NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = E.K.Warburton Found 238 matches. Showing 1 to 100. [Next]1996RA04 Phys.Rev. C53, 616 (1996) S.Raman, E.K.Warburton, J.W.Starner, E.T.Jurney, J.E.Lynn, P.Tikkanen, J.Keinonen Spectroscopy of 20F Levels NUCLEAR REACTIONS 19F(n, γ), E=thermal; measured Eγ, Iγ. 20F deduced levels, J, π, γ-branching ratios, spectroscopic strengths, γ multipolarity. Other reaction data input.
doi: 10.1103/PhysRevC.53.616
1994HO12 Phys.Rev. C50, 775 (1994) M.Horoi, G.Clausnitzer, B.A.Brown, E.K.Warburton New Calculations of the Parity Nonconservation Matrix Element for J(πT) 0+1, 0-1 Doublet in 14N NUCLEAR STRUCTURE 14N; calculated levels, B(λ), isoscalar parity nonconserving matrix element. Shell model.
doi: 10.1103/PhysRevC.50.775
1994ME02 Phys.Rev. C49, 743 (1994) B.Meltzow, E.K.Warburton, Ch.Ender, J.Gerl, D.Habs, U.Lauff, J.Schirmer, D.Schwalm, P.Thirolf Measurement and Significance of Γ(γ)/Γ for the 7117-keV 4+ Level of 18O NUCLEAR REACTIONS 12C(7Li, p), (7Li, pγ), E=18 MeV; measured Ep, pγ-coin. 18O level deduced Γγ/Γ, B(λ). Shell model.
doi: 10.1103/PhysRevC.49.743
1994WA01 Phys.Rev. C49, 824 (1994) E.K.Warburton, I.S.Towner, B.A.Brown First-Forbidden β Decay: Meson-exchange enhancement of the axial charge at A ≈ 16 NUCLEAR STRUCTURE 11Be, 15,16N(β-); calculated two-body exchange current, one-body impulse approximation matrix elements; deduced axial-charge matrix element multiplicative factor. Shell model.
doi: 10.1103/PhysRevC.49.824
1993CH06 Phys.Rev. C47, 163 (1993) W.-T.Chou, E.K.Warburton, B.A.Brown Gamow-Teller Beta-Decay Rates for A ≤ 18 Nuclei NUCLEAR STRUCTURE 1n, 3H, 6,8He, 7,12Be, 8,9,11Li, 8,12,13,14B, 9,10,11,14,15,16,18C, 12,13,16,17,18N, 13,14,15O; analyzed Gamow-Teller β-decay data; deduced log ft, β-decay matrix elements. Effective operators, discussed specific decays.
doi: 10.1103/PhysRevC.47.163
1992CH09 Phys.Rev. C45, 1720 (1992) Construction of Shell-Model Interactions for Z ≈ 50, N ≈ 82 Nuclei: Predictions for A = 133-134 β- decays NUCLEAR STRUCTURE 133,134Sn, 134Sb; analyzed β-decay data; calculated β-decay shape factors. 141Ce, 134Sn, 134Sb, 134Te; calculated β-decay matrix elements, branching ratios. Shell model, effective interactions.
doi: 10.1103/PhysRevC.45.1720
1992KA27 Z.Phys. A343, 165 (1992) M.K.Kabadiyski, F.Cristancho, C.J.Gross, A.Jungclaus, K.P.Lieb, D.Rudolph, H.Grawe, J.Heese, K.-H.Maier, J.Eberth, S.Skoda, W.-T.Chou, E.K.Warburton A Study of High Spin States in the Transitional Nucleus 90Mo NUCLEAR REACTIONS 58Ni(36Ar, 4p), E=149 MeV; measured γγ-, γγ(particle)-coin, DCO ratios. 90Mo deduced levels, J, π, γ-branching ratios. Shell model comparison.
doi: 10.1007/BF01291821
1992WA02 Phys.Rev. C45, 463 (1992) Second-Forbidden Unique β Decays of 10Be, 22Na, and 26Al RADIOACTIVITY 10Be(β-); 22Na(β+); 26Al(β+), (EC); calculated second-forbidden decay unique matrix elements shell model.
doi: 10.1103/PhysRevC.45.463
1992WA22 Phys.Rev. C46, 923 (1992) Effective Interactions for the 0p1s0d Nuclear Shell-Model Space NUCLEAR STRUCTURE A=13-20; calculated mass, neutron separation energies. 20F, 15,17,19,16,18,20,10B, 10Be; calculated levels. A=11-22; calculated exotic neutron rich nuclei Coulomb energies. Effective interactions, 0p1s0d shell model space. RADIOACTIVITY 16C(β-); calculated Gamow-Teller transition strength. Effective interactions, 0p1s0d shell model space.
doi: 10.1103/PhysRevC.46.923
1992WA25 Phys.Lett. 293B, 7 (1992) E.K.Warburton, B.A.Brown, D.J.Millener Large-Basis Shell-Model Treatment of A = 16 NUCLEAR STRUCTURE 16O; calculated levels. Large basis shell model. RADIOACTIVITY 16N(β-); calculated unique first forbidden β-decay matrix element. Large basis shell model.
doi: 10.1016/0370-2693(92)91472-L
1992WA28 Phys.Lett. 294B, 1 (1992) Renormalization of the Axial Charge at A ≈ 132 NUCLEAR STRUCTURE 133,134Sn, 134Sb; calculated mesonic exchange contributions to axial charge in first-forbidden β-decay; deduced other effects contribution estimates. Shell model.
doi: 10.1016/0370-2693(92)91629-N
1991BE06 Phys.Rev. C43, 1639 (1991) Z.Berant, R.B.Schuhmann, D.E.Alburger, W.T.Chou, R.L.Gill, E.K.Warburton, C.Wesselborg Spectroscopy of 214Bi and Systematics of 210,212,214Pb(0+) → β- 210,212,214Bi(0-) RADIOACTIVITY 214Pb(β-); measured γγ-coin, γγ(θ), I(ce), Eγ, Iγ, βγγ-coin. 214Bi deduced levels, J, π, T1/2. Shell model.
doi: 10.1103/PhysRevC.43.1639
1991WA01 Phys.Rev. C43, 602 (1991) Appraisal of the Kuo-Herling Shell-Model Interaction and Application to A = 210-212 Nuclei NUCLEAR STRUCTURE A=204-212; calculated levels, binding energies, μ. Shell model.
doi: 10.1103/PhysRevC.43.602
1991WA16 Phys.Rev.Lett. 66, 1823 (1991) Mesonic Enhancement of the Weak Axial-Vector Current Evaluated from β Decay in the Lead Region NUCLEAR STRUCTURE A=205-212; analyzed first forbidden β-decay data; deduced weak axial-vector current mesonic enhancement. Shell model.
doi: 10.1103/PhysRevLett.66.1823
1991WA17 Phys.Rev. C44, 233 (1991) First-Forbidden β Decay in the Lead Region and Mesonic Enhancement of the Weak Axial Current NUCLEAR STRUCTURE A=205-212; analyzed first-forbidden β-decay, related processes data. Shell model, weak axial current mesonic enhancement.
doi: 10.1103/PhysRevC.44.233
1991WA18 Phys.Rev. C44, 261 (1991) Shell-Model Interpretation of the β- Decay of 212gBi, 212m1Bi, and 212m2Bi NUCLEAR STRUCTURE 212Bi, 212Po; calculated levels. 212Bi deduced isomers, J, π, β-decay rate. Shell model.
doi: 10.1103/PhysRevC.44.261
1991WA19 Phys.Rev. C44, 268 (1991) Shell-Model Predictions for 41,42Cl(β-)41,42Ar and the A = 41-43 Ar Isotopes NUCLEAR STRUCTURE 41,42Cl; calculated levels, binding energies, β-decay rates. 41,42,43Ar; calculated levels. 41Ar; calculated B(λ). Shell model.
doi: 10.1103/PhysRevC.44.268
1991WA22 Phys.Rev. C44, 1500 (1991) Shell-Model Description of 211Bi(β-)211Po and 211At(EC)211Po and the Spectroscopy of 211Po NUCLEAR STRUCTURE 211Po; calculated levels, spectroscopic factors. Shell model. RADIOACTIVITY 211Bi(β-); 211At(EC); calculated log ft. Shell model wave functions.
doi: 10.1103/PhysRevC.44.1500
1991WA23 Phys.Rev. C44, 1024 (1991) In-Medium and Core-Polarization Effects in 50K(0-) (β-) → 50Ca(0+) RADIOACTIVITY 50K(β-); calculated β-decay features; deduced in-medium, core polarization effects role. Shell model.
doi: 10.1103/PhysRevC.44.1024
1990KR06 Phys.Rev. C42, 878 (1990) A.J.Kreiner, J.Davidson, M.Davidson, P.Thieberger, E.K.Warburton Rotational Structures in 181,182,183Ir NUCLEAR REACTIONS, ICPND 172Yb(14N, 4n), (14N, 5n), 174Yb(14N, 5n), E=65-83 MeV; measured γγ(t), Eγ, Iγ, σ(E), γ(θ), γ(X-ray)-coin. 181,182,183Ir deduced levels, J, π, band structure.
doi: 10.1103/PhysRevC.42.878
1990MA03 Phys.Rev. C41, 226 (1990) H.Mach, E.K.Warburton, R.L.Gill, R.F.Casten, J.A.Becker, B.A.Brown, J.A.Winger Meson-Exchange Enchancement of the First-Forbidden 96gY(0-) → 96gZr(0+) β Transition: β decay of the low-spin isomer of 96Y RADIOACTIVITY 96Y(β-) [from 96Rb decay chain]; measured Eγ, Iγ, γγ(t), βγ-coin, I(ce); deduced Qβ, T1/2. 96Zr deduced levels, J, π, E0 transition strengths. Shell model calculations. NUCLEAR STRUCTURE 96Y; calculated β-transition strength. Shell model.
doi: 10.1103/PhysRevC.41.226
1990MA40 Phys.Rev. C42, 568 (1990) H.Mach, E.K.Warburton, W.Krips, R.L.Gill, M.Moszynski Evidence for the Contribution of 0f5/2, 1p3/2 Proton Excitations in the Low-Lying States in 92,94Zr RADIOACTIVITY 92,94Y(β-) [from 92,94Rb β-decay chain]; measured βγγ-coin, βγ(t). 92,94Zr levels deduced T1/2, B(E2), configuration. Shell model.
doi: 10.1103/PhysRevC.42.568
1990WA02 Phys.Rev. C41, 1147 (1990) E.K.Warburton, J.A.Becker, B.A.Brown Mass Systematics for A = 29-44 Nuclei: The deformed A ≈ 32 region NUCLEAR STRUCTURE A=29-44; calculated levels, binding energy, B(λ), quadrupole moments; deduced island of inversion anomaly evidence. Shell model.
doi: 10.1103/PhysRevC.41.1147
1990WA20 Phys.Rev. C42, 2479 (1990) Core Polarization Effects on Spin-Dipole and First-Forbidden β-Decay Operators in the Lead Region NUCLEAR STRUCTURE 206Hg, 206Tl; calculated spin-dipole, first forbidden β-decay transition matrix elements; deduced tensor interaction role. Realistic shell model effective interactions.
doi: 10.1103/PhysRevC.42.2479
1990WI12 Phys.Rev. C42, 956 (1990) J.A.Winger, J.C.Hill, F.K.Wohn, E.K.Warburton, R.L.Gill, A.Piotrowski, R.B.Schuhmann, D.S.Brenner Structure of 76Zn from 76Cu Decay and Systematics of Neutron-Rich Zn Nuclei RADIOACTIVITY 76Cu(β-); measured Eγ, Iγ, γγ-coin. 76Zn deduced levels, J, π. Shell model. NUCLEAR STRUCTURE 68,70,72,74,76Zn; calculated levels. Shell model.
doi: 10.1103/PhysRevC.42.956
1989AL24 Phys.Rev. C40, 2789 (1989) D.E.Alburger, E.K.Warburton, Z.Tao Half-Life of 56Co RADIOACTIVITY 56Co(β+); measured Eγ, Iγ, γ-decay peaks; deduced T1/2. Ge(Li) spectrometer.
doi: 10.1103/PhysRevC.40.2789
1989AL25 Phys.Rev. C40, 2891 (1989) D.E.Alburger, E.K.Warburton, Z.Tao New Gamma Ray in the Decay of 56Co RADIOACTIVITY 56Co(β+); measured Eγ, Iγ. 56Fe deduced level, transition Iγ, branching ratio, B(M1), γ-multipolarity, possible J, π.
doi: 10.1103/PhysRevC.40.2891
1989LO02 Phys.Scr. 39, 56 (1989) T.Lonnroth, C.W.Beausang, D.B.Fossan, L.Hildingsson, W.F.Piel, Jr., E.K.Warburton Very-High-Spin and Core-Coupled States in 213Rn. A Test of the Applicability of the Deformed Independent Particle Model NUCLEAR REACTIONS 204Hg(14C, 6n), (14C, 5n), E=80-90 MeV; measured σ(E(γ), E), γ(θ), γγ(t), I(ce). 213,212Rn deduced levels, J, π, γ-transitions, γ-multipolarity, B(λ).
1989WA06 Phys.Rev. C39, 1120 (1989) Structure of 17C and 17N NUCLEAR STRUCTURE 17C; calculated levels, β-decay observables. 17N; calculated levels, B(λ). Shell model. NUCLEAR REACTIONS 18O(3He, d), E not given; calculated spectroscopic factors. Shell model.
doi: 10.1103/PhysRevC.39.1120
1989WA09 Phys.Rev. C39, 1535 (1989) Shell Model Study of 40S(β-)40Cl and the Energy Levels of 40Cl RADIOACTIVITY 40S(β-); calculated first-forbidden β-decay, T1/2, shell model. NUCLEAR STRUCTURE 40S, 40Cl; calculated levels, masses, binding energy, B(λ). Shell model.
doi: 10.1103/PhysRevC.39.1535
1989WA28 Phys.Rev. C40, 2823 (1989) Shell-Model Study of 39S(β-)39Cl and the Energy Levels of 39Cl NUCLEAR STRUCTURE 39S; calculated levels, binding energy, β-decay log ft, branching ratio, Gamow-Teller transition strength. 39Cl; calculated levels, binding energy, μ, quadrupole moment, T1/2, B(λ), single nucleon transfer spectroscopic factors. Shell model, effective interactions.
doi: 10.1103/PhysRevC.40.2823
1989WI11 Phys.Rev. C39, 1976 (1989) J.A.Winger, J.C.Hill, F.K.Wohn, E.K.Warburton, R.L.Gill, A.Piotrowski, D.S.Brenner Structure of Neutron-Rich 74Zn from 74Cu Decay and Shell-Model Calculations for Even-A Zn Nuclei RADIOACTIVITY 74Cu(β-); calculated Eγ, Iγ, γγ-coin, T1/2. 74Zn deduced levels, J, π. Shell model. NUCLEAR STRUCTURE 74Cu; calculated levels, B(E2). 62,68,69Ni, 68,70,72,74,67,69,71,73Cu, 68,70,72,74,69,71,73Zn; calculated binding energy. Shell model.
doi: 10.1103/PhysRevC.39.1976
1988AL01 J.Phys.(London) G14, 229 (1988) D.E.Alburger, E.K.Warburton, J.A.Becker Decay of 87Y NUCLEAR REACTIONS 87Sr(p, n), (p, 2np), (p, 2n2p), E=18 MeV; measured Eγ, Iγ; deduced evidence for 85Sr, 83Rb decay. RADIOACTIVITY 87Y(β+), (EC); 85Sr, 83Rb(EC); measured Eγ, Iγ. 87Y deduced log ft. 87Sr deduced levels, γ-branching. 85Rb, 83Kr deduced transitions.
doi: 10.1088/0305-4616/14/2/015
1988AL27 Phys.Rev. C38, 1843 (1988) First-Forbidden 0+ → 0-, 1- Electron Capture of 44Ti RADIOACTIVITY 44Ti(EC); measured Eγ, Iγ, (X-ray)γ(t), γγ(t). 44Sc levels deduced (EC), γ-branching, T1/2. Shell model. NUCLEAR STRUCTURE 44Ti, 44Sc; calculated wave functions, β-, γ-transition features. Shell model.
doi: 10.1103/PhysRevC.38.1843
1988BA67 Nucl.Phys. A487, 269 (1988) The Beta-Decay of 8He RADIOACTIVITY 8He(β-); calculated T1/2, branching ratio, delayed n, t spectra; deduced Gamow-Teller matrix elements. R-matrix, shell model methods.
doi: 10.1016/0375-9474(88)90613-6
1988KR17 Nucl.Phys. A489, 525 (1988) A.J.Kreiner, J.Davidson, M.Davidson, P.Thieberger, E.K.Warburton, S.Andre, J.Genevey Band Structure of 184Ir NUCLEAR REACTIONS 174Yb(14N, 4n), E=65-80 MeV; 175Lu(13C, 4n), E=64 MeV; 176Lu(12C, 4n), E=68 MeV; 174Yb(14N, 4n), E=68 MeV; 176Yb(14N, 6n), E=96 MeV; measured E(γ), I(γ), σ(E, Eγ, θγ, t), γγ(t). 184Ir deduced levels, J, π, alignments, inertia parameters. Ge detectors, enriched targets. Particle-rotor and cranking analysis.
doi: 10.1016/0375-9474(88)90010-3
1988LI07 Z.Phys. A329, 413 (1988) C.J.Lister, B.J.Varley, W.Fieber, J.Heese, K.P.Lieb, E.K.Warburton, J.W.Olness Structure of High Spin States in 83Y NUCLEAR REACTIONS 58Ni(28Si, 3p), E=100 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), recoil distance Doppler shift. 83Y deduced levels, T1/2, J, π, δ(E2/M1), B(λ), transition quadrupole moments, branching ratios, yrast band features.
1988WA04 Phys.Rev. C37, 754 (1988) Shell-Model Description of the β- Decay of the N = 21 and 22 Isotones 34Al, 36Si, and 37P NUCLEAR STRUCTURE 34Al, 34,35,36Si, 35,36,37P, 37S; calculated levels, branching ratios, log ft, B(λ), β-decay T1/2. Shell model.
doi: 10.1103/PhysRevC.37.754
1988WA17 Phys.Rev. C38, 935 (1988) Shell Model Predictions for 19N(β-)19O NUCLEAR STRUCTURE 19N, 19O; calculated levels, wave functions. Shell model. RADIOACTIVITY 19N; calculated β-decay T1/2, decay modes. Shell model.
doi: 10.1103/PhysRevC.38.935
1988WA26 Nucl.Instrum.Methods Phys.Res. A272, 791 (1988) G.Wang, E.K.Warburton, D.E.Alburger Precision Energy Determinations of Gamma Transitions from 56Co Decay RADIOACTIVITY 56Co(EC), (β+); measured Eγ, Iγ. 56Fe deduced transition energies. 110mAg, 124Sb, 182Ta, 144Ce(β-); measured Eγ, Iγ for standardization. 108mAg, 58Co, 56Ni measured Eγ. Mixed source, γ-ray energy standard technique, high precision.
doi: 10.1016/0168-9002(88)90761-9
1988WA28 Phys.Rev. C38, 2822 (1988) 43K(β-)43Ca and the Structure of 43K and 43Ca RADIOACTIVITY 43K(β-) [44Ca(t, α), E=3.2 MeV]; measured Eγ, Iγ. 43Ca deduced levels, β-, γ-branching ratios. Ge(Li) detector. Shell model.
doi: 10.1103/PhysRevC.38.2822
1988WA30 Ann.Phys.(New York) 187, 471 (1988) E.K.Warburton, J.A.Becker, B.A.Brown, D.J.Millener First-Forbidden Beta Decay Near A = 40 NUCLEAR STRUCTURE A=34-44; calculated first forbidden β-decay transition strengths. Shell model.
doi: 10.1016/0003-4916(88)90156-X
1987AL06 Phys.Rev. C35, 1479 (1987) D.E.Alburger, G.Wang, E.K.Warburton Beta Decay of 20O RADIOACTIVITY 20O(β-); measured Eγ, Iγ; deduced β- branching, logft. 20F levels deduced γ-branching, allowed, first-forbidden unique, nonunique transition strength. Ge-NaI(Tl) Compton-suppression spectrometer.
doi: 10.1103/PhysRevC.35.1479
1987CO11 Phys.Rev. C35, 1939 (1987) P.D.Cottle, M.Gai, J.F.Ennis, J.F.Shriner, Jr., S.M.Sterbenz, D.A.Bromley, C.W.Beausang, L.Hildingsson, W.F.Piel, Jr., D.B.Fossan, J.W.Olness, E.K.Warburton Yrast States of 216Rn and the Extent of a Region of Possible Static Intrinsic Reflection Asymmetry NUCLEAR REACTIONS 208Pb(14C, 2nα), E=67-68 MeV; measured Eγ, Iγ, γ(θ), γγ-, γ(X-ray)-coin. 216Rn deduced levels, J, π, yrast scheme. Hyperpure Ge, Ge(Li) detectors.
doi: 10.1103/PhysRevC.35.1939
1987CO36 Phys.Rev. C36, 2286 (1987) P.D.Cottle, M.Gai, J.F.Ennis, J.F.Shriner, Jr., D.A.Bromley, C.W.Beausang, L.Hildingsson, W.F.Piel, Jr., D.B.Fossan, J.W.Olness, E.K.Warburton Level Spectrum of 219Ra and Weak Coupling in the Light Actinide Region NUCLEAR REACTIONS, ICPND 208Pb(14C, 3n), E=60-78 MeV; measured Eγ, Iγ, γ(θ), I(ce), thick target yield, σ(E). 219Ra deduced levels, J, π, ICC, B(λ) ratios, γ-multipolarity. Weak coupling model.
doi: 10.1103/PhysRevC.36.2286
1987GA15 Phys.Rev. C36, 1256 (1987) M.Gai, R.Keddy, D.A.Bromley, J.W.Olness, E.K.Warburton Spectroscopy of 18O: Radiative capture, 14C(α, γ)18O NUCLEAR REACTIONS, ICPND 14C(α, γ), E=1.7-2.7 MeV; measured γ yield vs E. 18O deduced resonances, B(λ), γ-multipolarity, γ-branching, Γγ, Γ, Γα/Γ, α-reduced widths.
doi: 10.1103/PhysRevC.36.1256
1987WA10 Phys.Rev. C35, 1851 (1987) Shell-Model Description of the Beta Decay of the N = 21 Isotones 35Si and 36P NUCLEAR STRUCTURE 35Si, 35,36P, 36S; calculated binding energies. Shell model. RADIOACTIVITY 36P, 35Si(β-); calculated T1/2, log ft, branching ratio, Gamow-Teller transition strengths, Eγ, Γγ. 35P, 36S deduced levels, B(λ), decay characteristics. Shell model.
doi: 10.1103/PhysRevC.35.1851
1987WA12 Phys.Rev. C35, 2272 (1987) G.Wang, E.K.Warburton, D.E.Alburger Beta Decay of 39Cl RADIOACTIVITY 39Cl(β-) [from 37Cl(t, p), E=3.1 MeV]; measured Eγ, Iγ; deduced log ft. 39Ar deduced levels, J, π, β-branching, Gamow-Teller, unique first forbidden transition strengths. NUCLEAR REACTIONS 37Cl(t, p), E=3-1 MeV; measured Eγ, Iγ. Compton-suppression γ-ray spectrometer.
doi: 10.1103/PhysRevC.35.2272
1987WA13 Phys.Rev. C35, 2278 (1987) Structure of 39Ar NUCLEAR STRUCTURE 39Ar; calculated binding energies, levels, single neutron transfer spectroscopic factors, B(λ), branching ratios, T1/2. Shell model calculations.
doi: 10.1103/PhysRevC.35.2278
1987WA14 Phys.Rev. C36, 429 (1987) E.K.Warburton, D.E.Alburger, G.Wang Confirmation of the 2805-keV Level of 38S NUCLEAR REACTIONS 36S(t, pγ), E=3.2 MeV; measured γγ-coin. 38S deduced level.
doi: 10.1103/PhysRevC.36.429
1987WA28 Nucl.Instrum.Methods Phys.Res. A260, 413 (1987) G.Wang, D.E.Alburger, E.K.Warburton Precision Energy and Intensity Measurements for γ Transitions from 134Cs Decay RADIOACTIVITY 134Cs(β-); measured Eγ, Iγ; deduced log ft. 134Ba deduced levels, Iβ, decay scheme.
doi: 10.1016/0168-9002(87)90109-4
1986CH01 Phys.Rev. C33, 130 (1986) T.Chapuran, K.Dybdal, D.B.Fossan, T.Lonnroth, W.F.Piel, Jr., D.Horn, E.K.Warburton High-Spin γ-Ray Spectroscopy in 197Bi NUCLEAR REACTIONS, ICPND 192Pt(10B, 5n), E=50-80 MeV; measured σ(Eγ, E), γγ-coin, γ(θ), γγ(t), gamma-ray yields. 197Bi deduced levels, J, π, isomers, T1/2, configurations, B(λ), yrast sequence.
doi: 10.1103/PhysRevC.33.130
1986CO05 Phys.Rev. C33, 1855 (1986) P.D.Cottle, M.Gai, J.F.Ennis, J.F.Shriner, Jr., D.A.Bromley, C.W.Beausang, L.Hildingsson, W.F.Piel, Jr., D.B.Fossan, J.W.Olness, E.K.Warburton Intermediate and Weak Coupling in 219Ra NUCLEAR REACTIONS 208Pb(14C, 3n), E=60-78 MeV; measured Eγ, Iγ, γ(θ). 219Ra deduced levels, γ-branching, J, π, rotational band. Weak coupling model.
doi: 10.1103/PhysRevC.33.1855
1986KR09 Phys.Rev. C34, 1150 (1986) A.J.Kreiner, P.Thieberger, E.K.Warburton Doubly Decoupled Structure in 182,184Ir NUCLEAR REACTIONS 172,174Yb(14N, 4n), E=65-83 MeV; measured Eγ, Iγ, γγ(t), γ(θ), σ(Eγ, E). 182,184Ir deduced levels, J, π, configuration, alignments. Enriched targets, γ-ray spectroscopy techniques.
doi: 10.1103/PhysRevC.34.1150
1986LO05 Phys.Rev. C33, 1641 (1986) T.Lonnroth, C.W.Beausang, D.B.Fossan, L.Hildingsson, W.F.Piel, Jr., M.A.Quader, S.Vajda, T.Chapuran, E.K.Warburton Excited States in Neutron-Deficient 195Bi NUCLEAR REACTIONS, ICPND 182W(19F, 6n), E=85-135 MeV; 169Tm(30Si, 4n), E=142 MeV; measured Eγ, Iγ, γγ(t), γ(t), I(ce), relative γ yields. 195Bi deduced levels, J, π, δ, ICC. Enriched targets, Ge(Li), Si(Li) detectors, mini-orange magnetic spectrometer. Shell model comparison.
doi: 10.1103/PhysRevC.33.1641
1986LO13 Phys.Scr. 34, 669 (1986) T.Lonnroth, J.Hattula, V.Koponen, E.K.Warburton Medium-Spin Structure of the N = 28 Isotones 54Fe and 55Co NUCLEAR REACTIONS 54Fe(3He, 3He'), (3He, d), (3He, n2p), (3He, pn), (3He, pd), E=27 MeV; measured Eγ, Iγ, γ(θ), γγ-coin. 54Fe, 55Co deduced levels, J, π, shapes, deformation parameters. Enriched target, Ge detector. NUCLEAR STRUCTURE 58Ni; calculated proton, neutron levels. Hartree-Fock calculations.
1986OL08 Phys.Rev. C34, 2049 (1986) J.W.Olness, E.K.Warburton, J.A.Becker, D.J.Decman, E.A.Henry, L.G.Mann, L.Ussery 36S(t, pγ)38S Reaction NUCLEAR STRUCTURE 38S; calculated levels, B(λ). Shell model. NUCLEAR REACTIONS 36S(t, pγ), E ≤ 7 MeV; measured pγ-coin, pγ(θ). 38S deduced levels, mean T1/2. Enriched target, Si, Ge(Li), NaI(Tl) detectors. Shell model calculations.
doi: 10.1103/PhysRevC.34.2049
1986WA01 Phys.Rev. C33, 303 (1986) R-Matrix Analysis of the β--, β+-Delayed Alpha Spectra from the Decay of 8Li and 8B NUCLEAR REACTIONS 4He(α, α), E ≤ 34 MeV; analyzed phase shifts. R-matrix. RADIOACTIVITY 8Li(β-); 8B(β+); analyzed β-delayed breakup α-spectra; deduced intruder states role. 8Be deduced level, Γ, Gamow-Teller matrix elements. R-matrix.
doi: 10.1103/PhysRevC.33.303
1986WA13 J.Phys.(London) G12, 523 (1986) Is the 9.13 MeV level of 14N a doublet ( Question ) NUCLEAR STRUCTURE 12C; analyzed data; deduced doublet existence evidence validity.
doi: 10.1088/0305-4616/12/6/010
1986WA19 Phys.Rev. C34, 136 (1986) E.K.Warburton, C.W.Beausang, D.B.Fossan, L.Hildingsson, W.F.Piel, Jr., J.A.Becker High-Spin (f7/2)(A-40) States in 47Ti, 47Sc, 44Ca, 45Ca, and 48Ti via 36S + 14C Fusion-Evaporation Reactions NUCLEAR REACTIONS, ICPND 36S(14C, 2n), (14C, 3n), (14C, np), (14C, 2np), (14C, nα), (14C, 2nα), E=18-38 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), DSA, σ(Eγ, E); deduced residual production σ. 47,48Ti, 47Sc, 44,45Ca deduced levels, J, π, γ-branching, B(λ), T1/2, γ-multipolarity, δ, B(λ), configuration.
doi: 10.1103/PhysRevC.34.136
1986WA22 Phys.Rev. C34, 1031 (1986) E.K.Warburton, D.E.Alburger, J.A.Becker, B.A.Brown, S.Raman Probe of the Shell Crossing at A = 40 via Beta Decay: Experiment and theory RADIOACTIVITY 35P, 37,38S, 38Cl(β-) [from 36S(d, X), (t, X), E=3-3.4 MeV]; measured Eγ, Iγ; deduced log ft. 38,37Cl, 35S, 38Ar deduced levels, γ-branching ratios, Gamow-Teller transition strengths. Shell model calculations. NUCLEAR STRUCTURE 35S, 37,38Cl, 38Ar; calculated levels, Gamow-Teller, unique first forbidden β-decay. Shell model.
doi: 10.1103/PhysRevC.34.1031
1986WA25 J.Phys.(London) G12, 1017 (1986) E.K.Warburton, J.W.Olness, C.J.Lister, J.A.Becker, S.D.Bloom Yrast Decays in 87,89Zr, 87,88,89,90Y and 86Sr from 74,76Ge(18O, xn, yp, zαγ) Reactions NUCLEAR REACTIONS 74,76Ge(18O, nα), (18O, 2nα), (18O, 3nα), (18O, 4nα), (18O, 2np), (18O, 3np), (18O, 4np), (18O, 5np), (18O, 2n), (18O, 3n), (18O, 4n), (18O, 5n), (18O, 6n), E=40-80 MeV; measured residual production σ, γγ-coin, γ(θ), σ(Eγ, E), γ yields, linear polarizations, DSA, recoil distance. 87,89Zr, 87,88,89,90Y, 86Sr deduced levels, J, π, T1/2, γ-branching, B(λ), γ-multipolarity. Ge detector. Shell model calculations.
doi: 10.1088/0305-4616/12/10/012
1986WA33 Nucl.Instrum.Methods Phys.Res. A253, 38 (1986) Precision Measurements of Gamma-Ray Energies from 13.3 a 152Eu Decay RADIOACTIVITY 152Eu(EC), (β-); measured Eγ, Iγ; deduced calibration standards. 152Sm deduced transition energies. Ge detector, mixed source technique.
doi: 10.1016/0168-9002(86)91123-X
1985DA15 Phys.Rev. C32, 713 (1985) N.J.Davis, J.A.Kuehner, A.A.Pilt, A.J.Trudel, M.C.Vetterli, C.Bamber, E.K.Warburton, J.W.Olness, S.Raman States of 38S from the 36S(t, p)38S Reaction NUCLEAR STRUCTURE 38S; calculated levels. Shell, weak coupling models. NUCLEAR REACTIONS 36S(t, p), E=18 MeV; measured σ(θ). 38S deduced levels J, π. Enriched target. DWBA analysis.
doi: 10.1103/PhysRevC.32.713
1985LI11 Phys.Rev. C32, 311 (1985) C.J.Lister, J.W.Olness, E.K.Warburton, J.A.Becker, S.D.Bloom Identification of the Yrast Decay Scheme of 86Y NUCLEAR REACTIONS 62Ni(27Al, xnypzα), E=85 MeV; measured (particle)γ-coin, Eγ, Iγ. 86Y deduced levels, J, π.
doi: 10.1103/PhysRevC.32.311
1985LI12 J.Phys.(London) G11, 969 (1985) C.J.Lister, R.Moscrop, B.J.Varley, H.G.Price, E.K.Warburton, J.W.Olness, J.A.Becker Band Structure in 81Y and Its Radioactive Decay RADIOACTIVITY 81Y(β+), (EC) [from 58Ni(28Si, pα), E=80-130 MeV; 58Ni(28Si, 2n3p), E=100-130 MeV]; measured Eγ, Iγ, γγ-coin; deduced log ft. 81Sr deduced levels, γ-branching. NUCLEAR REACTIONS, ICPND 58Ni(28Si, pα), E=80-130 MeV; 58Ni(28Si, 2n3p), E=100-130 MeV; measured σ(E), σ(θ), (particle)γ-, γγ-coin. 81Y deduced levels, possible J, π, γ-branching ratios. Ge(Li), Ge, Si detectors, enriched targets.
doi: 10.1088/0305-4616/11/8/013
1985PI05 Phys.Rev. C31, 2087 (1985) W.F.Piel, Jr., T.Chapuran, K.Dybdal, D.B.Fossan, T.Lonnroth, D.Horn, E.K.Warburton High-Spin γ-Ray Spectroscopy in Z = 83 Isotopes: 199,201Bi NUCLEAR REACTIONS 194,196Pt(10B, 5n), E=57-72 MeV; measured Eγ, Iγ, γγ-coin, Iγ(t), Iγ(θ), γγ(θ). 199,201Bi deduced levels, J, π, T1/2, δ, configurations, B(λ), yrast sequence. Enriched targets, Ge(Li), Ge detectors.
doi: 10.1103/PhysRevC.31.2087
1985SH25 Phys.Rev. C32, 1888 (1985) J.F.Shriner, Jr., P.D.Cottle, J.F.Ennis, M.Gai, D.A.Bromley, J.W.Olness, E.K.Warburton, L.Hildingsson, M.A.Quader, D.B.Fossan Level Structure of 220Ra NUCLEAR REACTIONS 208Pb(14C, 2n), E=60-78 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, σ(Eγ). 220Ra deduced levels, J, π, B(E1)/B(E2) ratios. Stable octupole deformation, α-clustering.
doi: 10.1103/PhysRevC.32.1888
1985WA09 Phys.Rev. C31, 1184 (1985) E.K.Warburton, J.W.Olness, C.J.Lister, R.W.Zurmuhle, J.A.Becker High-Spin State Spectroscopy of 88,90Zr NUCLEAR REACTIONS, ICPND 76Ge(18O, 3n), (18O, 4n), (18O, 5n), (18O, 6n), E ≈ 40-80 MeV; measured residuals relative yield. 74,76Ge(18O, xnypzα)87Sr/86Sr/85Sr/84Sr/89Y/88Y/87Y/86Y/90Zr/91Zr/92Zr/89Zr/88Zr/86Zr, E=60 MeV; measured residual relative production σ. 74,76Ge(18O, 4n), E=40-80 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), γ linear polarization, DSA, recoil. 88,90Zr deduced levels, J, π, T1/2, γ-branching, B(λ), δ. Shell model.
doi: 10.1103/PhysRevC.31.1184
1985WA10 Phys.Rev. C31, 1211 (1985) E.K.Warburton, C.J.Lister, J.W.Olness, P.E.Haustein, S.K.Saha, D.E.Alburger, J.A.Becker, R.A.Dewberry, R.A.Naumann High Spin States of 86Zr RADIOACTIVITY 86Nb(β+), (EC) [from 58Ni(32S, n3p), E=130-150 MeV]; measured γγ-, βγ-coin, γ(θ), recoil, σ(E), DSA. 86Zr deduced levels, T1/2, J, π, γ-branching, B(E2). NUCLEAR REACTIONS 60Ni(29Si, n2p), E=70-120 MeV; measured γγ-coin, γ(θ), recoil, σ(E), DSA. 58Ni(32S, n3p), E=130-150 MeV; measured γγ-, βγ-coin, σ(Eγ). 86Zr deduced levels, T1/2, J, π, γ-branching, B(E2).
doi: 10.1103/PhysRevC.31.1211
1985WA14 Phys.Rev. C31, 1896 (1985) Calculation of the 48Ca(β-)48Sc Decay Rate RADIOACTIVITY 48Ca(β-); calculated partial β-decay T1/2.
doi: 10.1103/PhysRevC.31.1896
1984AL10 Phys.Rev. C29, 2294 (1984) D.E.Alburger, E.K.Warburton, J.B.Cumming Decay of 50V RADIOACTIVITY 50V(EC), (β-); measured Eγ, Iγ; deduced T1/2, EC decay log ft, β-decay lower limit. Hyperpure Ge detector, vanadium metal sample.
doi: 10.1103/PhysRevC.29.2294
1984AL18 Phys.Rev. C30, 1005 (1984) D.E.Alburger, E.K.Warburton, B.A.Brown Decays of 50Sc, 50mSc, 50Ca, and 47K RADIOACTIVITY 50,50mSc, 50Ca, 47K(β-), 83Rb [from 48Ca(t, xnyp), E=3.2 MeV]; measured Eγ, Iγ; deduced log ft. 50Ti, 50Sc, 47Ca levels deduced Iβ, Gamow-Teller matrix elements.
doi: 10.1103/PhysRevC.30.1005
1984CO22 Phys.Rev. C30, 1768 (1984) P.D.Cottle, J.F.Shriner, Jr., F.Dellagiacoma, J.F.Ennis, M.Gai, D.A.Bromley, J.W.Olness, E.K.Warburton, L.Hildingsson, M.A.Quader, D.B.Fossan Level Structure and Deexcitations in 220Ra and Their Systematic Behavior as a Function of Neutron Number NUCLEAR REACTIONS 208Pb(14C, 2n), E=60-68 MeV; measured Eγ, Iγ, γγ-coin, σ(Eγ, E), γ(θ). 220Ra deduced levels, J, π, γ-branching, B(λ) ratios.
doi: 10.1103/PhysRevC.30.1768
1984KO31 Phys.Rev. C30, 1324 (1984) R.L.Kozub, C.B.Chitwood, D.J.Fields, C.J.Lister, E.K.Warburton Observation of Weak γ-Ray Transitions in 52Cr using an Efficient Isotope Identification Technique for Fusion-Evaporation Reactions NUCLEAR REACTIONS 7Li(51V, xnypzα), E=180 MeV; measured Iγ, Eγ, pγ-, αγ-coin. 52,53Cr, 54,55Mn deduced transitions.
doi: 10.1103/PhysRevC.30.1324
1984TH08 Phys.Rev. C30, 1442 (1984) C.E.Thorn, J.W.Olness, E.K.Warburton, S.Raman 36S(d, p)37S and 34,36S(d, 3He)33,35P Reactions NUCLEAR REACTIONS 36S(d, p), E=25 MeV; 34,36S(d, 3He), E=30 MeV; measured σ(θ), σ(Ep), σ(E(3He)). 37S deduced levels, thermal neutron capture σ, J, π, (2J+1)S. 33,35P deduced levels, L, J, π, C2S.
doi: 10.1103/PhysRevC.30.1442
1984WA07 Phys.Rev. C29, 2281 (1984) E.K.Warburton, D.E.Alburger, D.J.Millener Shapes of the 16N and 15C Beta Spectra and Extraction of Matrix Elements for 15C(β-)15N(g.s.) NUCLEAR STRUCTURE 15N; calculated partial muon capture rates. RADIOACTIVITY 16N, 15C(β-); analyzed β-spectra shapes; deduced matrix elements, β-branching ratios, meson exchange effect. Shell model.
doi: 10.1103/PhysRevC.29.2281
1983DY02 Phys.Rev. C28, 1171 (1983) K.Dybdal, T.Chapuran, D.B.Fossan, W.F.Piel, Jr., D.Horn, E.K.Warburton High-Spin States in 201,203At and the Systematic Behavior of Z = 85 Isotopes NUCLEAR REACTIONS, ICPND 192,194Pt(14N, 5n), E=58-100 MeV; measured γγ-coin, σ(Eγ, E), γ(θ), γ(t), Eγ, Iγ, γ yields. 201,203At deduced levels, J, π, T1/2, γ-branching, configurations.
doi: 10.1103/PhysRevC.28.1171
1983KO01 Phys.Rev. C27, 158 (1983) R.L.Kozub, J.Lin, J.F.Mateja, C.J.Lister, D.J.Millener, J.W.Olness, E.K.Warburton Lifetimes of Levels in 20,21F, 22Ne, and 16N NUCLEAR REACTIONS 7Li(18O, α), (18O, nα), (18O, t), E=10-60 MeV; 7Li(11B, np), E=7-35 MeV; measured Eγ, Iγ, recoil. 21F, 22Ne levels deduced T1/2. 16N, 20F levels deduced T1/2, B(λ). Shell model.
doi: 10.1103/PhysRevC.27.158
1983KO38 Phys.Rev. C28, 2343 (1983) R.L.Kozub, C.B.Chitwood, D.J.Fields, C.J.Lister, J.W.Olness, E.K.Warburton Electromagnetic Transitions in 30Al NUCLEAR REACTIONS, ICPND 14C(18O, pn), E=15-35 MeV; measured Iγ(E, θ), relative γ yield vs E, Eγ, pγ-, γγ-coin. 30Al deduced levels, limits on T1/2, γ-branching ratios, probable J.
doi: 10.1103/PhysRevC.28.2343
1983MI08 Phys.Rev. C28, 497 (1983) D.J.Millener, J.W.Olness, E.K.Warburton, S.S.Hanna Strong E1 Transitions in 9Be, 11Be, and 13C NUCLEAR STRUCTURE 9,11Be, 13C; calculated B(λ). Shell model. NUCLEAR REACTIONS 9Be(t, pγ), E=1.5-3.3 MeV; 3H(9Be, pγ), E=10-16 MeV; measured DSA. 11Be level deduced T1/2.
doi: 10.1103/PhysRevC.28.497
1982AL27 Nucl.Phys. A385, 474 (1982) Beta Decays of 25Na, 25Al and 29Al RADIOACTIVITY 25Na(β-), 29Al(β-), 25Al(β+) [from 23Na, 27Al(t, p), 24Mg(d, n)]; measured Eγ, Iγ; deduced log ft, Iβ. 25Mg, 29Si deduced γ-branching.
doi: 10.1016/0375-9474(82)90098-7
1982MI08 Phys.Rev. C26, 1167 (1982) D.J.Millener, D.E.Alburger, E.K.Warburton, D.H.Wilkinson Decay Scheme of 11Be RADIOACTIVITY 11Be [from 9Be(t, p)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 11B levels deduced β-, γ-branching, B(λ). Shell model.
doi: 10.1103/PhysRevC.26.1167
1982OL01 Nucl.Phys. A373, 13 (1982) J.W.Olness, E.K.Warburton, D.E.Alburger, C.J.Lister, D.J.Millener The Beta Decay of 18N and T = 2 States of Mass 18 RADIOACTIVITY 18N; measured Eγ, Iγ, T1/2; deduced log ft. 18O deduced levels, β-branches. He transport, Ge(Li) detectors. Shell model.
doi: 10.1016/0375-9474(82)90179-8
1982OL02 Nucl.Phys. A378, 539 (1982) J.W.Olness, E.K.Warburton, D.E.Alburger A Re-Investigation of 19O(β-)19F RADIOACTIVITY 19O [from 18O(d, p)]; measured Eγ, Iγ; deduced log ft. 19F levels deduced Iβ, γ-branching.
doi: 10.1016/0375-9474(82)90464-X
1982SJ01 Phys.Rev. C25, 889 (1982) T.P.Sjoreen, D.B.Fossan, U.Garg, A.Neskakis, A.R.Poletti, E.K.Warburton High-Spin States in 205At NUCLEAR REACTIONS 197Au(12C, 4n), E=77 MeV; measured γγ-coin, γ(θ), γ(t), Eγ, Iγ. 205At deduced levels, J, π, T1/2, B(λ), γ-multipolarity.
doi: 10.1103/PhysRevC.25.889
1982WA05 Nucl.Phys. A378, 397 (1982) E.K.Warburton, D.E.Alburger, J.W.Olness Beta Decay of 28P RADIOACTIVITY 28P; measured Eγ, Iγ; deduced log ft. 28Si deduced levels, γ-branching, Iβ.
doi: 10.1016/0375-9474(82)90456-0
1982WA16 Nucl.Phys. A385, 189 (1982) Energy of the 14N First-Excited State and the 14O 0+ → 14N 0+ ft Value RADIOACTIVITY 14O(β+) [from 12C(3He, n), E=3.2 MeV]; measured Eγ; deduced β+-endpoint energy, ft. NUCLEAR REACTIONS 12C(3He, n), E=3.2 MeV; measured Eγ; deduced β+-endpoint energy. 14N level deduced energy.
doi: 10.1016/0375-9474(82)90166-X
1982WA18 Phys.Rev. C26, 1186 (1982) E.K.Warburton, D.E.Alburger, D.H.Wilkinson Electron-Neutrino Correlation in the First-Forbidden Beta Decay of 11Be RADIOACTIVITY 11Be(β-) [from 9Be(t, p)]; measured βγ-coin, Doppler shift; deduced βν-asymmetry, meson exchange effects. Shell model.
doi: 10.1103/PhysRevC.26.1186
1982WA24 Phys.Rev. C26, 2595 (1982) Decay of 90Nb RADIOACTIVITY 90Nb(β+), (EC) [from 90Zr(p, n), E=12 MeV]; measured Eγ, Iγ, γγ-coin; deduced log ft. 90Zr deduced levels, J, π, γ-branching. Ge(Li), anti-Compton detectors, natural targets.
doi: 10.1103/PhysRevC.26.2595
1981AL13 Phys.Rev. C24, 296 (1981) Beta-Ray Branching in the Decay of 20F RADIOACTIVITY 20F [from 19F(d, p), E=2 MeV]; measured Eγ, Iγ; deduced log ft, Iβ. 20Ne deduced level.
doi: 10.1103/PhysRevC.24.296
1981KO08 Phys.Rev. C23, 1571 (1981) R.L.Kozub, J.Lin, J.F.Mateja, C.J.Lister, D.J.Millener, E.K.Warburton Electromagnetic Transitions in 14C and 14N NUCLEAR REACTIONS 7Li(9Be, pn), E=5.5 MeV; 9Be(7Li, pn), (7Li, 2n), E=3.8-7.8 MeV; measured Eγ, Iγ, recoil. 14C, 14N levels deduced T1/2. Shell model, SU(3) basis. NUCLEAR STRUCTURE 14C, 14N; calculated levels, B(λ), δ, Γγ, T1/2, γ-branching. Shell model, SU(3) basis.
doi: 10.1103/PhysRevC.23.1571
1981LE02 Phys.Rev. C23, 244 (1981) M.J.LeVine, E.K.Warburton, D.Schwalm Static Quadrupole Moments for the 2+ States of 54,56,58Fe NUCLEAR REACTIONS 56,58Fe(12C, 12C'), E=22 MeV; 56,58Fe(52Cr, 56Fe), (52Cr, 58Fe), E=110-120 MeV; 54Fe(16O, 16O'), E=28 MeV; 54Fe(40Ca, 40Ca'), E=86 MeV; measured σ(E(12C)), σ(E(16O)), target recoil, reorientation in Coulomb excitation. 54,56,58Fe levels deduced B(E2), quadrupole moment. Enriched targets, Q3D spectrometer.
doi: 10.1103/PhysRevC.23.244
1981PO07 Phys.Rev. C23, 1550 (1981) A.R.Poletti, E.K.Warburton, J.W.Olness Nuclear Structure of High-Spin States in 46Ti and 46V NUCLEAR REACTIONS 40Ca(9Be, n2p), (9Be, p2n), E=20-45 MeV; measured σ(E, Eγ), γγ-coin, Iγ(θ), DSA, recoil. 46V, 46Ti deduced levels, J, π, γ-multipolarity, transition strengths, T1/2.
doi: 10.1103/PhysRevC.23.1550
1981WA06 Phys.Rev. C23, 1234 (1981) Beta Decay of 21F RADIOACTIVITY 21F [from 19F(t, p), E=1-1.8 MeV]; measured Eγ, Iγ, T1/2; deduced log ft, β-branching ratios. 21Ne deduced levels, γ-branching ratios. Analog decay, Coulomb effects discussed.
doi: 10.1103/PhysRevC.23.1234
1981WA07 Phys.Rev. C23, 1242 (1981) E.K.Warburton, C.J.Lister, D.E.Alburger, J.W.Olness Beta Decay of 24Al RADIOACTIVITY 24Al [from 24Mg(p, n)]; measured Eγ, Iγ, γγ-coin; deduced log ft, β+-branching. 24Mg deduced levels, γ-branching ratios, B(E2), band structure, Nilsson assignments.
doi: 10.1103/PhysRevC.23.1242
1980SA32 Phys.Rev. C22, 2213 (1980) A.M.Sandorfi, C.J.Lister, D.E.Alburger, E.K.Warburton Isospin-Symmetry Violating Branch of 42Sc β+ Decay RADIOACTIVITY 42Sc [from 42Ca(p, n), E=8 MeV]; measured γγγ-coin. 42Ca levels deduced β-branching ratio. Isospin symmetry violation effects, vector coupling constant.
doi: 10.1103/PhysRevC.22.2213
1980WA24 Phys.Rev. C22, 2330 (1980) E.K.Warburton, D.E.Alburger, D.J.Millener Energies and Branching Ratios of γ transitions in 13C NUCLEAR REACTIONS 10B(α, p), E=1.66 MeV; 12C(d, p) E=2.51 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 13C level deduced T1/2. 13C deduced levels, γ-branching, B(λ). Shell model.
doi: 10.1103/PhysRevC.22.2330
1980WA25 Nucl.Instrum.Methods 178, 443 (1980) Precision Energy Measurement of γ Rays from Short-Lived Activities RADIOACTIVITY 11Be [from 9Be(t, p), E=3.1 MeV]; measured Eγ. 11B level deduced E. Short life time effects considered, precision measurement, Ge(Li) detectors.
doi: 10.1016/0029-554X(80)90823-X
1979AL17 Phys.Rev. C20, 793 (1979) ΔT = 1, 0+ → 0+ Beta Decay of 28Mg RADIOACTIVITY 28Mg [from 26Mg(t, p)]; measured βγ-coin; deduced branching ratio, log ft. 28Al deduced charge dependent matrix element between analog, anti-analog states. Magnetic spectrometer, NaI(Tl) detector.
doi: 10.1103/PhysRevC.20.793
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