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Search: Author = A.G.Van Hees

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1994BO04      Nucl.Phys. A569, 510 (1994)

J.G.L.Booten, A.G.M.van Hees

Magnetic Electron Scattering from p-Shell Nuclei

NUCLEAR REACTIONS 6Li, 10,11B, 14,15N(e, e), (e, e'), E not given; calculated form factors. Shell model, meson exchange currents.

doi: 10.1016/0375-9474(94)90316-6
Citations: PlumX Metrics

1994SP02      Nucl.Phys. A570, 472 (1994)

W.F.M.Spit, A.G.M.van Hees, P.J.Brussaard, P.J.Mulders

Quark Antisymmetrization and Deep-Inelastic Scattering I. Nuclear Quark Momentum Distributions

NUCLEAR STRUCTURE 6Li, 14N, 16O; calculated charge density for different deformations. Full, impulse approximation calculations. Quark antisymmatrization, deep inelastic scattering.

doi: 10.1016/0375-9474(94)90069-8
Citations: PlumX Metrics

1993SP03      Nucl.Phys. A553, 689c (1993)

W.F.M.Spit, V.Vento, A.G.M.van Hees, P.J.Brussaard, P.J.Mulders

Quark Antisymmetrization in Nuclei

NUCLEAR STRUCTURE 6Li, 16O; calculated Coulomb, magnetic form factors, charge density. 14N; calculated charge density. Quark antisymmetrization.

doi: 10.1016/0375-9474(93)90680-V
Citations: PlumX Metrics

1992BO30      Nucl.Phys. A549, 197 (1992)

J.G.L.Booten, A.G.M.van Hees, P.W.M.Glaudemans, P.J.Brussaard

Large-Basis Space and Mesonic Effects on the 7Li Form Factors

NUCLEAR REACTIONS 7Li(e, e), (e, e'), E not given; calculated form factors; deduced meson exchange role. Shell model.

doi: 10.1016/0375-9474(92)90040-Q
Citations: PlumX Metrics

1992KI05      Nucl.Phys. A539, 1 (1992)

S.W.Kikstra, S.S.Hanna, A.G.M.van Hees, Z.Guo, C.van der Leun

Resonant Absorption by the Lowest Two T = (3/2) Levels of 9Be

NUCLEAR REACTIONS 9Be(γ, X), E=14.38-16.98 MeV; measured σ(Eγ), 9Be levels deduced Γγ0, isospin mixing, giant M1 resonance parameters. Shell model calculations. Monochromatic γ's from 11B(p, γ0γ1).

doi: 10.1016/0375-9474(92)90232-9
Citations: PlumX Metrics

1992WO01      Phys.Rev. C45, 477 (1992)

A.A.Wolters, A.G.M.van Hees, P.W.M.Glaudemans

Reply to ' Comment on ' p-Shell Nuclei in a (0+2)(h-bar x Omega) Model Space. I. Method ' and on ' p-Shell Nuclei in a (0+2)(h-bar x Omega) Model Space. II. Results ' '

doi: 10.1103/PhysRevC.45.477
Citations: PlumX Metrics

1991BO02      Phys.Rev. C43, 335 (1991)

J.G.L.Booten, A.G.M.van Hees, P.W.M.Glaudemans, R.Wervelman

Meson Exchange Current Effects on Magnetic Dipole Moments of p-Shell Nuclei

NUCLEAR STRUCTURE 9,7,8Li, 9Be, 8,11,12,13B, 11,13C, 12,13,15N, 15O, 3H, 3He; calculated μ; deduced meson exchange currents role.

doi: 10.1103/PhysRevC.43.335
Citations: PlumX Metrics

1991PA18      Phys.Lett. 271B, 1 (1991)

V.Paar, D.Vorkapic, K.Heyde, A.G.M.van Hees, A.A.Wolters

Broken Isospin Symmetry in the Shell Model and Chaotic Behavior

NUCLEAR STRUCTURE A=22; calculated nearest neighbor spacing distribution with, without Coulomb interaction, Δ3 statistics; deduced isospin symmetry breaking effect on quantum chaos. Realistic shell model.

doi: 10.1016/0370-2693(91)91267-Y
Citations: PlumX Metrics

1991WE06      Nucl.Phys. A526, 265 (1991)

R.Wervelman, K.Abrahams, H.Postma, J.G.L.Booten, A.G.M.van Hees

Nuclear Capture by 3He and the Production of Solar Hep-Neutrinos: Cross-section measurements and shell-model calculations

NUCLEAR REACTIONS 3He(n, γ), E=thermal, 24.5 keV; measured capture σ. Enriched target. Shell model calculations for 3He(n, γ), (p, e+, ν(e)), meson exchange currents.

doi: 10.1016/0375-9474(91)90287-G
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22230.

1990EN02      Nucl.Phys. A510, 209 (1990)

P.M.Endt, C.Alderliesten, F.Zijderhand, A.A.Wolters, A.G.M.van Hees

Spectroscopic Information on 24Mg and 28Si from Proton Capture

NUCLEAR REACTIONS 23Na(p, γ), E=1020, 1318, 1417 keV; measured Eγ, Iγ, σ(E, Eγ). 24Mg deduced levels, γ-branching, J, π, T. 27Al(p, γ), E=655, 760, 767, 992, 1317 keV; measured Eγ, Iγ, σ(E, Eγ). 28Si deduced levels, γ-branching, T1/2, J, π, T. Ge detectors with, without Compton suppression.

doi: 10.1016/0375-9474(90)90237-G
Citations: PlumX Metrics

1990HO19      Nucl.Phys. A516, 205 (1990)

A.Hogenbirk, H.P.Blok, M.G.E.Brand, A.G.M.van Hees, J.F.A.van Hienen, F.A.Jansen

A Study of 36S by High-Resolution Inelastic Proton and Alpha Scattering

NUCLEAR REACTIONS 36S(p, p'), E=28 MeV; 36S(α, α'), E=32 MeV; measured σ(E, θ); deduced optical model parameters. 36S levels deduced J, π, L, deformation parameters, B(λ). Enriched target, magnetic spectrometer. Coupled-channels calculations, macroscopic rotational, vibrational, rotation-vibration models, semi-microscopic folding model, microscopic extended-RPA model, shell model analysis.

doi: 10.1016/0375-9474(90)90307-8
Citations: PlumX Metrics

1990KI07      Nucl.Phys. A512, 425 (1990)

S.W.Kikstra, C.van der Leun, P.M.Endt, J.G.L.Booten, A.G.M.van Hees, A.A.Wolters

The 40Ca Level Scheme Investigated with the 39K(p, γ)40Ca Reaction

NUCLEAR REACTIONS, ICPND 39K(p, γ), E=0.3-2.9 MeV; measured σ(E, Eγ), γ yield; deduced Q. 40Ca deduced levels, resonance strengths, γ-branchings, T1/2, J, π, T. Enriched targets, Ge detectors. Shell-model calculations.

doi: 10.1016/0375-9474(90)90080-6
Citations: PlumX Metrics

1990SP03      Nucl.Phys. A510, 609 (1990)

W.F.M.Spit, A.G.M.van Hees, P.J.Mulders

Quark Exchange and Nuclear Form Factors

NUCLEAR STRUCTURE 6Li, 16O; calculated form factors. Quark exchange.

doi: 10.1016/0375-9474(90)90351-L
Citations: PlumX Metrics

1990VA01      Nucl.Phys. A507, 55c (1990)

A.G.M.Van Hees, J.G.L.Booten, P.W.M.Glaudemans

Three-Body Forces in p-Shell Nuclei

NUCLEAR STRUCTURE 4,5He, 6,7Li, 8,9Be, 10,11B, 12,13C, 14,15N, 16O; calculated three-body contribution to binding energy.

doi: 10.1016/0375-9474(90)90568-7
Citations: PlumX Metrics

1990WO09      Phys.Rev. C42, 2053 (1990)

A.A.Wolters, A.G.M.van Hees, P.W.M.Glaudemans

p-Shell Nuclei in a (0 + 2)(h-bar x Omega) Model Space. I. Method

NUCLEAR STRUCTURE 8Be; calculated levels. 4He, 12,14C, 16O, 14N, 8Be; calculated Coulomb energies, radial excitation strengths. Empirical effective interaction, complete (0+2) (h-bar x omega) space.

doi: 10.1103/PhysRevC.42.2053
Citations: PlumX Metrics

1990WO10      Phys.Rev. C42, 2062 (1990)

A.A.Wolters, A.G.M.van Hees, P.W.M.Glaudemans

p-Shell Nuclei in a (0 + 2)(h-bar x Omega) Model Space. II. Results

NUCLEAR STRUCTURE 6,4,5,7,8He; 7,8,9Li, 9,10,11,12Be, 10,11,12,13B, 15,12,13,14C, 14,15,16N, 16O; calculated levels. Effective interactions, (0+2)(h-bar x omega) space.

NUCLEAR REACTIONS 4He, 7Li, 13C(e, e'), E not given; calculated form factors. Effective interactions, (0+2)(h-bar x omega) space.

doi: 10.1103/PhysRevC.42.2062
Citations: PlumX Metrics

1989LA13      Phys.Rev.Lett. 62, 2925 (1989)

J.B.J.M.Lanen, A.M.van den Berg, H.P.Blok, J.F.J.van den Brand, C.T.Christou, R.Ent, A.G.M.van Hees, E.Jans, G.J.Kramer, L.Lapikas, D.R.Lehman, W.C.Parke, E.N.M.Quint, G.van der Steenhoven, P.K.A.de Witt Huberts

Electrodisintegration of 6Li Studied with the Reaction 6Li(e, e'p)

NUCLEAR REACTIONS 6Li(e, e'p), E not given; measured missing energy spectra, momentum distributions; deduced spectroscopic strength. Three-body model.

doi: 10.1103/PhysRevLett.62.2925
Citations: PlumX Metrics

1989VA06      Phys.Rev.Lett. 62, 2245 (1989); Erratum Phys.Rev.Lett. 62, 3099 (1989)

A.G.M.van Hees, J.G.L.Booten, P.W.M.Glaudemans

Three-Body Forces and the Description of Light Nuclei

NUCLEAR STRUCTURE 4,5He, 6,7Li, 8,9Be, 10,11B, 12,13C, 14,15N, 16O; calculated total binding energy. Three-body forces.

doi: 10.1103/PhysRevLett.62.2245
Citations: PlumX Metrics

1988VA03      Nucl.Phys. A476, 61 (1988)

A.G.M.van Hees, A.A.Wolters, P.W.M.Glaudemans

Static Moments and Phenomenological Interactions

NUCLEAR STRUCTURE 9,6,7,8Li, 8,10,11,12,13B, 9Be, 11,13,14,15C, 12,13,14,15,16N, 15,16O; calculated μ. Phenomenological interactions.

doi: 10.1016/0375-9474(88)90373-9
Citations: PlumX Metrics

1988WO04      Europhys.Lett. 5, 7 (1988)

A.A.Wolters, A.G.M.van Hees, P.W.M.Glaudemans

An Expansion of the Shell-Model Space for Light Nuclei

NUCLEAR STRUCTURE 4He, 6,7Li, 10,11B, 9Be, 12,13,14C, 14,15N, 16O; calculated ground state wave functions, rms charge radii, quadrupole moments. Shell model, phenomenological interaction.

doi: 10.1209/0295-5075/5/1/002
Citations: PlumX Metrics

1987DO10      Nucl.Phys. A469, 518 (1987)

A.J.H.Donne, L.Lapikas, A.G.M.van Hees, D.Zwarts

Transverse Electroexcitation of Positive- and Negative-Parity States in 19F

NUCLEAR REACTIONS 19F(e, e'), E=46-272 MeV; measured σ(E, θ). 19F deduced transverse form factors. Shell-model calculation.

doi: 10.1016/0375-9474(87)90037-6
Citations: PlumX Metrics

1987ME16      Nucl.Phys. A473, 160 (1987)

W.Mettner, A.Richter, W.Stock, B.C.Metsch, A.G.M.van Hees

Electroexcitation of 58Ni: A study of the fragmentation of the magnetic dipole strength

NUCLEAR REACTIONS 58Ni(e, e'), E=39-57 MeV; measured σ(E(e')), σ(θ). 58Ni deduced B(λ). Comparison with shell model calculation.

doi: 10.1016/0375-9474(87)90159-X
Citations: PlumX Metrics

1987VA26      Phys.Lett. 196B, 19 (1987)

A.G.M.van Hees, A.A.Wolters, P.W.M.Glaudemans

An Effective Interaction Derived from Spectra and Static Moments

NUCLEAR STRUCTURE 8Li, 11Be, 8,12,14B, 14,15C, 12,16N; calculated magnetic dipole moments. Phenomenological interaction.

doi: 10.1016/0370-2693(87)91668-6
Citations: PlumX Metrics

1985CA23      Phys.Rev. C32, 323 (1985)

B.Castel, I.P.Johnstone, A.G.M.van Hees

Magnetic Quadrupole Strength in 12C

NUCLEAR STRUCTURE 12C; calculated M2 transition strength fragmentation; deduced 2p-2h correlation, two-body spin-orbit force in quenching. Large basis shell model.

doi: 10.1103/PhysRevC.32.323
Citations: PlumX Metrics

1985CA26      Z.Phys. A321, 451 (1985)

B.Castel, A.G.M.Van Hees

Can Spin-Flip Quadrupole Resonances be Observed ( Question )

NUCLEAR STRUCTURE 16O; calculated E2 transition strength distribution; deduced GQR spin-flip strength region. Shell model.

doi: 10.1007/BF01411979
Citations: PlumX Metrics

1984CA07      Nucl.Phys. A415, 30 (1984)

B.Castel, A.G.M.Van Hees, L.Zamick

Electric Spin Resonances in Light Nuclei

NUCLEAR STRUCTURE 16O, 40Ca; calculated levels, dipole spin-flip strength distribution.

doi: 10.1016/0375-9474(84)90597-9
Citations: PlumX Metrics

1984CA11      Phys.Rev. C29, 1912 (1984)

B.Castel, A.G.M.Van Hees, H.Toki

Origin of M1 Strength in 16O

NUCLEAR STRUCTURE 16O; calculated M1 transition strengths; deduced enhancement mechanisms. Shell model, isobar excitation, core polarization, meson exchange.

doi: 10.1103/PhysRevC.29.1912
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1984VA06      Z.Phys. A315, 223 (1984)

A.G.M.van Hees, P.W.M.Glaudemans

A Shell-Model Treatment of (0 + 1) (h-bar x Omega) States in A = 4-16 Nuclei. (II)

NUCLEAR STRUCTURE 4,5,6,7,8,9,10,11He, 7,8,9,10,11,12Li, 8,9,10,11,12,13Be, 10,11,12,13,14B, 12,13,14,15C, 14,15,16N, 16O; calculated levels, B(λ), g, quadrupole moments. Shell model, spuriosity elimination.

1983CA24      Phys.Rev. C28, 2571 (1983)

B.Castel, A.G.M.van Hees

Distribution of E1 Spin Flip Strength in 12C

NUCLEAR STRUCTURE 12C; calculated spin-flip E1 transition strength distribution. Shell model.

doi: 10.1103/PhysRevC.28.2571
Citations: PlumX Metrics

1983NA09      Phys.Rev. C28, 642 (1983)

H.Nann, D.W.Miller, W.W.Jacobs, D.W.Devins, W.P.Jones, A.G.M.van Hees

1f7/2 Neutron Hole Strength in 59Ni with the 60Ni(p(pol), d)59Ni Reaction at 94 MeV

NUCLEAR REACTIONS 60Ni(polarized p, d), E=94 MeV; measured σ(Ed), σ(θ), analyzing power vs θ, Ed. 59Ni deduced levels, J, π, C2S. Enriched target. DWBA analysis, shell model comparison.

doi: 10.1103/PhysRevC.28.642
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0171.

1983VA08      Nucl.Phys. A396, 105c (1983)

A.G.M.Van Hees, P.W.M.Glaudemans

Normal- and Nonnormal-Parity States in p-Shell Nuclei

NUCLEAR STRUCTURE 4,5He, 6,7Li, 8,9,10,11Be, 10,11,12,13B, 12,13,14C, 14,15N, 16O; calculated levels, g, B(λ), quadrupole moments. Shell model, empirical parameters.

doi: 10.1016/0375-9474(83)90012-X
Citations: PlumX Metrics

1983VA31      Z.Phys. A314, 323 (1983)

A.G.M.van Hees, P.W.M.Glaudemans

A Translationally Invariant Shell-Model Treatment of (0 + 1)(h-bar x Omega) States in A = 4-16 Nuclei. (I)

NUCLEAR STRUCTURE 4He, 6,7Li, 9Be, 10,11B, 12,13,14C, 14,15N, 16O; calculated rms charge radii. 1,2,3,4H, 4,5,6,7,8,9He, 6,7,8,9,10,11Li, 9,10,11,12,13Be, 10,11,12,13,14B, 12,13,14,15C, 14,15,16N, 16,17O; calculated binding energies. 4,5He, 6,7Li, 8,9,10,11Be, 10,11,12,13B, 12,13,14C, 14,15N, 16O; calculated yrast nonnormal parity states. Shell model, harmonic oscillator basis.

1981MO19      Phys.Lett. 104B, 251 (1981)

R.B.M.Mooy, P.W.M.Glaudemans, A.G.M.van Hees

On the J-Dependence of Excitation Energies in fp-Shell Nuclei

NUCLEAR STRUCTURE A=52-60; calculated levels; deduced J-dependence. Statistical assumptions, shell model.

doi: 10.1016/0370-2693(81)90120-9
Citations: PlumX Metrics

1981VA25      Z.Phys. A303, 267 (1981)

A.G.M.van Hees, P.W.M.Glaudemans

Effects of Configuration Mixing on Predominantly f7/2(n) States in A = 52-55 Nuclei

NUCLEAR STRUCTURE 52,53,54Fe, 52,53Mn, 52Cr, 54Co; calculated levels, μ, quadrupole moments, B(λ), log ft, g. Shell model.

1979VA19      Z.Phys. A293, 327 (1979)

A.G.M.van Hees, P.W.M.Glaudemans, B.C.Metsch

The Influence of f7/2 Hole Configurations on Properties of 57-59Ni

NUCLEAR STRUCTURE 57,58,59Ni; calculated energy levels, B(λ), S, μ, quadrupole moment. Shell model, surface delta interactions.

1978GL06      Fizika, Suppl. 10, 57 (1978)

P.W.M.Glaudemans, R.J.G.Goossens, A.G.M.van Hees, B.C.Metsch, R.Vennink

Effects of 56Ni Core Excitations

NUCLEAR STRUCTURE 57Ni; calculated electromagnetic properties. Shell model, effective interactions.

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