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NSR database version of May 22, 2024.

Search: Author = A.K.Kerman

Found 29 matches.

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2010PE08      Nucl.Phys. A834, 381c (2010)

J.C.Pei, W.Nazarewicz, J.A.Sheikh, A.K.Kerman

Fission barriers and neutron gas in compound superheavy nuclei

NUCLEAR STRUCTURE 278Cn, 292Fl; calculated fission barriers, related features using the finite-temperature Hartree-Fock-Bogoliubov method.

doi: 10.1016/j.nuclphysa.2010.01.045
Citations: PlumX Metrics

2009PE10      Phys.Rev.Lett. 102, 192501 (2009)

J.C.Pei, W.Nazarewicz, J.A.Sheikh, A.K.Kerman

Fission Barriers of Compound Superheavy Nuclei

NUCLEAR STRUCTURE 264Fm, 272Ds, 278Cn, 292Fl, 312124; calculated isentropic fission barriers. Self-consistent nuclear density functional theory.

doi: 10.1103/PhysRevLett.102.192501
Citations: PlumX Metrics

2001HU06      Nucl.Phys. A686, 163 (2001)

M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov, A.K.Kerman

Estimate of the Anapole Moment of an Exotic Nucleus

NUCLEAR STRUCTURE 11Be; analyzed data; deduced anapole moment, halo anomaly.

doi: 10.1016/S0375-9474(00)00519-4
Citations: PlumX Metrics

2000KE13      Ann.Phys.(New York) 281, 853 (2000)

A.K.Kerman, H.McManus, R.M.Thaler

The Scattering of Fast Nucleons from Nuclei

NUCLEAR REACTIONS 12C, 208Pb(n, X), (p, X), E=90, 156, 310 MeV; calculated optical model parameters. 12C(p, p), E=90, 310 MeV; 12C, 16O(n, n'), E=156 MeV; calculated polarization. 4He(p, p), (n, n), E=147, 156, 310 MeV; 2H(p, p), E=156 MeV; calculated σ(θ). Reprint of earlier article.

doi: 10.1006/aphy.2000.6024
Citations: PlumX Metrics

1999GA50      Phys.Rev. C60, 064311 (1999); Erratum Phys.Rev. C 80, 039903 (2009)

F.Garcia, O.Rodriguez, F.Guzman, H.Dias, J.D.T.Arruda-Neto, M.S.Hussein, A.K.Kerman

Particle-Hole Level Densities in Deformed Nuclei

NUCLEAR STRUCTURE 233Th, 239U; calculated potential energy surfaces, particle-hole level densities; deduced deformation effects. Microscopic combinatorial approach.

doi: 10.1103/PhysRevC.60.064311
Citations: PlumX Metrics

1999HU16      Phys.Rev. C60, 064615 (1999)

M.S.Hussein, A.F.R.de Toledo Piza, O.K.Vorov, A.K.Kerman

Enhancement of Parity Violating Mixing in Halo Nuclei and the Problem of Neutron Weak Parity Nonconserving Potential Constant

NUCLEAR STRUCTURE 11Be; calculated halo density, wave-function; deduced parity-nonconserving effects.

doi: 10.1103/PhysRevC.60.064615
Citations: PlumX Metrics

1995AR06      Phys.Rev. C51, R1078 (1995)

G.Arbanas, M.B.Chadwick, F.S.Dietrich, A.K.Kerman

Linking of Direct and Compound Chains in Multistep Nuclear Reactions

NUCLEAR REACTIONS 93Nb(n, n'), E=14 MeV; analyzed angle integrated σ data; deduced direct, compound chains linking role on emisssion probabilities. Modified DWBA, multi-step reactions.

doi: 10.1103/PhysRevC.51.R1078
Citations: PlumX Metrics

1995CA22      Phys.Rev. C52, R11 (1995)

B.V.Carlson, M.S.Hussein, A.K.Kerman, C.-Y.Lin

Optical-Model Analysis of Parity-Nonconserving Neutron Scattering at Epithermal Energies

NUCLEAR REACTIONS 238U, 232Th(polarized n, n), E=epithermal; analyzed data; deduced doorway state role in <Δσ> for +, - helicity in parity nonconserving p-wave scattering.

doi: 10.1103/PhysRevC.52.R11
Citations: PlumX Metrics

1995FE07      Z.Phys. A351, 133 (1995)

H.Feshbach, M.S.Hussein, A.K.Kerman

Time Reversal Symmetry Breaking Effects in Resonant Nuclear Reactions

doi: 10.1007/BF01289522
Citations: PlumX Metrics

1995HU10      Z.Phys. A351, 301 (1995)

M.S.Hussein, A.K.Kerman, C.-Y.Lin

Fine Structure Discussion of Parity-Nonconserving Neutron Scattering at Epithermal Energies

NUCLEAR REACTIONS 232Th(n, n), E=epithermal; analyzed parity nonconserving spin-correlation data. Non-collective 2p-1h local doorway model.

doi: 10.1007/BF01290912
Citations: PlumX Metrics

1995PA24      Phys.Rev. C52, 252 (1995)

W.E.Parker, M.B.Chadwick, F.S.Dietrich, J.E.Kammeraad, S.J.Luke, K.E.Sale, R.M.Chasteler, M.A.Godwin, L.H.Kramer, G.J.Schmid, H.R.Weller, A.K.Kerman

Fluctuation Effects in Radiative Capture to Unstable Final States: A test via the 89Y(p(pol), γ) reaction at E(p) = 19.6 MeV

NUCLEAR REACTIONS 89Y(polarized p, γ), E=19.6 MeV; measured σ(θ), analyzing power(θ) vs Eγ. Direct-semdirect Hauser-Feshbach analyses. NaI(T1) detector.

doi: 10.1103/PhysRevC.52.252
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0909.

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
Citations: PlumX Metrics

1980BE35      Nucl.Phys. A345, 493 (1980)

M.Betz, A.K.Kerman

(π, d) Pick-Up reaction

NUCLEAR REACTIONS 16O(π, π), (π, d), E=50 MeV; 16O(d, d), E=200 MeV; calculated σ(θ); deduced distortion effects. One-step DWBA model.

doi: 10.1016/0375-9474(80)90352-8
Citations: PlumX Metrics

1979DI06      Phys.Rev.Lett. 43, 114 (1979)

F.S.Dietrich, A.K.Kerman

Pure-Resonance Model for Radiative Capture of Fast Nucleons

NUCLEAR REACTIONS 208Pb(n, γ), E=6-16 MeV; calculated σ(E). Direct semidirect model giant resonance projected from continuum space.

doi: 10.1103/PhysRevLett.43.114
Citations: PlumX Metrics

1975CA27      Nucl.Phys. A251, 193 (1975)

X.Campi, H.Flocard, A.K.Kerman, S.Koonin

Shape Transition in the Neutron Rich Sodium Isotopes

NUCLEAR STRUCTURE 19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34,35Na; calculated single particle energies, quadrupole moments, β.

doi: 10.1016/0375-9474(75)90065-2
Citations: PlumX Metrics

1974FL10      Nucl.Phys. A231, 176 (1974)

H.Flocard, P.Quentin, D.Vautherin, M.Veneroni, A.K.Kerman

Self-Consistent Calculation of the Fission Barrier of 240Pu

NUCLEAR STRUCTURE 240Pu; calculated deformation energy curve, levels.

doi: 10.1016/0375-9474(74)90300-5
Citations: PlumX Metrics

1973FL02      Nucl.Phys. A203, 433 (1973)

H.Flocard, P.Quentin, A.K.Kerman, D.Vautherin

Nuclear Deformation Energy Curves with the Constrained Hartree-Fock Method

NUCLEAR STRUCTURE 40Ca, 126,134,140,150Ce, 208Pb; calculated deformation energy curves with constrained Hartree-Fock technique.

doi: 10.1016/0375-9474(73)90357-6
Citations: PlumX Metrics

1973KA02      Ann.Phys.(New York) 75, 156 (1973)

M.Kawai, A.K.Kerman, K.W.McVoy

Modification of Hauser-Feshbach Calculations by Direct-Reaction Channel Coupling

doi: 10.1016/0003-4916(73)90465-X
Citations: PlumX Metrics

1973KL01      Phys.Rev. C7, 795 (1973)

S.Klawansky, H.W.Kendall, A.K.Kerman, D.Isabelle

Quasielastic Electron Scattering and a Giant Collective State in 209Bi

NUCLEAR REACTIONS 209Bi(e, e'), Q=150-300 MeV/c; analyzed σ(E;Ee').

doi: 10.1103/PhysRevC.7.795
Citations: PlumX Metrics

1973ST21      Phys.Rev. C8, 1269 (1973)

M.R.Strayer, W.H.Bassichis, A.K.Kerman

Correlation Effects in Nuclear Densities

NUCLEAR STRUCTURE 16O, 40Ca, 56Ni; calculated nuclear densities, rms radius.

doi: 10.1103/PhysRevC.8.1269
Citations: PlumX Metrics

1972AU04      Rev.Mod.Phys. 44, 48 (1972)

N.Auerbach, J.Hufner, A.K.Kerman, C.M.Shakin

A Theory of Isobaric Analog Resonances

doi: 10.1103/RevModPhys.44.48
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1972BA57      Phys.Rev. C6, 370 (1972)

W.H.Bassichis, A.K.Kerman

Note on Self-Consistent Calculation of Shell Effects

doi: 10.1103/PhysRevC.6.370
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1972SP02      Phys.Lett. 38B, 289 (1972)

J.E.Spencer, A.K.Kerman

A Potential Model Interpretation of Isobaric Analog Resonances Applicable to Even-Even and Even-Odd Targets

NUCLEAR REACTIONS 88Sr, 89Y(p, p), E=4.6-5.2 MeV; calculated σ(E). 87Rb, 88Sr, 89Y, 90Zr, 91Nb, 93Tc calculated isobaric analog resonances, level-width, S.

doi: 10.1016/0370-2693(72)90248-1
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1971SP04      Phys.Rev. C3, 1179 (1971)

J.E.Spencer, E.R.Cosman, H.A.Enge, A.K.Kerman

Analysis of Proton Scattering and Reactions with the Generalized Optical Model

NUCLEAR REACTIONS 88Sr(p, p), (p, p'), (p, n), E=4.8-8.2 MeV; measured nothing; deduced σ(E;θ). Generalized optical model. 89Sr; calculated levels, J, π.

doi: 10.1103/PhysRevC.3.1179
Citations: PlumX Metrics

1970TU01      Nucl.Phys. A142, 49 (1970)

D.R.Tuerpe, W.H.Bassichis, A.K.Kerman

Self-Consistent Nuclear Calculations with a Deformed Basis

NUCLEAR STRUCTURE 4He, 8Be, 12C, 16O, 20Ne, 24Mg, 28Si, 32S, 36Ar, 40,44Ca, 44,48Ti, 48Cr, 52,56Fe; calculated binding energies, quadrupole moment, rms radii, kinetic energies/particle. Deformed harmonic oscillator basis functions.

doi: 10.1016/0375-9474(70)90473-2
Citations: PlumX Metrics

1968RA18      Nucl.Phys. A119, 641 (1968)

J.Rapaport, A.K.Kerman

Study of the 138Ba(d, p)139Ba Reaction for Incident Energies below the Coulomb Barrier

NUCLEAR REACTIONS 138Ba(d, p), Ed=5.0, 5.5, 6.0, 6.5, 7.0, 7.5 MeV; 138Ba(d, d), Ed=7.5 MeV; measured σ(E; θ). 139Ba deduced levels, S. Enriched target.

doi: 10.1016/0375-9474(68)90263-7
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1963KE16      Phys.Rev.Letters 11, 422 (1963)

A.K.Kerman, L.S.Rodberg, J.E.Young

Intermediate Structure in the Energy Dependence of Nuclear Cross Sections

doi: 10.1103/PhysRevLett.11.422
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1962KE07      Phys.Letters, 1, 151 (1962)

A.K.Kerman, C.M.Shakin

Vibrations of Spherical Nuclei

NUCLEAR STRUCTURE 62Ni; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(62)90331-1
Citations: PlumX Metrics

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