NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = B.H.Wildenthal Found 178 matches. Showing 1 to 100. [Next]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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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) Shell-Model Calculations of the Neutron-Rich 40Cl Nucleus NUCLEAR STRUCTURE 40Cl; calculated levels. Shell model.
doi: 10.1103/PhysRevC.39.701
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
1989JI06 Phys.Rev. C40, 389 (1989) 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
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
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
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
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
1988CA09 Phys.Rev. C37, 1681 (1988) 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
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
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
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
1988JI04 Phys.Rev. C38, 2849 (1988) 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
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
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
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
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
1988XI01 Phys.Rev. C37, 1256 (1988) 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
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
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
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
1987BR27 Phys.Lett. 198B, 29 (1987) 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
1987BR30 Nucl.Phys. A474, 290 (1987) 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
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
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
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
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
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
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
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
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
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
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
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
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
1985BR29 At.Data Nucl.Data Tables 33, 347 (1985) 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
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
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
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
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
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
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
1984FO16 Phys.Rev. C30, 1063 (1984) 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
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
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
1983BR04 Phys.Rev. C27, 1296 (1983) 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
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
1983BR29 Phys.Rev. C28, 2397 (1983) 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
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
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
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
1981MC10 Phys.Lett. 103B, 173 (1981) 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
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
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
1980BR08 Phys.Rev. C21, 2107 (1980) Relative Importance of Neutron and Proton Components of Nuclear Transitions and Comparative π-/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
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
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
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
1980WI18 Phys.Rev. C22, 2260 (1980) 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
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
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
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
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
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
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
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
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
1979NA07 Phys.Rev. C19, 2146 (1979) (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
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
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
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
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
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
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
1978NA04 Phys.Rev. C17, 916 (1978) (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
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
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
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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