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Search: Author = G.R.Satchler

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1239.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1535.

2000KH06      Nucl.Phys. A668, 3 (2000)

D.T.Khoa, G.R.Satchler

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1000.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1336.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0999.

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0779.

1997BR30      Phys.Rep. 285, 143 (1997)

M.E.Brandan, G.R.Satchler

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1997SA03      Phys.Rev. C55, 285 (1997)

G.R.Satchler, D.T.Khoa

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
Citations: PlumX Metrics

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
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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
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1996JO24      Ann.Phys.(New York) 248, 134 (1996)

M.B.Johnson, G.R.Satchler

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
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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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1205.

1995MC01      Nucl.Phys. A581, 665 (1995)

K.W.McVoy, G.R.Satchler

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
Citations: PlumX Metrics

1994HU04      Nucl.Phys. A567, 165 (1994)

M.S.Hussein, G.R.Satchler

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
Citations: PlumX Metrics

1994SA10      Phys.Rev. C49, 2254 (1994)

G.R.Satchler, W.G.Love

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
Citations: PlumX Metrics

1994SA16      Phys.Rev. C49, 3350 (1994)

G.R.Satchler, M.S.Hussein

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1994VA36      Phys.Lett. 341B, 123 (1994)

R.L.Varner, Jr., G.R.Satchler

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
Citations: PlumX Metrics

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1176.

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
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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
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1993MA36      Nucl.Phys. A560, 5 (1993)

C.Mahaux, G.R.Satchler

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
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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
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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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1148.

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
Citations: PlumX Metrics

1992SA05      Nucl.Phys. A540, 533 (1992)


Local Potential Model for Pion-Nucleus Scattering and 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
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1991BR08      Phys.Lett. 256B, 311 (1991)

M.E.Brandan, G.R.Satchler

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
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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
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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
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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
Citations: PlumX Metrics

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
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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
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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
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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
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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
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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
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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
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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
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1988BR29      Nucl.Phys. A487, 477 (1988)

M.E.Brandan, G.R.Satchler

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
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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
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1988EL02      Nucl.Phys. A481, 542 (1988)

M.El-Azab Farid, G.R.Satchler

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
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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
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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
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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
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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
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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
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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
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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
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1986MA04      Nucl.Phys. A449, 354 (1986)

C.Mahaux, H.Ngo, G.R.Satchler

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
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1986MA35      Nucl.Phys. A456, 134 (1986)

C.Mahaux, H.Ngo, G.R.Satchler

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
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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
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1986NA06      Phys.Lett. 173B, 29 (1986)

M.A.Nagarajan, G.R.Satchler

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
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1985EL02      Nucl.Phys. A438, 525 (1985)

M.El-Azab Farid, G.R.Satchler

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
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1985EL06      Nucl.Phys. A441, 157 (1985)

M.El-Azab Farid, G.R.Satchler

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
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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
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1985SH21      Nucl.Phys. A442, 469 (1985)

M.M.Shalaby, G.R.Satchler

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
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1984EL09      Phys.Lett. 146B, 389 (1984)

M.El-Azab Farid, G.R.Satchler

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
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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
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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
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1984KO15      Phys.Rev. C30, 403 (1984)

A.M.Kobos, G.R.Satchler

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
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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
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1984KO30      Nucl.Phys. A427, 589 (1984)

A.M.Kobos, G.R.Satchler

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
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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
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1984MC06      Nucl.Phys. A417, 157 (1984)

K.W.McVoy, G.R.Satchler

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
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1984SA04      Phys.Lett. 134B, 7 (1984)

G.R.Satchler, W.T.Pinkston

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
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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
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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
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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
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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
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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
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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
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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
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1983SA33      Nucl.Phys. A411, 144 (1983)

G.R.Satchler, W.T.Pinkston

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
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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
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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
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1982NA22      Phys.Rev.Lett. 49, 1899 (1982)

M.A.Nagarajan, G.R.Satchler

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12786.

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
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1981BR01      J.Phys.(London) G7, 43 (1981)

D.M.Brink, G.R.Satchler

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
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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
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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
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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
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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
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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
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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
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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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