NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 11, 2024.

Search: Author = J.A.McNeil

Found 27 matches.

Back to query form



2001HO23      Nucl.Phys. A688, 527c (2001)

M.A.Hofstee, A.K.Pallone, F.E.Cecil, J.A.McNeil, C.S.Galovich

Measurement of Low Energy (d, n) Reactions on Light Nuclei Important to Astrophysics

NUCLEAR REACTIONS 2H, 6,7Li, 9Be, 10,11B(d, n), E=24-111 keV; measured σ, S-factor. Comparison with earlier data.

doi: 10.1016/S0375-9474(01)00777-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1511.


1997YA02      Phys.Rev. C55, 1890 (1997)

J.Yan, F.E.Cecil, J.A.McNeil, M.A.Hofstee, P.D.Kunz

Deuteron-Induced Reactions on 9Be, 10B, and 11B at Low Energies

NUCLEAR REACTIONS, ICPND 9Be(d, p), (d, α), E(cm)=57-139 keV; 10B(d, p), (d, α), E(cm)=67-141 keV; 11B(d, p), (d, α), E(cm)=76-144 MeV; 9Be(d, t), E(cm)=57-139 MeV; measured energy spectra, σ(θ); deduced σ, astrophysical S-factor vs E.

doi: 10.1103/PhysRevC.55.1890
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0452.


1997YA08      Nucl.Phys. A621, 127c (1997)

J.Yan, F.E.Cecil, J.A.McNeil, M.A.Hofstee

Measurement of Astrophysical S-Factors for Deuteron-Induced Reactions on 7Li, 9Be, 10B, and 11B at Low Energies

NUCLEAR REACTIONS, ICPND 7Li(d, nα), (d, α), E(cm)=30-130 keV; 9Be, 10,11B(d, p), (d, α), E(cm)=57-141 keV; 9Be(d, t), E(cm)=57-139 keV; measured astrophysical S-factors.

doi: 10.1016/S0375-9474(97)00223-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0452.


1992CE02      Nucl.Phys. A539, 75 (1992)

F.E.Cecil, D.Ferg, H.Liu, J.C.Scorby, J.A.McNeil, P.D.Kunz

Radiative Capture of Protons by Light Nuclei at Low Energies

NUCLEAR REACTIONS, ICPND 6,7Li, 9Be, 11B(p, γ), E=40-180 keV; measured capture Eγ, Iγ, γ(θ); deduced astrophysical S-factor. 7,8Be, 10B, 12C levels deduced γ-ray to charged particle branching ratio. Thick targets, hyperpure Ge detectors.

doi: 10.1016/0375-9474(92)90236-D
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1290.


1992PR01      Phys.Rev. C45, 1089 (1992)

C.E.Price, E.Rost, J.R.Shepard, J.A.McNeil

Toward a Consistent Random Phase Approximation Based on the Relativistic Hartree Approximation

NUCLEAR STRUCTURE 16O, 40Ca; calculated levels, isoscalar transitions. RPA, relativistic Hartree approximation.

NUCLEAR REACTIONS 16O, 12C, 40Ca(e, e'), E not given; calculated longitudinal form factor. RPA, relativistic Hartree approximation.

doi: 10.1103/PhysRevC.45.1089
Citations: PlumX Metrics


1990MC07      Phys.Rev. C42, 2442 (1990)

J.A.McNeil, C.E.Price, J.R.Shepard

Nuclear Ground-State Correlations in the Relativistic Random-Phase Approximation

NUCLEAR STRUCTURE 16O, 40Ca; calculated binding energy per particle, rms radii, levels, charge density. Relativistic RPA.

doi: 10.1103/PhysRevC.42.2442
Citations: PlumX Metrics


1989MC05      Phys.Rev. C40, 399 (1989)

J.A.McNeil, R.J.Furnstahl, E.Rost, J.R.Shepard

Finite Nucleus Dirac Mean Field Theory and Random Phase Approximation using Finite B Splines

NUCLEAR STRUCTURE 16O, 40Ca; calculated levels, isoscalar longitudinal form factors. Finite nucleus Dirac mean field theory.

doi: 10.1103/PhysRevC.40.399
Citations: PlumX Metrics


1989SH27      Phys.Rev. C40, 2320 (1989)

J.R.Shepard, E.Rost, J.A.McNeil

Nonspectral Dirac Random-Phase Approximation for Finite Nuclei

NUCLEAR REACTIONS 12C, 16O, 48,40Ca(e, e'), E not given; calculated form factors. Nonspectral Dirac RPA.

NUCLEAR STRUCTURE 16O; calculated lowest 1-, T=0 level B(E1). RPA.

doi: 10.1103/PhysRevC.40.2320
Citations: PlumX Metrics


1988SH07      Phys.Rev. C37, 1130 (1988)

J.R.Shepard, E.Rost, C.-Y.Cheung, J.A.McNeil

Magnetic Response of Closed-Shell ±1 Nuclei in Dirac-Hartree Approximation

NUCLEAR REACTIONS 15N(e, e), E not given; calculated isoscalar M1 form factor. Dirac-Hartree approximation.

NUCLEAR STRUCTURE 15N, 15O; A=15, 17, 39, 41; calculated μ. Dirac-Hartree approximation.

doi: 10.1103/PhysRevC.37.1130
Citations: PlumX Metrics


1986MC02      Phys.Rev. C33, 1106 (1986)

J.A.McNeil, J.R.Shepard

Reply to ' Relativistic Nuclear Model and 0+ → 0-, 0- → 0+ Weak Transitions '

NUCLEAR STRUCTURE 16O, 16N; calculated β-decay, muon capture rates; deduced relativistic nuclear dynamics sensitivity.

doi: 10.1103/PhysRevC.33.1106
Citations: PlumX Metrics


1986MC13      Phys.Rev. C34, 746 (1986)

J.A.McNeil, R.D.Amado, C.J.Horowitz, M.Oka, J.R.Shepard, D.A.Sparrow

Resolution of the Magnetic Moment Problem in Relativistic Theories

NUCLEAR STRUCTURE A=15, 17, 39, 41; calculated isoscalar μ; deduced Schmidt value equality. Relativistic treatment.

doi: 10.1103/PhysRevC.34.746
Citations: PlumX Metrics


1986SH01      Phys.Rev. C33, 634 (1986)

J.R.Shepard, E.Rost, J.A.McNeil

Relativistic Plane-Wave Impulse Approximation for Nuclear Inelastic Scattering of Protons and Electrons

NUCLEAR REACTIONS 12C(e, e'), E not given; 12C(p, p'), E=150 MeV; calculated nuclear transition densities, currents. 12C levels deduced structure information. Relativistic plane-wave impulse approximation.

doi: 10.1103/PhysRevC.33.634
Citations: PlumX Metrics


1985SP03      Phys.Rev.Lett. 54, 2207 (1985)

D.A.Sparrow, J.Piekarewicz, E.Rost, J.R.Shepard, J.A.McNeil, T.A.Carey, J.B.McClelland

Relativistic Impulse Approximation, Nuclear Currents, and the Spin-Difference Function

NUCLEAR REACTIONS 12C(p, p'), E=150 MeV; calculated P(θ), analyzing power vs θ difference; deduced nuclear currents role. Relativistic approximation.

doi: 10.1103/PhysRevLett.54.2207
Citations: PlumX Metrics


1984AM02      Phys.Rev. C29, 936 (1984)

R.D.Amado, J.Piekarewicz, D.A.Sparrow, J.A.McNeil

Analytic Expressions for the Dirac Treatment of Nucleon-Nucleus Scattering

NUCLEAR REACTIONS 40Ca(polarized n, n), E=500 MeV; 208Pb(polarized p, p), E=800 MeV; calculated σ(θ), asymmetry, spin rotation parameter vs θ. Dirac treatment, analytically evaluated scattering amplitudes.

doi: 10.1103/PhysRevC.29.936
Citations: PlumX Metrics


1984CL11      Phys.Rev.Lett. 53, 1423 (1984)

B.C.Clark, S.Hama, J.A.McNeil, R.L.Mercer, L.Ray, B.D.Serot, D.A.Sparrow, K.Stricker-Bauer

Relative Impulse-Approximation Calculation of p(bar)-Nucleus Elastic Scattering

NUCLEAR REACTIONS 12C(p-bar, p-bar), (polarized p-bar, p-bar), E=46.8 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ. Relativistic impulse approximation.

doi: 10.1103/PhysRevLett.53.1423
Citations: PlumX Metrics


1984RO02      Phys.Rev. C29, 209 (1984)

E.Rost, J.R.Shepard, E.R.Siciliano, J.A.McNeil

Impulse Approximation Dirac Theory of Inelastic Proton Nucleus Collective Excitations

NUCLEAR REACTIONS 54Fe(polarized p, p), E=800 MeV; calculated σ(θ), analyzing power vs θ. Dirac theory, impulse approximation.

doi: 10.1103/PhysRevC.29.209
Citations: PlumX Metrics


1984SH08      Phys.Rev. C29, 2243 (1984)

J.R.Shepard, E.Rost, E.R.Siciliano, J.A.McNeil

Dirac Single-Particle Wave Functions in Inelastic Electron Scattering

NUCLEAR REACTIONS 12C(e, e), (e, e'), E not given; calculated charge, transverse form factors; deduced transverse isoscalar transition linear inelastic amplitude role. Dirac single particle wave functions.

doi: 10.1103/PhysRevC.29.2243
Citations: PlumX Metrics


1983AM04      Phys.Rev. C28, 1663 (1983)

R.D.Amado, J.Piekarewicz, D.A.Sparrow, J.A.McNeil

Dirac-Eikonal Scattering Amplitude

NUCLEAR REACTIONS 40Ca(p, p), E=500 MeV; calculated σ(θ) vs momentum transfer. Dirac-eikonal amplitude, Dirac impulse approximation.

doi: 10.1103/PhysRevC.28.1663
Citations: PlumX Metrics


1983AM05      Phys.Rev. C28, 2180 (1983)

R.D.Amado, J.Piekarewicz, D.A.Sparrow, J.A.McNeil

Intermediate-Energy-Proton Scattering, the Dirac Equation, and Nuclear Structure

NUCLEAR REACTIONS 40Ca(p, p), (polarized p, p), E=500 MeV; calculated σ(θ), analyzing power, spin rotation parameter vs θ.

doi: 10.1103/PhysRevC.28.2180
Citations: PlumX Metrics


1983MC04      Phys.Rev. C27, 2123 (1983)

J.A.McNeil, L.Ray, S.J.Wallace

Impulse Approximation NN Amplitudes for Proton-Nucleus Interactions

NUCLEAR REACTIONS 40Ca(p, p), E=800 MeV; calculated σ(θ). 40Ca(polarized p, p), E=500 MeV; calculated analyzing power vs θ. Impulse approximation, invariant nucleon-nucleon amplitudes.

doi: 10.1103/PhysRevC.27.2123
Citations: PlumX Metrics


1983SH05      Phys.Rev.Lett. 50, 1443 (1983)

J.R.Shepard, J.A.McNeil, S.J.Wallace

Relativistic Impulse Approximation for p-Nucleus Elastic Scattering

NUCLEAR REACTIONS 40Ca(polarized p, p), E=500 MeV; calculated σ(θ), analyzing power vs θ. Impulse approximation, Dirac optical potential.

doi: 10.1103/PhysRevLett.50.1443
Citations: PlumX Metrics


1982AM01      Phys.Rev. C25, 13 (1982)

R.D.Amado, J.A.McNeil, D.A.Sparrow

Analytic Treatment of Multistep Processes in Hadron-Nucleus Scattering

NUCLEAR REACTIONS 166Er, 182W, 154Sm(p, p'), E=800 MeV; calculated σ(θ). Analytic treatment, multi-step processes, eikonal formalism, coupled-channels method.

doi: 10.1103/PhysRevC.25.13
Citations: PlumX Metrics


1982MC09      Phys.Rev. C26, 1141 (1982)

J.A.McNeil, D.A.Sparrow, R.D.Amado

Spin Observables and Nuclear Geometry

NUCLEAR REACTIONS 40Ca(polarized p, p), E=500 MeV; calculated proton polarization, spin rotation parameter vs momentum transfer. Analytic formulation.

doi: 10.1103/PhysRevC.26.1141
Citations: PlumX Metrics


1982SP01      Phys.Rev.Lett. 48, 124 (1982)

D.A.Sparrow, R.D.Amado, J.A.McNeil

New Measure of Nuclear Transition Strengths

NUCLEAR REACTIONS 208Pb(p, p'), E=800 MeV; 208Pb(π+, π+'), (π-, π-'), E=291 MeV; 60Ni(p, p'), E=1047 MeV; analyzed data. 208Pb, 60Ni levels deduced inelastic strength factor. Tassie model, eikonal framework, analytic methods.

doi: 10.1103/PhysRevLett.48.124
Citations: PlumX Metrics


1981AM03      Phys.Rev. C23, 2186 (1981)

R.D.Amado, J.A.McNeil, D.A.Sparrow

Two-Step Processes in Intermediate Energy Hadron-Nucleus Scattering

NUCLEAR REACTIONS 154Sm, 24Mg(p, p'), E=800 MeV; analyzed σ(θ). Two-step process, closed form eikonal approximation.

doi: 10.1103/PhysRevC.23.2186
Citations: PlumX Metrics


1981IK02      Phys.Rev. C24, 2754 (1981)

R.M.Ikeda, J.A.McNeil

Comment on Analytical Evaluation of the Coulomb Distortion

NUCLEAR REACTIONS 208Pb(p, p), E=800 MeV; 208Pb(π+, π+), (π-, π-), E=291 MeV; calculated σ(θ). Coulomb distortion analytic treatment.

doi: 10.1103/PhysRevC.24.2754
Citations: PlumX Metrics


1981MC08      Phys.Rev. C23, 2791 (1981)

J.A.McNeil

Approximating Coulomb Effects in Hadron-Nucleus Scattering

NUCLEAR REACTIONS 208Pb(p, p), E=800 MeV; 208Pb(π+, π+), (π-, π-), E=291 MeV; calculated σ(θ). Analytic hadron-nucleus scattering amplitudes, Coulomb effects.

doi: 10.1103/PhysRevC.23.2791
Citations: PlumX Metrics


Back to query form