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Search: Author = B.H.Wildenthal

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1998VE01      Phys.Rev. C57, 1256 (1998)

J.Vernotte, G.Berrier-Ronsin, S.Fortier, E.Hourani, J.Kalifa, J.M.Maison, L.-H.Rosier, G.Rotbard, B.H.Wildenthal

25Mg(d, 3He)24Na Reaction at 29 MeV and a Spectroscopic Analysis of the Levels of 24Na

NUCLEAR REACTIONS 27Al, 29Si, 25Mg(d, 3He), E=29 MeV; measured σ(E(3He), θ). 24Na deduced levels, J, π, spectroscopic factors. DWBA analysis, shell model calculations.

doi: 10.1103/PhysRevC.57.1256
Citations: PlumX Metrics

1997BR07      Z.Phys. A357, 157 (1997)

J.Brenneisen, B.Erhardt, F.Glatz, Th.Kern, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal

The Structure of 32S I. Spectroscopy of the Highly-Excited States

NUCLEAR REACTIONS 29Si(α, n), E=14.4 MeV; measured neutron spectra, γn-coin, γn(θ). 31P(p, γ), E=2-3.3 MeV; measured Eγ, Iγ, γ(θ). 32S deduced high-spin levels, J, π, T, γ-branching ratios, T1/2, δ, B(M1). Other data input.

doi: 10.1007/s002180050231
Citations: PlumX Metrics

1997BR12      Z.Phys. A357, 377 (1997)

J.Brenneisen, B.Erhardt, F.Glatz, Th.Kern, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal

The Structure of 32S II. Shell Model Interpretation

NUCLEAR STRUCTURE 32S; calculated levels, Γγ, branching ratios, other aspects. Shell model.

doi: 10.1007/s002180050257
Citations: PlumX Metrics

1996BR06      Z.Phys. A354, 301 (1996)

J.Brenneisen, D.Grathwohl, B.Ehrhard, P.M.Endt, S.Fischer, M.Lickert, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal

Quantum Numbers of 26Al Levels Above 6 MeV Excitation Energy

NUCLEAR REACTIONS, ICPND 25Mg(p, γ), E=2-4 MeV; measured Eγ, Iγ, γ yield, γ(θ), anisotropies, resonance strengths. 26Al deduced levels, J, π, T, δ, IAR features.

doi: 10.1007/s002180050049
Citations: PlumX Metrics

1995BR16      Z.Phys. A352, 149 (1995)

J.Brenneisen, D.Grathwohl, M.Lickert, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal

The Structure of 28Si Above 10 MeV Excitation Energy I: Gamma-decay modes and radiative widths of levels

NUCLEAR REACTIONS 27Al(p, γ), E=1.097-4.492 MeV; 24Mg(α, γ), E=1.5-4 MeV; measured Eγ, Iγ. 27Al(d, nγ), E=4-6 MeV; measured nγ-coin, Eγ, Iγ. 28Si deduced levels, Γ, γ-branching ratios, resonance strengths.

doi: 10.1007/BF01298901
Citations: PlumX Metrics

1995BR17      Z.Phys. A352, 279 (1995)

J.Brenneisen, D.Grathwohl, M.Lickert, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal

The Structure of 28Si Above 10 MeV Excitation Energy II: Assignments of quantum numbers

NUCLEAR REACTIONS 27Al(p, γ), E not given; 24Mg(α, γ), E=3.355 MeV; measured Eγ, Iγ(θ). 28Si deduced levels, J, π, δ, T.

doi: 10.1007/BF01289501
Citations: PlumX Metrics

1995BR32      Z.Phys. A352, 403 (1995)

J.Brenneisen, D.Grathwohl, M.Lickert, R.Ott, H.Ropke, J.Schmalzlin, P.Siedle, B.H.Wildenthal

The Structure of 28Si Above 10 MeV Excitation Energy III: Level scheme and shell model interpretation

NUCLEAR STRUCTURE 28Si; analyzed data; deduced level scheme, J, π, T, γ-branching ratio. Shell model.

doi: 10.1007/BF01299758
Citations: PlumX Metrics

1995SE03      Phys.Rev.Lett. 74, 642 (1995); Erratum Phys.Rev.Lett. 74, 3306 (1995)

K.K.Seth, R.Soundranayagam, A.Saha, C.W.de Jager, H.de Vries, B.A.Brown, B.H.Wildenthal

Absence of M3 Quenching in 26Mg

NUCLEAR REACTIONS 26Mg(e, e'), E not given; measured σ(θ). 26Mg level deduced B(λ).

doi: 10.1103/PhysRevLett.74.642
Citations: PlumX Metrics

1994VE04      Nucl.Phys. A571, 1 (1994)

J.Vernotte, G.Berrier-Ronsin, J.Kalifa, R.Tamisier, B.H.Wildenthal

Spectroscopic Factors from One-Proton Stripping Reactions on sd-Shell Nuclei: Experimental Measurements and Shell-Model Calculations

NUCLEAR REACTIONS 16,18O, 19F, 23Na, 24,25,26Mg, 27Al, 28,29,30Si, 31P, 32,34S, 35,37Cl, 39K(3He, d), E=25 MeV; measured σ(θ); deduced bound proton optical potential parametrization. 17,19F, 20Ne, 24Mg, 25,26,27Al, 28Si, 29,30,31P, 32S, 33,35Cl, 36,38Ar, 40Ca levels deduced spectroscopic factors.

doi: 10.1016/0375-9474(94)90339-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2282.

1993RO06      Phys.Rev. C47, 1455 (1993)

J.D.Robertson, D.M.Moltz, T.F.Lang, J.E.Reiff, J.Cerny, B.H.Wildenthal

Beta-Delayed Proton Decay of 25Si

NUCLEAR REACTIONS 24Mg(3He, 2n), E=40 MeV; measured β-delayed proton spectra.

RADIOACTIVITY 25Si(β+p) [from 24Mg(3He, 2n), E=40 MeV]; measured β-delayed Ep, Ip; deduced log ft. 25Al deduced levels, J, π, T, branching ratios, Gamow-Teller transition strength.

doi: 10.1103/PhysRevC.47.1455
Citations: PlumX Metrics

1993VE03      Phys.Rev. C48, 205 (1993)

J.Vernotte, G.Berrier-Ronsin, S.Fortier, E.Hourani, J.Kalifa, J.M.Maison, L.H.Rosier, G.Rotbard, B.H.Wildenthal

27Al(d, 3He)26Mg Reaction at 29 MeV

NUCLEAR REACTIONS 27Al(d, 3He), E=29 MeV; measured σ(θ), σ(3He); deduced model parameters. 26Mg deduced levels, J, π, C2S. DWBA analysis. Model comparison.

doi: 10.1103/PhysRevC.48.205
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1148.

1991HE05      Z.Phys. A338, 23 (1991)

F.Heidinger, P.Betz, W.Brendler, F.Glatz, A.Hoffmann, H.Ropke, B.H.Wildenthal

The Structure of 25Mg

NUCLEAR REACTIONS 24Mg(d, p), E=6.5 MeV; measured σ(Ep). 22Ne(α, nγ), E=11.8-15.5 MeV; measured Eγ, Iγ, nγ-coin, nγ(θ). 25Mg deduced levels, J, π, branching ratio, δ, T1/2, B(λ), T. Shell model.

doi: 10.1007/BF01279113
Citations: PlumX Metrics

1991LI35      Phys.Rev. C44, 2413 (1991)

R.A.Lindgren, B.L.Clausen, G.S.Blanpied, J.Hernandez, C.S.Mishra, W.K.Mize, C.S.Whisnant, B.G.Ritchie, C.L.Morris, S.J.Seestrom-Morris, C.F.Moore, P.A.Seidl, B.H.Wildenthal, R.Gilman, J.A.Carr

Pion Scattering to 6- Stretched States in 24Mg and 26Mg

NUCLEAR REACTIONS 26,24Mg(π+, π+'), (π-, π-'), E=116-180 MeV; measured pion spectra, σ(θ). 26,24Mg levels deduced stretched configuration isoscalar, isovector strength.

doi: 10.1103/PhysRevC.44.2413
Citations: PlumX Metrics

1990BL04      Phys.Rev. C41, 1625 (1990)

G.S.Blanpied, J.Hernandez, C.S.Mishra, W.K.Mize, C.S.Whisnant, B.G.Ritchie, C.L.Morris, S.J.Seestrom-Morris, C.F.Moore, P.A.Seidl, R.A.Lindgren, B.H.Wildenthal, R.Gilman

Pion Elastic and Inelastic Scattering from 24Mg and 26Mg

NUCLEAR REACTIONS 26,24Mg(π+, π+'), (π-, π-'), E=150, 180 MeV; measured σ(θ), σ(E(π)). 26,24Mg levels deduced deformation parameters, neutron, proton matrix elements.

doi: 10.1103/PhysRevC.41.1625
Citations: PlumX Metrics

1990TI02      Phys.Rev. C42, 581 (1990)

P.Tikkanen, J.Keinonen, K.Arstila, A.Kuronen, B.H.Wildenthal

Lifetimes of the Lowest (5/2)+ and (9/2)+ States in the Mirror Nuclei 23Na-23Mg

NUCLEAR REACTIONS 12C(12C, p), (15N, α), (12C, n), E=15-27 MeV; measured DSA, nγ-coin, Eγ. 23Na, 23Mg levels deduced T1/2. Implanted enriched 12C targets.

doi: 10.1103/PhysRevC.42.581
Citations: PlumX Metrics

1990TI07      Nucl.Phys. A517, 176 (1990)

P.Tikkanen, J.Keinonen, A.Kuronen, A.Z.Kiss, E.Koltay, E.Pintye, B.H.Wildenthal

Short Lifetimes in 29Si-29P for the Test of Shell-Model Wave Functions

NUCLEAR REACTIONS 15N(16O, np), E=17, 20, 22 MeV; 28Si(p, γ), E=1.38, 1.65, 2.08, 2.29 MeV; measured DSA. 29Si, 29P levels deduced T1/2, δ, γ-branching. Implanted, enriched 15N, 28Si targets. Shell model comparison.

doi: 10.1016/0375-9474(90)90267-P
Citations: PlumX Metrics

1990VE04      Phys.Rev. C41, 1956 (1990)

J.Vernotte, A.Khendriche, G.Berrier-Ronsin, S.Grafeuille, J.Kalifa, G.Rotbard, R.Tamisier, B.H.Wildenthal

30Si(3He, d)31P Reaction at 25 MeV

NUCLEAR REACTIONS 30Si(3He, d), E=25 MeV; measured σ(θ). 31P deduced levels, S. DWBA analysis, shell model predictions.

doi: 10.1103/PhysRevC.41.1956
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1150.

1989ET01      Phys.Rev. C39, 680 (1989)

A.Etchegoyen, M.C.Etchegoyen, B.H.Wildenthal

Neutron-Proton Weak Coupling: Reducing shell-model dimensions by truncations in the neutron and proton subspaces

NUCLEAR STRUCTURE 20,22Ne; calculated levles, B(E2). Shell model truncations, separate neutron, proton subspaces.

doi: 10.1103/PhysRevC.39.680
Citations: PlumX Metrics

1989HO07      Z.Phys. A332, 289 (1989)

A.Hoffmann, P.Betz, H.Ropke, B.H.Wildenthal

Structure of the Mirror Nuclei 21Ne and 21Na

NUCLEAR REACTIONS 18O(α, nγ), E=12-15.4 MeV; measured nγ(θ), σ(En), nγ-coin. 18O(α, 2nγ), E=13.4 MeV; measured σ(En). 21Ne deduced levels, J, π, δ. Shell model comparison.

NUCLEAR STRUCTURE 21Ne, 21Na; calculated levels, Gamow-Teller matrix elements, T1/2. Shell model.

1989JI01      Phys.Rev. C39, 701 (1989)

X.Ji, B.H.Wildenthal

Shell-Model Calculations of the Neutron-Rich 40Cl Nucleus

NUCLEAR STRUCTURE 40Cl; calculated levels. Shell model.

doi: 10.1103/PhysRevC.39.701
Citations: PlumX Metrics

1989JI03      Nucl.Phys. A492, 215 (1989)

X.Ji, B.H.Wildenthal, M.Vallieres

A Generalized LS-Coupling Scheme for Shell-Model Calculations and Related Truncation Schemes

NUCLEAR STRUCTURE 58,60,62,64,66Ni; calculated leading wave function probability.

doi: 10.1016/0375-9474(89)90083-3
Citations: PlumX Metrics

1989JI06      Phys.Rev. C40, 389 (1989)

X.Ji, B.H.Wildenthal

Shell-Model Calculations for the Energy Levels of the N = 50 Isotones with A = 80-87

NUCLEAR STRUCTURE 80Zn, 81Ga, 82Ge, 83As, 84Se, 85Br, 86Kr, 87Rb; calculated levels, single nucleon transfer spectroscopic factors. Shell model.

doi: 10.1103/PhysRevC.40.389
Citations: PlumX Metrics

1989KE04      Nucl.Phys. A493, 124 (1989)

J.Keinonen, P.Tikkanen, A.Kuronen, A.Z.Kiss, E.Somorjai, B.H.Wildenthal

Short Lifetimes in 24Mg for Test of Rotational Collectivity in Shell-Model Wave Functions

NUCLEAR REACTIONS 23Na(p, γ), E=0.7, 1.7 MeV; 12C(14N, pn), E=20, 24 MeV; measured γ-spectra, DSA. 24Mg levels deduced T1/2. Implanted, enriched 23Na, 12C targets.

doi: 10.1016/0375-9474(89)90536-8
Citations: PlumX Metrics

1988BL04      Phys.Rev. C37, 1304 (1988)

G.S.Blanpied, B.G.Ritchie, M.L.Barlett, R.W.Fergerson, J.A.McGill, B.H.Wildenthal

Elastic and Inelastic Scattering of 0.8 GeV Protons from 40Ar

NUCLEAR REACTIONS 40Ar(p, p), (p, p'), E=0.8 GeV; measured σ(θ); deduced optical model parameters. 40Ar levels deduced deformation parameters. Collective model transition densities.

doi: 10.1103/PhysRevC.37.1304
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0690.

1988BL13      Phys.Rev. C38, 2180 (1988)

G.S.Blanpied, B.G.Ritchie, M.L.Barlett, R.W.Fergerson, G.W.Hoffmann, J.A.McGill, B.H.Wildenthal

Elastic and Inelastic Scattering of 0.8 GeV Protons from 20Ne and 22Ne

NUCLEAR REACTIONS 20,22Ne(p, p), (p, p'), E=0.8 GeV; measured σ(Ep), σ(θ). 22,20Ne levels deduced multipole moments, deformation lengths.

doi: 10.1103/PhysRevC.38.2180
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0688.

1988BR11      Ann.Phys.(New York) 182, 191 (1988)

B.A.Brown, W.A.Richter, R.E.Julies, B.H.Wildenthal

Semi-Empirical Effective Interactions for the 1s-0d Shell

NUCLEAR STRUCTURE A=17-39; analyzed binding energy data; deduced density dependent two-body potential parameters.

doi: 10.1016/0003-4916(88)90013-9
Citations: PlumX Metrics

1988CA09      Phys.Rev. C37, 1681 (1988)

M.Carchidi, B.H.Wildenthal

Rotational Collectivity in Shell-Model Wave Functions for A = 20-28 Nuclei

NUCLEAR STRUCTURE 20,22Ne, 24,26Mg, 28Si, 22Na; calculated levels, electric quadrupole matrix elements; deduced band features, rotational collectivity.

doi: 10.1103/PhysRevC.37.1681
Citations: PlumX Metrics

1988EN06      Nucl.Phys. A487, 221 (1988)

P.M.Endt, P.de Wit, C.Alderliesten, B.H.Wildenthal

Spins, Parities and Isospins of 26Al Levels: Shell-model aspects

NUCLEAR REACTIONS 25Mg(p, γ), E=0.31-1.84 MeV; analyzed data. 26Al levels deduced J, π, isospin. Other data input.

doi: 10.1016/0375-9474(88)90611-2
Citations: PlumX Metrics

1988ET01      Phys.Rev. C38, 1382 (1988)

M.C.Etchegoyen, A.Etchegoyen, B.H.Wildenthal, B.A.Brown, J.Keinonen

Analysis of Magnetic Dipole Transitions between sd-Shell States

NUCLEAR STRUCTURE A=18-38; calculated B(M1); deduced effective magnetic dipole operator. Shell model.

doi: 10.1103/PhysRevC.38.1382
Citations: PlumX Metrics

1988HE15      Phys.Rev. C38, 1698 (1988)

D.M.Headly, R.K.Sheline, S.L.Tabor, U.J.Huttmeier, C.J.Gross, E.F.Moore, B.H.Wildenthal, H.R.Weller, R.M.Whitton, I.Ragnarsson

Gamma Decay of High Spin States in 25Mg above 6.1 MeV

NUCLEAR REACTIONS 12C(14N, p), E=23.5 MeV; measured Eγ, Iγ, pγ(θ). 25Mg deduced levels, J, π, δ, band structure, deformation length. Shell model, cranked Nilsson-Strutinsky model.

NUCLEAR STRUCTURE 25Mg; calculated levels, potential energy surfaces, rotational bands. Shell model, cranked Nilsson-Strutinsky model.

doi: 10.1103/PhysRevC.38.1698
Citations: PlumX Metrics

1988JI04      Phys.Rev. C38, 2849 (1988)

X.Ji, B.H.Wildenthal

Shell-Model Predictions for Electromagnetic Properties of N = 50 Nuclei

NUCLEAR STRUCTURE 86Kr, 87Rb, 88Sr, 89Y, 90Zr, 91Nb, 92Mo, 93Tc, 94Ru, 95Rh, 96Pd; calculated levels, B(λ). Shell model.

doi: 10.1103/PhysRevC.38.2849
Citations: PlumX Metrics

1988KA06      Nucl.Phys. A480, 175 (1988)

T.Kajino, E.Shiino, H.Toki, B.A.Brown, B.H.Wildenthal

Beta Decay Rates of sd-Shell Nuclei in Stellar Interiors

NUCLEAR STRUCTURE 26Al, 30,31,32,33S, 34,35Cl; calculated stellar evolution related β-decay rates, Gamow-Teller matrix elements. Shell model, effective interaction.

doi: 10.1016/0375-9474(88)90391-0
Citations: PlumX Metrics

1988LI31      Z.Phys. A331, 409 (1988)

M.Lickert, J.Brenneisen, F.Glatz, D.Grathwohl, A.Martinez v.Remisowski, H.Ropke, J.Siefert, B.H.Wildenthal

The Structure of 27Al

NUCLEAR REACTIONS 24Mg(α, pγ), E=14.2, 15, 15.6 MeV; measured proton spectra, Eγ, Iγ, pγ-coin, pγ(θ). 26Mg(p, γ), E=1.82-2.574 MeV; measured γ(θ). 27Al deduced levels, J, π, δ, γ-branching ratios, B(λ), T1/2. Shell model.

NUCLEAR STRUCTURE 27Al; calculated levels, γ-branching ratios, T1/2, B(λ). Shell model.

1988LO12      Phys.Rev. C38, 2902 (1988)

L.Losano, H.Dias, F.Krmpotic, B.H.Wildenthal

Comparisons between Shell-Model Calculations, Seniority Truncation, and Quasiparticle Approximations: Application to the odd Ni isotopes and odd N = 82 isotones

NUCLEAR STRUCTURE 59,61,63,65Ni, 135I, 137Cs, 139La, 141Pr, 143Pm; calculated levels, μ, quadrupole moments, B(λ). Shell model.

doi: 10.1103/PhysRevC.38.2902
Citations: PlumX Metrics

1988MO13      Phys.Rev. C37, 2428 (1988)

R.Moreh, W.M.Sandefur, W.C.Sellyey, D.C.Sutton, B.H.Wildenthal

Ground State M1 Strength of d5/2-1 Levels in 39K

NUCLEAR REACTIONS 39K(γ, γ'), E=6.6, 8.5, 9.4 MeV bremsstrahlung; measured Eγ, Iγ. 39K levels deduced Γ, (gΓ02/Γ), B(M1).

doi: 10.1103/PhysRevC.37.2428
Citations: PlumX Metrics

1988WI17      Phys.Rev. C38, 285 (1988)

J.A.Winger, J.C.Hill, F.K.Wohn, R.L.Gill, X.Ji, B.H.Wildenthal

Test of the Singly Magic Character of the N = 50 Isotone 83As Populated in 83Ge Decay

RADIOACTIVITY 83Ge(β-); measured T1/2, Eγ, Iγ, γγ-coin; deduced log ft. 83As deduced levels, J, π, β-branching. Ge(Li) detector. Shell model.

doi: 10.1103/PhysRevC.38.285
Citations: PlumX Metrics

1988XI01      Phys.Rev. C37, 1256 (1988)

Xiangdong Ji, B.H.Wildenthal

Effective Interaction for N = 50 Isotones

NUCLEAR STRUCTURE 82Ge, 83As, 84Se, 85Br, 86Kr, 87Rb, 88Sr, 89Y, 90Zr, 91Nb, 92Mo, 93Tc, 94Ru, 95Rh, 96Pd; calculated binding energy, levels. Shell model, effective interaction.

doi: 10.1103/PhysRevC.37.1256
Citations: PlumX Metrics

1987AN13      Phys.Rev. C36, 2195 (1987)

B.D.Anderson, T.Chittrakarn, A.R.Baldwin, C.Lebo, R.Madey, P.C.Tandy, J.W.Watson, C.C.Foster, B.A.Brown, B.H.Wildenthal

Gamow-Teller and M1 Strength in the 32S(p, n)32Cl Reaction at 135 MeV

NUCLEAR REACTIONS, MECPD 32S(p, n), E=135 MeV; measured σ(E, θ), σ(θ). 32Cl deduced Gamow-Teller transition strength, M1 transition strength, DWIA analysis.

doi: 10.1103/PhysRevC.36.2195
Citations: PlumX Metrics

1987BA46      Phys.Rev. C36, 765 (1987)

P.Baumann, Ph.Dessagne, A.Huck, G.Klotz, A.Knipper, G.Marguier, C.Miehe, M.Ramdane, C.Richard-Serre, G.Walter, B.H.Wildenthal

Gamow-Teller Beta Decay of 29Na and Comparison with Shell-Model Predictions

RADIOACTIVITY 29Na(β-n) [from U(p, X), E=600 MeV]; measured Eγ, Iγ, β-delayed En, I(n), γγ-, nγ-coin, T1/2; deduced log ft, Gamow-Teller transition strength. 29Mg deduced levels, J, π, T1/2, β-branching ratios. Ge(Li), BaF2, plastic detectors. Shell model.

doi: 10.1103/PhysRevC.36.765
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1987BL07      Phys.Rev. C35, 1567 (1987)

G.S.Blanpied, C.S.Mishra, G.S.Adams, B.M.Preedom, C.S.Whisnant, J.-P.Egger, C.L.Morris, H.Breuer, N.S.Chant, B.G.Ritchie, B.H.Wildenthal, B.Hoistad, B.A.Brown

(π±, p) Reactions at Low Excitation Energy

NUCLEAR REACTIONS 24Mg, 27Al, 40Ca, 58Ni(π+, p), (π-, p), E=120 MeV; 12C(π-, p), E=145 MeV; measured σ(θ(π), E(π)); deduced σ(π+)/σ(π-), pion absorption mechanism.

doi: 10.1103/PhysRevC.35.1567
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1987BR27      Phys.Lett. 198B, 29 (1987)

B.A.Brown, B.H.Wildenthal

Prediction of A New High-Spin Mode of Transverse Excitation in Electron Scattering from Nuclei

NUCLEAR REACTIONS 26Mg(e, e'), E not given; calculated transverse form factor. 26Mg deduced high spin transverse excitation mode. Shell model.

doi: 10.1016/0370-2693(87)90151-1
Citations: PlumX Metrics

1987BR30      Nucl.Phys. A474, 290 (1987)

B.A.Brown, B.H.Wildenthal

Empirically Optimum M1 Operator for sd-Shell Nuclei

NUCLEAR STRUCTURE A=17, 28, 39; calculated effective g-factors; deduced effective M1 matrix elements. Shell model.

doi: 10.1016/0375-9474(87)90619-1
Citations: PlumX Metrics

1987HE26      Phys.Lett. 198B, 433 (1987)

D.M.Headly, R.K.Sheline, S.L.Tabor, U.J.Huttmeier, C.J.Gross, E.F.Moore, B.H.Wildenthal, H.R.Weller, R.M.Whitton, I.Ragnarsson

High-Spin States and Rotational Coexistence in 25Mg

NUCLEAR REACTIONS 12C(14N, pγ), E=23.5 MeV; measured Eγ, Iγ, pγ-, γγ-coin. 25Mg deduced levels, J, π, γ-multipolarity. E-ΔE telescope, Ge(Li) detectors.

doi: 10.1016/0370-2693(87)90894-X
Citations: PlumX Metrics

1987MA19      Phys.Rev. C35, 2011 (1987); Erratum Phys.Rev. C36, 1647 (1987)

R.Madey, B.S.Flanders, B.D.Anderson, A.R.Baldwin, C.Lebo, J.W.Watson, S.M.Austin, A.Galonsky, B.H.Wildenthal, C.C.Foster

Gamow-Teller Strength in the 26Mg(p, n)26Al Reaction at 135 MeV and Its Fractionation into T=0, 1, and 2 Isospin Channels

NUCLEAR REACTIONS, MECPD 26Mg(p, n), E=134.4 MeV; measured σ(En); deduced σ(θ). 26Al deduced levels, J, π, T, Gamow-Teller transition strength distribution. Tof. DWIA.

doi: 10.1103/PhysRevC.35.2011
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0133.

1987NE04      Phys.Rev. C35, 890 (1987)

B.T.Neyer, D.L.Clark, J.S.Dunham, W.A.Seale, J.L.Thornton, R.T.Westervelt, S.S.Hanna, B.A.Brown, B.H.Wildenthal

Lifetime of the Lowest 0+, T = 1 State of 22Na

NUCLEAR REACTIONS 19F(α, n), E=4.3 MeV; measured Doppler shift, recoil. 22Na level deduced T1/2, M1 transition characteristics, analog β-decay Gamow-Teller transition comparison.

doi: 10.1103/PhysRevC.35.890
Citations: PlumX Metrics

1987SA03      Nucl.Phys. A462, 1 (1987)

H.Sawaga, O.Scholten, B.A.Brown, B.H.Wildenthal

Core Polarization Effects on Transition Densities in Medium-Heavy Nuclei

NUCLEAR STRUCTURE 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm; calculated levels; 144Sm, 122Sn; calculated core polarization charges; 110Pd, 116,122Sn, 134Te, 136Xe, 138Ba, 140Ce, 142Nd, 144Sm, 146Gd, 148Dy, 150Er; calculated transition densities, B(E2); 110Pd, 116Sn, 134Te, 138Ba, 142Nd, 146Gd; calculated Coulomb form factors. Hartree-Fock-RPA method.

doi: 10.1016/0375-9474(87)90376-9
Citations: PlumX Metrics

1987TI03      Phys.Rev. C36, 32 (1987)

P.Tikkanen, J.Keinonen, R.Lappalainen, B.H.Wildenthal

Short Lifetimes in 30P

NUCLEAR STRUCTURE 30P; calculated levels, B(λ). Shell model.

NUCLEAR REACTIONS 29Si(p, γ), E=1.4-2.1 MeV; measured DSA. 30P deduced levels, T1/2, γ-branching ratio, B(λ). Shell model.

doi: 10.1103/PhysRevC.36.32
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1987VO01      Phys.Rev. C35, 921 (1987)

R.Vodhanel, R.Moreh, W.C.Sellyey, M.K.Brussel, B.H.Wildenthal

M1 Radiation Widths in 27Al

NUCLEAR REACTIONS 27Al(γ, γ'), E=7.66, 10.37 MeV; measured σ(E, θ). 27Al deduced levels, (gΓ0), B(M1). Shell model.

doi: 10.1103/PhysRevC.35.921
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1986AL06      Nucl.Phys. A454, 189 (1986)

W.P.Alford, J.A.Cameron, E.Habib, B.H.Wildenthal

Two-Neutron Excitations in 26Mg and 30Si

NUCLEAR REACTIONS 24Mg, 28Si(t, p), E=18 MeV; measured σ(Ep, θ). 30Si deduced level, J, π. DWBA analysis, shell model comparison. Enriched 24Mg target.

doi: 10.1016/0375-9474(86)90264-2
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1986AL15      Nucl.Phys. A457, 317 (1986)

W.P.Alford, P.Craig, D.A.Lind, R.S.Raymond, J.Ullman, C.D.Zafiratos, B.H.Wildenthal

Structure of 22Mg, 26Si, 34Ar and 38Ca via the (3He, n) Reaction

NUCLEAR REACTIONS 20Ne, 24Mg, 32S, 36Ar(3He, n), E=25.4 MeV; measured σ(E(n), θ). 22Mg, 26Si, 34Ar, 38Ca deduced levels, L, J, π, analogs. Tof. DWBA, shell model analyses.

doi: 10.1016/0375-9474(86)90381-7
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1986CA27      Phys.Rev. C34, 2280 (1986)

M.Carchidi, B.H.Wildenthal, B.A.Brown

Quadrupole Moments of sd-Shell Nuclei

NUCLEAR STRUCTURE 17,18O, 17,18,19,20F, 20,21,22Ne, 23Na, 24,25,26Mg, 27Al, 28,30Si, 32,33,34,35,36S, 35,36,37Cl, 36,38Ar, 39K; calculated charge radii, quadrupole moments. Shell model.

doi: 10.1103/PhysRevC.34.2280
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1986GL05      Z.Phys. A324, 173 (1986)

F.Glatz, M.Lickert, A.Burkard, Th.Kern, R.Lehmann, S.Norbert, H.Ropke, J.Siefert, B.H.Wildenthal

Search for Missing Predicted High-Spin States in 28Si

NUCLEAR REACTIONS 27Al(p, γ), E=1.911, 2.073 keV; measured Eγ, Iγ, γ(θ), linear polarization, DSA. 28Si deduced levels, J, π, T, K, rotational band structure, Γγ. Shell model comparison.

1986GL06      Z.Phys. A324, 187 (1986)

F.Glatz, S.Norbert, E.Bitterwolf, A.Burkard, F.Heidinger, Th.Kern, R.Lehmann, H.Ropke, J.Siefert, C.Schneider, B.H.Wildenthal

High-Spin States in 26Mg

NUCLEAR REACTIONS 23Na(α, pγ), E=14.2, 16 MeV; measured σ(Ep), pγ-coin, pγ(θ), DSA. 26Mg deduced levels, J, π, T1/2, K, γ-branching, δ, B(λ), intrinsic quadrupole moments, rotational band structure, prolate to oblate deformation transition.

1985AY02      Phys.Rev. C32, 1700 (1985)

J.Aysto, X.J.Xu, D.M.Moltz, J.E.Reiff, J.Cerny, B.H.Wildenthal

Beta-Delayed Proton Decays of 27P and 31Cl: Gamow-Teller decays with large Q values

RADIOACTIVITY 27P(β+p) [from 28Si(p, 2n), E=28-50 MeV]; 31Cl(β+p) [from 32S(p, 2n), E=28-50 MeV]; measured β-delayed Ep, Ip, T1/2; deduced β-branching, log ft. 27Si, 31S deduced Gamow-Teller strength function, levels, proton branching.

doi: 10.1103/PhysRevC.32.1700
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1985BE04      Phys.Rev. C31, 570 (1985)

Z.Berant, A.Wolf, J.C.Hill, F.K.Wohn, R.L.Gill, H.Mach, M.Rafailovich, H.Kruse, B.H.Wildenthal, G.Peaslee, A.Aprahamian, J.Goulden, C.Chung

g Factor of 4+1 States in the N = 82 Isotones 136Xe and 138Ba

RADIOACTIVITY 136I, 138Cs(β-); measured γγ(θ, H, t). 136Xe, 138Ba levels deduced g.

doi: 10.1103/PhysRevC.31.570
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1985BR15      Phys.Rev. C32, 1127 (1985)

B.A.Brown, B.H.Wildenthal, C.F.Williamson, F.N.Rad, S.Kowalski, H.Crannell, J.T.O'Brien

Shell-Model Analysis of High-Resolution Data for Elastic and Inelastic Electron Scattering on 19F

NUCLEAR REACTIONS 19F(e, e'), E=78-340 MeV; measured σ(E, θ); deduced longitudinal, transverse form factors. Shell model comparison.

NUCLEAR STRUCTURE 19F; calculated shell model wave functions; deduced electron scattering form factors, effective charges. Comparison with data.

doi: 10.1103/PhysRevC.32.1127
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1985BR29      At.Data Nucl.Data Tables 33, 347 (1985)

B.A.Brown, B.H.Wildenthal

Experimental and Theoretical Gamow-Teller Beta-Decay Observables for the sd-Shell Nuclei

NUCLEAR STRUCTURE A=17-39; analyzed Gamow-Teller decay data. Shell model, effective one-body operator, densities.

doi: 10.1016/0092-640X(85)90009-9
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1985WA24      Phys.Rev.Lett. 55, 1369 (1985)

J.W.Watson, W.Pairsuwan, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, R.J.McCarthy, B.A.Brown, B.H.Wildenthal, C.C.Foster

Relationship between Gamow-Teller Transition Proabilities and (p, n) Cross Sections at Small Momentum Transfers

NUCLEAR REACTIONS 14C, 15N, 17,18O, 26Mg, 39K(p, n), E=135 MeV; measured σ(θ), σ(θn, En). 13C, 19F(p, n), E=160 MeV; analyzed σ(θ). 14N, 15O, 17,18F, 26Al, 39Ca levels deduced Gamow-Teller transitions. DWBA analysis, β-decay input.

doi: 10.1103/PhysRevLett.55.1369
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1985WI17      Phys.Rev. C32, 2185 (1985)

B.H.Wildenthal, B.A.Brown, I.Sick

Electric Hexadecupole Transition Strength in 32S and Shell-Model Predictions for E4 Systematics in the sd Shell

NUCLEAR STRUCTURE 20,22Ne, 18O, 24,26Mg, 28,30Si, 32,34S, 36,38Ar; calculated E4 matrix elements. Shell model.

NUCLEAR REACTIONS 32S(e, e'), E=250, 500 MeV; calculated E2, E4 form factors. Shell model.

doi: 10.1103/PhysRevC.32.2185
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1984AN05      Phys.Rev.Lett. 52, 1409 (1984)

N.Anantaraman, B.A.Brown, G.M.Crawley, A.Galonsky, C.Djalali, N.Marty, M.Morlet, A.Willis, J.-C.Jourdain, B.H.Wildenthal

Observation of Quenching in Isoscalar and Isovector 0+ → 1+ Transitions in 28Si(p, p')

NUCLEAR REACTIONS 28Si(p, p'), E=201 MeV; measured σ(Ep'), σ(θ). 28Si levels deduced excitation σ, B(M1), isoscalar, isovector channel quenching. DWIA calculations.

doi: 10.1103/PhysRevLett.52.1409
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1984BE26      Phys.Lett. 140B, 191 (1984)

U.E.P.Berg, K.Ackermann, K.Bangert, C.Blasing, W.Naatz, R.Stock, K.Wienhard, M.K.Brussel, T.E.Chapuran, B.H.Wildenthal

Bound State M1 Transitions in sd-Shell Nuclei

NUCLEAR REACTIONS 20,22Ne, 24Mg, 28,30Si, 32,34S(γ, γ'), E=65 MeV bremsstrahlung; 26Mg(γ, γ'), E not given; measured Eγ, Iγ. 22Ne, 26Mg, 28,30Si, 32,34S(polarized γ, γ), E=22 MeV bremsstrahlung; measured γ asymmetry, polarization effect. 20,22Ne, 24,26Mg, 28,30Si, 32,34S levels deduced B(M1), (Γ0/Γ), Γ0. Nuclear resonance fluorescence technique, linearly polarized γ-beam. Shell model comparison.

doi: 10.1016/0370-2693(84)90918-3
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1984BL14      Phys.Rev. C30, 1233 (1984)

G.S.Blanpied, G.A.Balchin, G.E.Langston, B.G.Ritchie, M.L.Barlett, G.W.Hoffmann, J.A.McGill, M.A.Franey, M.Gazzaly, B.H.Wildenthal

Excitation of the Ground State Rotational Band in 20Ne by 0.8 GeV Protons

NUCLEAR REACTIONS 20Ne(polarized p, p'), E=0.8 GeV; measured σ(θ), analyzing power vs θ, σ(Ep'); deduced potential parameters. 20Ne levels deduced β, B(λ). Coupled-channels calculation.

doi: 10.1103/PhysRevC.30.1233
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1984BL18      Nucl.Phys. A431, 237 (1984)

L.C.Bland, H.T.Fortune, D.L.Watson, M.A.Abouzeid, B.H.Wildenthal

The 27Al(t, p)29Al Reaction at E(t) = 15 MeV

NUCLEAR REACTIONS 27Al(t, p), E=15 MeV; measured σ(θ). 29Al deduced levels L, J, π. DWBA analysis, shell model comparison.

doi: 10.1016/0375-9474(84)90173-8
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1984FO16      Phys.Rev. C30, 1063 (1984)

H.T.Fortune, B.H.Wildenthal

Level Densities in 20F: Experimental, shell model, and weak coupling results

NUCLEAR STRUCTURE 20F; calculated levels; deduced basis, model dependences. Shell model, weak coupling model.

doi: 10.1103/PhysRevC.30.1063
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1984WI17      Prog.Part.Nucl.Phys. 11, 5 (1984)


Empirical Strengths of Spin Operators in Nuclei

NUCLEAR STRUCTURE A=17-39; calculated wave functions, Gamow-Teller, magnetic dipole, other spin-type operator matrix elements. Shell model, effective Hamiltonian simple parametrization.

doi: 10.1016/0146-6410(84)90011-5
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1983AN05      Phys.Rev. C27, 1387 (1983)

B.D.Anderson, A.Fazely, R.J.McCarthy, P.C.Tandy, J.W.Watson, R.Madey, W.Bertozzi, T.N.Buti, J.M.Finn, J.Kelly, M.A.Kovash, B.Pugh, B.H.Wildenthal, C.C.Foster

Gamow-Teller Strength in the 18O(p, n)18F Reaction at 135 MeV

NUCLEAR REACTIONS 18O(p, n), E=135.2 MeV; measured σ(En), σ(θ). 18F deduced levels, J, π, T, Gamow-Teller transition strength. DWIA analysis.

doi: 10.1103/PhysRevC.27.1387
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1983BR04      Phys.Rev. C27, 1296 (1983)

B.A.Brown, B.H.Wildenthal

Strengths of Transitions between 0+ and 1+ States and Their Relationship to Inelastic Electron Scatteing Form Factors: Example of 24Mg

NUCLEAR REACTIONS 24Mg(e, e'), E not given; calculated form factors. Shell model.

NUCLEAR STRUCTURE 24Mg; calculated M1, Gamow-Teller transition strengths. Shell model.

doi: 10.1103/PhysRevC.27.1296
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1983BR27      Phys.Lett. 133B, 5 (1983)

B.A.Brown, R.Radhi, B.H.Wildenthal

Simultaneous Analysis of Magnetic Moments and Elastic Magnetic Electron Scattering Form Factors

NUCLEAR STRUCTURE 19F, 29Si, 31P; analyzed momentum dependent μ; deduced M1 operator momentum transfer, configuration mixing effect dependence. DWBA, shell model wave functions, elastic electron scattering data input.

doi: 10.1016/0370-2693(83)90092-8
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1983BR29      Phys.Rev. C28, 2397 (1983)

B.A.Brown, B.H.Wildenthal

Corrections to the Free-Nucleon Values of the Single-Particle Matrix Elements of the M1 and Gamow-Teller Operators, from a Comparison of Shell-Model Predictions with sd-Shell Data

NUCLEAR STRUCTURE A=17-39; analyzed magnetic dipole moment, B(M1), Gamow-Teller β-decay data; deduced effective single particle operator matrix elements. Complete shell model basis, empirical Hamiltonian.

doi: 10.1103/PhysRevC.28.2397
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1983WI08      Phys.Rev. C28, 1343 (1983)

B.H.Wildenthal, M.S.Curtin, B.A.Brown

Predicted Features of the Beta Decay of Neutron-Rich sd-Shell Nuclei

RADIOACTIVITY 21,22,23,24,25,26,27,28O, 23,24,25,26,27,28,29F, 25,26,27,28,29,30Ne, 27,28,29,30,31Na, 29,30,31,32Mg, 31,32,33Al, 33,34Si, 35P(β-); calculated Q, T1/2, log ft, Gamow-Teller transition strength, branching to daughter residual states. Shell model.

doi: 10.1103/PhysRevC.28.1343
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1982BE33      Phys.Rev. C26, 720 (1982)

K.B.Beard, J.Kasagi, E.Kashy, B.H.Wildenthal, D.L.Freisel, H.Nann, R.E.Warner

(d, 2He) Reaction at E(d) = 99 MeV

NUCLEAR REACTIONS 12C(d, 2p), E=99.2 MeV; measured σ(E(2He)), σ(θ). Sum, difference spectra, Watson-Migdal final state interaction.

doi: 10.1103/PhysRevC.26.720
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1982BR24      Phys.Rev. C26, 2247 (1982)

B.A.Brown, B.H.Wildenthal, W.Chung, S.E.Massen, M.Bernas, A.M.Bernstein, R.Miskimen, V.R.Brown, V.A.Madsen

Isovector E2 Matrix Elements from Electromagnetic Transitions in the s-d shell: Experiment and shell-model calculations.

NUCLEAR STRUCTURE A=17-39; calculated B(E2) for isovector transitions; deduced isovector effective charge. Shell model.

doi: 10.1103/PhysRevC.26.2247
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1981MC10      Phys.Lett. 103B, 173 (1981)

J.B.McGrory, B.H.Wildenthal

Shell-Model Calculation of M1 Scattering Strengths in 42,44,48Ca

NUCLEAR STRUCTURE 42,44,48Ca; calculated levels, B(M1). Shell model, complete f-, p-shell space.

doi: 10.1016/0370-2693(81)90734-6
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1981NA01      Phys.Rev. C23, 606 (1981)

H.Nann, A.Saha, B.H.Wildenthal

Energy Levels in 23Mg from the 25Mg(p, t)23Mg Reaction

NUCLEAR REACTIONS 25Mg(p, t), E=40 MeV; measured σ(Et, θ). 23Mg deduced levels, L, J, π. DWBA analysis, shell model spectroscopic amplitudes. Enriched target.

doi: 10.1103/PhysRevC.23.606
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1980BE43      Phys.Rev. C22, 1872 (1980)

M.Bernas, F.Pougheon, M.Roy-Stephan, G.P.A.Berg, B.Berthier, J.P.Le Fevre, B.H.Wildenthal

24Mg(18O, 16O)26Mg Reaction at E(18O) = 50 MeV Including Scattering in Entrance and Exit Channel

NUCLEAR REACTIONS 24Mg(18O, 16O), E=50 MeV; measured σ(θ, E(18O)); 24Mg(18O, 18O), (18O, 18O'), E=50 MeV; 26Mg(16O, 16O), (16O, 16O'), E=56 MeV; measured σ(θ); deduced optical model parameters. Microscopic exact finite-range DWBA, CCBA analyses, shell model wave functions.

doi: 10.1103/PhysRevC.22.1872
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1980BR08      Phys.Rev. C21, 2107 (1980)

B.A.Brown, B.H.Wildenthal

Relative Importance of Neutron and Proton Components of Nuclear Transitions and Comparative π-+ Inelastic Scattering

NUCLEAR REACTIONS 18O(π-, π-'), 26Mg(π+, π+'), E=164, 180, 230 MeV; calculated σ(π-)/σ(π+), T=1 component of transition strength. Shell model.

doi: 10.1103/PhysRevC.21.2107
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1980BR09      Phys.Rev. C21, 2600 (1980)

B.A.Brown, W.Chung, B.H.Wildenthal

Inelastic Scattering E4 Transition Probabilities in the 0d, 1s Shell

NUCLEAR STRUCTURE 18O, 19F, 20,22Ne, 24,25,26Mg, 28,30Si, 32,34S, 36,38Ar; calculated B(E4), α-, pion-inelastic scattering strengths, isoscalar effective charges. Full s-, d-shell space, Chung-Wildenthal Hamiltonian, shell model.

doi: 10.1103/PhysRevC.21.2600
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1980BR13      Phys.Rev. C22, 774 (1980)

B.A.Brown, W.Chung, B.H.Wildenthal

Electromagnetic Multipole Moments of Ground States of Stable Odd-Mass Nuclei in the sd Shell

NUCLEAR STRUCTURE 17O, 21Ne, 23Na, 25Mg, 27Al, 33S, 35,37Cl, 39K; calculated M1, M3, M5, E2, E4 ground state moments. Shell model, s-, d-shell space, Chung-Wildenthal Hamiltonian.

doi: 10.1103/PhysRevC.22.774
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1980BR14      Phys.Rev. C22, 842 (1980)

B.A.Brown, S.E.Massen, W.Chung, B.H.Wildenthal, T.A.Shibata

Effective M3 Operator and Relevant Transitions in 24Al, 24Na, 34Cl, 38K, and 38Cl

NUCLEAR STRUCTURE 24Na, 24Al, 34,38Cl, 38K; calculated B(M3); deduced effective M3 operator. Shell model, s-, d-shell space, Chung-Wildenthal Hamiltonian.

doi: 10.1103/PhysRevC.22.842
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1980WI18      Phys.Rev. C22, 2260 (1980)

B.H.Wildenthal, W.Chung

Collapse of the Conventional Shell-model Ordering in the Very-Neutron-Rich Isotopes of Na and Mg

NUCLEAR STRUCTURE 20,21,23,24,25,26,27,28,29,30Na, 20,22,24,26,28,30,32Mg; calculated binding energies, μ, levels. 20,21,22,23,24,25Ne; calculated binding energies. Chung-Wildenthal Hamiltonian, s-, d-shell included.

doi: 10.1103/PhysRevC.22.2260
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1979BE07      Phys.Rev. C19, 1099 (1979)

C.L.Bennett, H.W.Fulbright, J.F.A.van Hienen, W.Chung, B.H.Wildenthal

α-Particle Spectroscopy in Ni and Zn

NUCLEAR REACTIONS Ni(6Li, d), E not given; calculated Sα. Shell model.

doi: 10.1103/PhysRevC.19.1099
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1979BE20      Phys.Rev. C19, 2246 (1979)

M.Bernas, M.Roy-Stephan, F.Pougheon, M.Langevin, G.Rotbard, P.Roussel, J.P.LeFevre, M.C.Lemaire, K.S.Low, B.H.Wildenthal

Mechanism of the 26Mg(18O, 16O)28Mg Reaction at E = 50 MeV and the Energy Levels of 28Mg

NUCLEAR REACTIONS 26Mg(18O, 16O), E=50 MeV; measured σ(θ). 28Mg deduced levels, reaction mechanism. DWBA, CCBA analysis, shell-model wave functions. Enriched target.

doi: 10.1103/PhysRevC.19.2246
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1979BI05      Phys.Rev. C20, 1221 (1979)

J.N.Bishop, L.R.Medsker, H.T.Fortune, B.H.Wildenthal

17O(3He, p)19F and the Structure of 19F

NUCLEAR REACTIONS 17O(3He, p), E=18.0 MeV. 19F deduced levels, L, π. DWBA analysis.

doi: 10.1103/PhysRevC.20.1221
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1979CH04      Phys.Rev. C19, 530 (1979)

W.Chung, H.T.Fortune, B.H.Wildenthal

α-Transfer Spectroscopic Factors in 23Na

NUCLEAR STRUCTURE 23Na; calculated Sα in full sd basis of shell model. Comparison with SU(3).

doi: 10.1103/PhysRevC.19.530
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1979FO06      Phys.Rev. C19, 1147 (1979)

H.T.Fortune, J.N.Bishop, H.Nann, B.H.Wildenthal

Parity of 19F (5.10) and 19Ne (5.09)

NUCLEAR REACTIONS 17O(3He, p), E=18.0 MeV; 21Ne(p, t), E=40 MeV; measured σ(θ). 19F, 19Ne levels deduced L, π. DWBA analysis. Enriched targets.

doi: 10.1103/PhysRevC.19.1147
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1979FO17      Phys.Lett. 87B, 29 (1979)

H.T.Fortune, L.Bland, R.Middleton, W.Chung, B.H.Wildenthal

Systematics of Ground-State (t, p) Cross Sections in the 2s-1d Shell

NUCLEAR REACTIONS 16,18O, 20,22Ne, 32,34S, 36Ar(t, p), E=15 MeV; measured σ(θ) two-neutron binding energies. DWBA analysis, enriched gas targets.

doi: 10.1016/0370-2693(79)90009-1
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1979LA18      Phys.Rev. C20, 1673 (1979)

S.LaFrance, H.T.Fortune, S.Mordechai, M.E.Cobern, G.E.Moore, R.Middleton, W.Chung, B.H.Wildenthal

20O from 18O(t, p)

NUCLEAR REACTIONS 18O(t, p), E=15.0 MeV; measured σ(Ep, θ). 20O deduced levels, L, π, J. DWBA analysis, shell, weak-coupling models. Enriched gas target.

doi: 10.1103/PhysRevC.20.1673
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1979ME12      Phys.Rev. C20, 2130 (1979)

M.C.Mermaz, A.Greiner, B.T.Kim, M.A.G.Fernandes, N.Lisbona, E.Muller, W.Chung, B.H.Wildenthal

Multinucleon Transfer Reactions Induced by 18O on 28Si

NUCLEAR REACTIONS 28Si(18O, 16O), (18O, 20Ne), (18O, 22Ne), (18O, 15N), (18O, 15O), E=56 MeV; measured σ(θ). DWBA analysis; shell-model analysis.

doi: 10.1103/PhysRevC.20.2130
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1979NA07      Phys.Rev. C19, 2146 (1979)

H.Nann, B.H.Wildenthal

(p, t) and (p, 3He) Reactions on 33S

NUCLEAR REACTIONS 33S(p, t), (p, 3He), E=40 MeV; measured σ(Et, θ), σ(E(3He), t). 31S level deduced Q. 31P, 31S levels deduced L, J, π. Enriched target. DWBA analysis.

doi: 10.1103/PhysRevC.19.2146
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1978CH26      Phys.Lett. 79B, 381 (1978)

W.Chung, J.van Hienen, B.H.Wildenthal, C.L.Bennett

Shell-Model Predictions of Alpha-Spectroscopic Factors between Ground States of 16 ≤ A ≤ 40 Nuclei

NUCLEAR STRUCTURE 20,21,22Ne, 24,25,26Mg, 28,29,30Si, 32,33,34S, 36,37,38Ar, 39K, 40Ca; calculated Sα for ground state to ground state transitions using shell model comparison with SU(3).

doi: 10.1016/0370-2693(78)90387-8
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1978CH35      Fizika, Suppl. 10, 15 (1978)

W.Chung, J.van Hienen, B.H.Wildenthal, C.L.Bennett

Ground-State Alpha-Cluster Correlation in sd-Shell Nuclei

NUCLEAR STRUCTURE A=20-40; calculated Sα for ground-state transitions. Shell model.

1978FO11      Nucl.Phys. A301, 441 (1978)

H.T.Fortune, L.R.Medsker, H.Nann, B.H.Wildenthal

Study of the 17O(α, d)19F Reaction

NUCLEAR REACTIONS 17O(α, d), E=47.5 MeV; measured σ(Ed, θ). DWBA analysis. Enriched target.

doi: 10.1016/0375-9474(78)90060-X
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1978FO15      Phys.Rev. C18, 1 (1978)

H.T.Fortune, J.R.Powers, R.Middleton, H.Nann, B.H.Wildenthal

21Ne(3He, p)23Na Reaction

NUCLEAR REACTIONS 21Ne(3He, p), E=18.0 MeV; measured σ(Ep, θ). 23Na deduced levels, L, J, π. DWBA analysis with shell-model wave functions. Enriched gas target.

doi: 10.1103/PhysRevC.18.1
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1978FO22      Phys.Rev.Lett. 41, 527 (1978)

H.T.Fortune, J.N.Bishop, L.R.Medsker, B.H.Wildenthal

Direct Determination of [(sd)3]5/2 1/2(1p-2)01 Component In 17O(g.s.)

NUCLEAR STRUCTURE 17O; calculated 3p, 2h configuration in ground state.

NUCLEAR REACTIONS 17O(3He, α), E=18 MeV; calculated σ(θ).

doi: 10.1103/PhysRevLett.41.527
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1978FO26      Phys.Rev. C18, 1563 (1978)

H.T.Fortune, H.Nann, B.H.Wildenthal

Configuration of 19Ne(4.033, 3/2+)

NUCLEAR REACTIONS 21Ne(p, t), E=40 MeV; measured σ(Et, θ). 19Ne levels deduced configuration. DWBA with microscopic wave functions.

doi: 10.1103/PhysRevC.18.1563
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1978KA18      Phys.Rev. C17, 1961 (1978)

J.Kalifa, J.Vernotte, Y.Deschamps, F.Pougheon, G.Rotbard, M.Vergnes, B.H.Wildenthal

31P(3He, d)32S Reaction at 25 MeV

NUCLEAR REACTIONS 31P(3He, 3He), E=25 MeV; measured σ(θ); deduced optical model parameters. 31P(3He, d), E=25 MeV; measured σ(Ed, θ). 32S deduced levels, L, T, J, π, S. DWBA analysis.

doi: 10.1103/PhysRevC.17.1961
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1978NA04      Phys.Rev. C17, 916 (1978)

H.Nann, B.H.Wildenthal

(p, t) and (p, 3He) Reactions on 39K

NUCLEAR REACTIONS 39K(p, t), (p, 3He), E=40 MeV; measured σ(θ). 37K, 37Ar deduced levels, L. Natural target, DWBA analysis.

doi: 10.1103/PhysRevC.17.916
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1978ZA07      Phys.Lett. 80B, 26 (1978)

H.Zarek, S.Yen, B.O.Pich, T.E.Drake, C.F.Williamson, S.Kowalski, C.P.Sargent, W.Chung, B.H.Wildenthal, M.Harvey, H.C.Lee

Electroexcitation and the Determination of the K-Band Structure in 24Mg

NUCLEAR REACTIONS 24Mg(e, e'), E=218.1 MeV; measured σ. 24Mg levels deduced E2, E4 Coulomb form factors. Comparison with theory suggests K-band structure.

doi: 10.1016/0370-2693(78)90297-6
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1977CA11      Phys.Rev. C15, 2178 (1977)

F.P.Calaprice, W.Chung, B.H.Wildenthal

Calculation of Recoil-Order Matrix Elements for the Beta Decays of 20F And 20Na

RADIOACTIVITY 20F, 20Ne, 20Na; calculated β-shape spectrum, M1, E2 matrix elements, form factors.

doi: 10.1103/PhysRevC.15.2178
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1977FO09      Phys.Lett. 70B, 408 (1977)

H.T.Fortune, R.Middleton, M.E.Cobern, G.E.Moore, S.Mordechai, R.V.Kollarits, H.Nann, W.Chung, B.H.Wildenthal

Spectroscopy of 16C

NUCLEAR REACTIONS 14C(t, p), E=15, 17, 18 MeV; measured σ(Ep, θ). 16C deduced levels, J, π, configuration.

doi: 10.1016/0370-2693(77)90400-2
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