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NSR database version of May 24, 2024.

Search: Author = A.D.Mackellar

Found 18 matches.

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1995CH36      Phys.Rev. C52, 878 (1995)

B.Q.Chen, A.D.MacKellar

Proton-Nucleus Scattering Based on the Relativistic Brueckner-Hartree-Fock Model

NUCLEAR REACTIONS 40Ca, 16O, 90Zr, 208Pb(polarized p, p), E=160-500 MeV; analyzed σ(θ), polarization observables data. Optical potentials from relativistic Brueckner-Bethe-Goldstone equation.

doi: 10.1103/PhysRevC.52.878
Citations: PlumX Metrics

1990NU01      Nucl.Phys. A511, 525 (1990)

C.Nuppenau, A.D.Mackellar, Y.J.Lee

Study of Nucleon-Nucleus Scattering Based on the Relativistic Brueckner-Bethe-Goldstone Equation

NUCLEAR REACTIONS 40Ca(polarized p, p), E=160-497 MeV; calculated σ(θ), analyzing power vs θ. Relativistic Brueckner-Bethe-Goldstone equation.

doi: 10.1016/0375-9474(90)90108-X
Citations: PlumX Metrics

1986HO19      Phys.Rev. C34, 429 (1986)

D.J.Horen, C.H.Johnson, J.L.Fowler, A.D.MacKellar, B.Castel

208Pb + n Reaction and the Mean Nuclear Field near Threshold

NUCLEAR REACTIONS 208Pb(n, X), 208Pb(n, n), E=50-1005 keV; measured transmission, σ(E), σ(θ); deduced model parameters. 209Pb deduced resonances, J, π, Γn, neutron reduced width, strength function. Optical model, R-matrix analysis.

doi: 10.1103/PhysRevC.34.429
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13738.

1985HO23      Phys.Lett. 161B, 217 (1985)

D.J.Horen, C.H.Johnson, A.D.Mackellar

lJ-Dependence of the Real Optical Potential near Neutron Threshold

NUCLEAR REACTIONS 208Pb(n, X), (n, n), E=0.05-1.005 MeV; measured transmission, σ(θ). 208Pb(n, n), E=4, 7 MeV; analyzed σ(θ); deduced optical model parameters, l-, j-dependences.

doi: 10.1016/0370-2693(85)90748-8
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1985WI02      Phys.Rev. C31, 384 (1985)

R.R.Winters, C.H.Johnson, A.D.MacKellar

Optical Model for Low-Energy Neutrons on 60Ni

NUCLEAR REACTIONS 60Ni(n, n), E=1-450 keV; analyzed σ(E); deduced optical model parameters.

doi: 10.1103/PhysRevC.31.384
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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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1984MA24      Phys.Rev. C29, 1993 (1984)

A.D.MacKellar, B.Castel

s- and p-Wave Neutrons on 30Si and 34S: Coupled channels optical model

NUCLEAR REACTIONS 30Si, 34S(n, n), E not given; analyzed data; deduced optical model parameter target excitation dependence. Coupled-Channels model, collective effects.

doi: 10.1103/PhysRevC.29.1993
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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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1983MA30      Phys.Rev. C28, 441 (1983)

A.D.MacKellar, B.Castel

l Dependence of the Optical Potential: Application to the 32S + n reaction using coupled channels

NUCLEAR REACTIONS 32S(n, n), E=0.5 MeV; calculated s-, p-wave, σ(shape elastic). 32S(n, n), E=0.1-0.8 MeV; calculated s-wave σ(shape elastic); deduced optical potential parameters. Dynamical deformation, coupled-channels calculation.

doi: 10.1103/PhysRevC.28.441
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1976MA39      Nucl.Phys. A269, 1 (1976)

A.D.Mackellar, M.Coz

Separable Coupled Channels Method for Nucleon-Nucleus Scattering

NUCLEAR REACTIONS 76,82Se(n, X), E ≤ 8 MeV; 208Pb(n, X), E < 16 MeV; calculated σ(E).

doi: 10.1016/0375-9474(76)90392-4
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1974MA20      Nucl.Phys. A225, 61 (1974)

A.D.MacKellar, R.E.Schenter, H.M.Schadel, A.Lev, W.P.Beres

Complex Local Equivalents to Imaginary Non-Local Potentials: Neutron Scattering from 208Pb

NUCLEAR REACTIONS 208Pb(n, n); calculated σ(E), local potential.

doi: 10.1016/0375-9474(74)90365-0
Citations: PlumX Metrics

1974WO06      Nucl.Phys. A228, 345 (1974)

J.W.Woodring, A.D.Mackellar, R.K.Tripathi

Three Body Clusters in Finite Nuclei (I). 4He

NUCLEAR STRUCTURE 4He; calculated binding energy.

doi: 10.1016/0375-9474(74)90438-2
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1973FA14      Nucl.Phys. A215, 525 (1973)

A.Faessler, A.D.MacKellar, R.K.Tripathi

The Influence of the Pauli Operator on the Density Distribution in the Brueckner-Hartree-Fock Approach in 40Ca

NUCLEAR STRUCTURE 40Ca; calculated charge distribution;single particle energies, binding energy.

doi: 10.1016/0375-9474(73)90485-5
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1973TR08      Phys.Rev. C8, 129 (1973)

R.K.Tripathi, A.Faessler, A.D.MacKellar

Self-Consistent Treatment of the Pauli Operator in the Brueckner-Hartree-Fock Approach

NUCLEAR STRUCTURE 16O; calculated binding energies, charge distributions using the Brueckner-Hartree-Fock equations with addition of Pauli operator.

doi: 10.1103/PhysRevC.8.129
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1971MA05      Phys.Rev. C3, 460 (1971)

A.D.MacKellar, J.F.Reading, A.K.Kerman

Low-Energy Neutron-Oxygen Scattering Derived from Two-Body Forces

NUCLEAR REACTIONS 16O(n, n), E=0-4 MeV calculated phase shifts.

doi: 10.1103/PhysRevC.3.460
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1971MA62      Nucl.Phys. A178, 249 (1971)

A.D.Mackellar, R.E.Schenter

A Comparison of Hartree-Fock and Perey-Buck Non-Local Potentials for Low-Energy Scattering

NUCLEAR REACTIONS 16O(n, n), E not given; analyzed Hartree-Fock, Perey-Buck non-local potentials.

doi: 10.1016/0375-9474(71)90202-8
Citations: PlumX Metrics

1971SC22      Phys.Rev. C4, 2020 (1971)

R.E.Schenter, A.D.MacKellar

Origin of Damping of Wave Functions in the Nuclear Interior

NUCLEAR REACTIONS 16O(n, n), E=2.5 MeV; calculated damping of single-particle wave functions. Hartree-Fock method, nonlocal potentials.

doi: 10.1103/PhysRevC.4.2020
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1965MA36      Phys.Letters 18, 308 (1965)

A.D.MacKellar, R.L.Becker

Nuclear Ground State Properties of 16O by an Extension of the Eden-Emery Method

NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90350-1
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