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Search: Author = L.J.Goldfarb

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1987BA68      Phys.Rev. C36, 1807 (1987)

A.J.Baltz, L.J.B.Goldfarb

Spatial Development of Inelastic Scattering and Particle Transfer Cross Sections in very Heavy Ion Reactions

NUCLEAR REACTIONS ²³⁸U(²⁰⁸Pb, ²⁰⁸Pb'), E=1.12 GeV; calculated inelastic σ(θ). Quantal method.

doi: 10.1103/PhysRevC.36.1807
Citations: PlumX Metrics

1987GO14      Nucl.Phys. A465, 529 (1987)

L.J.B.Goldfarb

Systematic Features of the Statistical-Fission Model

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁶O, X), (¹⁶O, F), E=90, 110, 130 MeV; ²³²Th(¹⁶O, X), (¹⁶O, F), E=90, 95, 120 MeV; ²⁰⁸Pb(¹⁹F, X), (¹⁹F, F), E=110, 135 MeV; ²⁰⁸Pb(²⁴Mg, X), (²⁴Mg, F), E=145, 160 MeV; ²⁰⁸Pb(²⁸Si, X), (²⁸Si, F), E=160, 180 MeV; ¹⁹⁷Au(³²S, F), (³²S, X), E=185, 198 MeV; ²⁰⁸Pb(³²S, X), (³²S, F), E=210, 219 MeV; calculated fission, fusion σ(fragment θ), anisotropy. Statistical model.

doi: 10.1016/0375-9474(87)90363-0
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1985GO01      Phys.Lett. 150B, 62 (1985)

L.J.B.Goldfarb

Densities of Calcium Nuclei as Deduced by Analyses of ¹⁶O Scattering

NUCLEAR REACTIONS ^40,42,44,48Ca(¹⁶O, ¹⁶O), E=56, 60 MeV; analyzed potential, nuclear size parameters. ^40,42,44,48Ca deduced densities.

doi: 10.1016/0370-2693(85)90138-8
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1984GO13      Nucl.Phys. A429, 365 (1984)

L.J.B.Goldfarb

A Method of Probing Nuclear Skin Thicknesses by Analyses of Heavy-Ion Scattering

NUCLEAR REACTIONS ⁴⁸Ca, ⁶⁰Ni, ¹²⁰Sn, ²⁰⁸Pb(¹⁶O, ¹⁶O), E=61.4 MeV; analyzed σ(θ); deduced nuclear skin thickness, density parameter dependences. Real interaction global description.

doi: 10.1016/0375-9474(84)90213-6
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1983GO09      Nucl.Phys. A401, 557 (1983)

L.J.B.Goldfarb, Y.K.Gambhir

Essential Features of the Folding Potential in Heavy-Ion Scattering

NUCLEAR REACTIONS ⁴⁸Ca, ⁶⁰Ni, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb(¹⁶O, ¹⁶O), (¹⁶O, X), E ≈ 20 MeV; calculated real potential; deduced nucleon density, effective nucleon-nucleon interaction role. Folding model.

doi: 10.1016/0375-9474(83)90365-2
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1982GO10      Phys.Lett. 115B, 166 (1982)

L.J.B.Goldfarb

Sequential and Simultaneous Transfer in the Reactions ¹⁸O(p, t)¹⁶O, ⁴⁸Ca(t, p)⁵⁰Ca and ⁹⁰Zr(t, p)⁹²Zr

NUCLEAR REACTIONS ¹⁸O(p, t), E=20 MeV; ⁴⁸Ca(t, p), E=12.08 MeV; ⁹⁰Zr(t, p), E=20 MeV; analyzed σ(θ); deduced sequential transfer, spin-orbit distortion effects. Coupled-channels analysis.

doi: 10.1016/0370-2693(82)90636-0
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1981GO14      Phys.Lett. 104B, 103 (1981)

L.J.B.Goldfarb

The Influence of g Bosons on the Interacting Boson Model

NUCLEAR STRUCTURE ¹⁶⁸Er, ¹⁵⁶Gd; calculated band-head energies. Interacting boson model, SU(3) limit, g bosons.

doi: 10.1016/0370-2693(81)90569-4
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1980GO08      Nucl.Phys. A341, 494 (1980)

L.J.B.Goldfarb, P.Nagel

Effects of Local Density Dependence on the Scattering of Heavy Ions and Alpha Particles

NUCLEAR REACTIONS ⁴⁰Ca(α, α), E=29 MeV; ⁵⁸Ni(α, α), E=50.2 MeV; ⁶⁰Ni(¹⁶O, ¹⁶O), E=61.4 MeV; ²⁸Si(¹⁶O, ¹⁶O), E=53 MeV; ⁴⁰Ca, ²⁰⁸Pb(¹⁶O, ¹⁶O), ²⁰⁸Pb(α, α), E not given; calculated σ(θ); deduced local density dependence. Double-folding calculations.

doi: 10.1016/0375-9474(80)90380-2
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1980SI12      Nucl.Phys. A342, 312 (1980)

S.J.Singleton, V.Managoli, L.J.B.Goldfarb

Non-Orthogonality Effects in Heavy-Ion Transfer Reactions

NUCLEAR REACTIONS ¹³C(¹⁶O, ¹⁷O), E=30-60 MeV; ²⁹Si(¹⁶O, ¹⁷O), E=73.5 MeV; calculated σ(θ). Coupled channel treatment, channel nonorthogonality.

doi: 10.1016/0375-9474(80)90258-4
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1976DU04      Nucl.Phys. A269, 443 (1976)

J.L.Durell, P.J.A.Buttle, L.J.B.Goldfarb, W.R.Phillips, G.D.Jones, B.W.Hooton, M.Ivanovich

The Calibration of Sub-Coulomb Heavy-Ion Transfer Reactions

NUCLEAR REACTIONS ¹³C(¹⁶O, ¹⁷O), E=13, 14 MeV; measured σ(E(¹⁷O), θ). ¹³C(¹⁸O, ¹⁹O), E=12.5-14.5 MeV; measured σ(θ). ¹⁸O(¹⁷O, ¹⁶O), E=14.2-15.3 MeV; measured σ(E). ¹³C, ^17,19O deduced rms radii of single-particle orbitals, rms radii of neutron excess.

doi: 10.1016/0375-9474(76)90692-8
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1976FE01      Phys.Rev. C13, 1151 (1976)

D.H.Feng, A.R.Barnett, L.J.B.Goldfarb

Systematics of Coulomb Excitation with Limited Effects from Nuclear Distortion

NUCLEAR REACTIONS ¹⁵²Sm, ²⁰⁸Pb, ²³⁴U(α, α'), E ≈ 15 MeV; measured calculated σ. Coulomb excitation systematics.

doi: 10.1103/PhysRevC.13.1151
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1975GO14      Nukleonika 20, 345 (1975)

L.J.B.Goldfarb

Aspects of Transfer Reactions between Heavy Ions

NUCLEAR REACTIONS ⁸⁸Sr(¹⁶O, ¹⁵N), E=44 MeV; ⁴⁸Ca(¹⁷O, ¹⁶O), E=28 MeV; ²⁰⁸Pb(¹⁶O, ¹⁷O), E=80 MeV; ⁴⁰Ca(¹³C, ¹⁴N), ¹²C(¹⁴N, ¹³C), E=78 MeV; analyzed σ.

1974BA10      Phys.Lett. 48B, 290 (1974)

A.R.Barnett, D.H.Feng, L.J.B.Goldfarb

A Quantal Treatment of Octupole Coulomb-Nuclear Interference

NUCLEAR REACTIONS ²⁰⁸Pb(α, α'), E=21, 22 MeV; measured σ(θ), calculated nuclear-Coulomb interference.

doi: 10.1016/0370-2693(74)90592-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0519.

1974GO02      Nucl.Phys. A218, 396 (1974)

L.J.B.Goldfarb, K.Takeuchi

Effects of Non-Orthogonality and Virtual Excitations in Direct Reactions (II)

NUCLEAR REACTIONS ⁴⁰Ca(d, p), E=10-40 MeV; measured nothing, calculated σ(θ).

doi: 10.1016/0375-9474(74)90012-8
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1974GO03      Nucl.Phys. A218, 405 (1974)

L.J.B.Goldfarb, K.Takeuchi

Effects of Non-Orthogonality and Virtual Excitations in Direct Reactions (III)

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁶O, ¹⁷O); measured nothing, calculated σ(θ).

doi: 10.1016/0375-9474(74)90013-X
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1973BO44      Phys.Lett. 47B, 203 (1973)

D.P.Bouldin, L.J.B.Goldfarb

Improvements in the Form Factors for Heavy-Ion Transfer Reactions

NUCLEAR REACTIONS ⁴⁸Ca(¹⁷O, ¹⁶O), E=29.5 MeV; ⁸⁸Sr(¹⁶O, ¹⁵N), E=44-59 MeV; calculated σ(θ).

doi: 10.1016/0370-2693(73)90708-9
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1972GO04      Nucl.Phys. A181, 609 (1972)

L.J.B.Goldfarb, K.Takeuchi

Effects of Non-Orthogonality and Virtual Excitations in Direct Reactions (I)

doi: 10.1016/0375-9474(72)90503-9
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1972GO08      Phys.Lett. 38B, 379 (1972)

L.J.B.Goldfarb, E.F.Hefter

Application of the Sudden Approximation to the ¹²C(d, p₀)¹³C Reaction

NUCLEAR REACTIONS ¹²C(d, p₀), E=51 MeV; calculated σ(θ), P(θ). Sudden approximation.

doi: 10.1016/0370-2693(72)90161-X
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1972GO14      Nucl.Phys. A185, 337 (1972)

L.J.B.Goldfarb, J.A.Gonzalez, M.Posner, K.W.Jones

The ⁴⁰Ca(t, d₀)⁴¹Ca Reaction Near the Coulomb Barrier

NUCLEAR REACTIONS ⁴⁰Ca(t, d), E(lab)=2.0, 2.5, 3.0, 3.5 MeV; measured σ(θ);E(lab)=1.7 to 3.5 MeV; measured σ(160°). ⁴¹Ca deduced S.

doi: 10.1016/0375-9474(72)90017-6
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1971BA84      Nucl.Phys. A176, 321 (1971)

A.R.Barnett, W.R.Phillips, P.J.A.Buttle, L.J.B.Goldfarb

Nucleon Tunneling between ¹⁶O and ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁶O, ¹⁷O), (¹⁶O, ¹⁵N), E=69.1 MeV; measured σ(θ). ²⁰⁹Bi, ²⁰⁷Pb deduced S, bound-state wells.

doi: 10.1016/0375-9474(71)90273-9
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1971BU23      Nucl.Phys. A176, 299 (1971)

P.J.A.Buttle, L.J.B.Goldfarb

Systematics of Nucleon Transfer between Heavy Ions at Low Energies

NUCLEAR REACTIONS ²⁵Mg(¹⁷O, ¹⁶O), E=12, 14 MeV; ²⁰⁸Pb(¹⁷O, ¹⁶O), E=65 MeV; ²⁰⁸Pb(¹⁶O, ¹⁵N), E=69 MeV;¹⁴N(¹⁴N, ¹⁶N), E=12 MeV; ⁴⁰Ca(¹⁴N, ¹³N), E=22 MeV; ²⁰⁸Pb(¹⁶O, ¹⁷O), E=69 MeV; analyzed σ(Q).

doi: 10.1016/0375-9474(71)90272-7
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1970CO03      Nucl.Phys. A141, 532 (1970)

P.M.Cockburn, L.J.B.Goldfarb, I.S.Grant, H.E.Reed

The Dynamics of Three α-Particle Decay from an Unpolarized Source

NUCLEAR REACTIONS ¹¹B(p, 3α), E=0.68 MeV; measured αα-coin. ⁸Be deduced resonance parameters.

doi: 10.1016/0375-9474(70)90985-1
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1966GO14      Phys.Letters 22, 310 (1966)

L.J.B.Goldfarb, K.K.Wong

The Influence of Compound Nucleus Contributions on (d, p) Reactions

NUCLEAR STRUCTURE ⁵³Cr; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90627-5
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1960GO32      Nuclear Phys. 21, 462 (1960)

L.J.B.Goldfarb, R.C.Johnson

Selection Rules and Correlations for Polarization in Stripping and Direct Processes

doi: 10.1016/0029-5582(60)90070-5
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