.M.Clarke, M.F.Steeden Elastic and Inelastic Scattering of 88 MeV 6Li Ions NUCLEAR REACTIONS 24,25,26Mg, 27Al, 40,48Ca, 59Co, 60Ni, 197Au, 206,208Pb(6Li, 6Li), 24,26Mg, 60Ni(6Li, 6Li'), E=88 MeV; measured σ(θ); deduced optical potentials. DWBA, coupled-channels calculations.
doi: 10.1016/0375-9474(81)90125-1
1980BE50 Phys.Rev. C22, 1832 (1980) F.E.Bertrand, G.R.Satchler, D.J.Horen, J.R.Wu, A.D.Bacher, G.T.Emery, W.P.Jones, D.W.Miller, A. van der Woude Giant Multipole Resonances from Inelastic Scattering of 152-MeV Alpha Particles NUCLEAR REACTIONS 208Pb, 120Sn, 90Zr, 58Ni, 46Ti(α, α), (α, α'), E=152 MeV; measured σ(Eα, θ). 46Ti, 58Ni, 90Zr, 120Sn, 208Pb deduced GQR, giant monopole resonances, Γ, L, T, β(L), B(λ), EWSR. Folding model analysis.
doi: 10.1103/PhysRevC.22.1832
1980CA06 Phys.Lett. 91B, 185 (1980) B.Castel, G.R.Satchler, K.Goeke Core Polarization Effects and Giant Quadrupole Resonances in the A = 90 Region NUCLEAR STRUCTURE A ≈ 90; calculated proton, neutron effective charges. Linearized Hartree-Fock, macroscopic GQR excitation models.
doi: 10.1016/0370-2693(80)90426-8
1980EC04 Nucl.Phys. A341, 178 (1980) J.S.Eck, T.R.Ophel, P.D.Clark, D.C.Weisser, G.R.Satchler Inelastic Scattering of 9Be Projectiles to Low-Lying Collective States in 28Si and 40Ca at E(9Be) = 45 and 60 MeV NUCLEAR REACTIONS 40Ca, 28Si(9Be, 9Be'), E=45, 60 MeV; measured σ(θ). DWBA, double-folding model potential.
doi: 10.1016/0375-9474(80)90369-3
1980SA17 Phys.Rev. C22, 919 (1980) Elastic and Inelastic Scattering of 6Li at About 74 MeV and the Folding Model NUCLEAR REACTIONS 58Ni, 90Zr, 124Sn, 208Pb(6Li, 6Li), E=73.7 MeV; 58Ni(6Li, 6Li'), E=71 MeV; calculated σ(θ); deduced folding model parameters.
doi: 10.1103/PhysRevC.22.919
1980SA25 Nucl.Phys. A346, 179 (1980) G.R.Satchler, M.L.Halbert, R.G.Stokstad, R.M.Devries, D.A.Goldberg, J.G.Cramer Energy Dependence in 12C + 28Si Elastic Scattering NUCLEAR REACTIONS 28Si(12C, 12C), E=131.5 MeV; measured σ(θ); deduced optical model potentials. Enriched targets. Optical model analyses.
doi: 10.1016/0375-9474(80)90496-0
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