NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = D.Burke Found 159 matches. Showing 1 to 100. [Next]2019RA06 Phys.Rev. C 99, 021301 (2019) J.S.Randhawa, R.Kanungo, M.Holl, J.D.Holt, P.Navratil, S.R.Stroberg, G.Hagen, G.R.Jansen, M.Alcorta, C.Andreoiu, C.Barnes, C.Burbadge, D.Burke, A.A.Chen, A.Chester, G.Christian, S.Cruz, B.Davids, J.Even, G.Hackman, J.Henderson, S.Ishimoto, P.Jassal, S.Kaur, M.Keefe, D.Kisliuk, R.Krucken, J.Liang, J.Lighthall, E.McGee, J.Measures, M.Moukaddam, E.Padilla-Rodal, A.Shotter, I.J.Thompson, J.Turko, M.Williams, O.Workman Observation of excited states in 20Mg sheds light on nuclear forces and shell evolution NUCLEAR REACTIONS 2H(20Mg, d), (20Mg, d'), E=8.5 MeV/nucleon, [secondary 20Mg beam produced in Si(p, X), E=480 MeV fragmentation reaction using SiC target at ISAC-II facility]; measured scattered deuteron spectra, differential σ(θ) using annular single-sided silicon strip detector array and CsI(Tl) detectors (IRIS reaction spectroscopy facility) at TRIUMF. 20Mg; deduced levels, J, π, proton-unbound resonances. Comparison with ab initio calculations using the valence-space in-medium similarity renormalization-group (VS-IMSRG) approach.
doi: 10.1103/PhysRevC.99.021301
2018CH08 Phys.Rev. C 97, 025802 (2018) G.Christian, G.Lotay, C.Ruiz, C.Akers, D.S.Burke, W.N.Catford, A.A.Chen, D.Connolly, B.Davids, J.Fallis, U.Hager, D.Hutcheon, A.Mahl, A.Rojas, X.Sun Direct measurement of astrophysically important resonances in 38K(p, γ) 39Ca NUCLEAR REACTIONS 1H(38K, γ)39Ca, E=15.58, 20.56, 27.17 MeV, [38K secondary beam produced at ISAC-I, TRIUMF facility by impinging 500 MeV protons on a high-power TiC production target]; measured recoils using DRAGON spectrometer, prompt Eγ, Iγ, (recoil)γ-coin using bismuth-germanate scintillator array for γ detection. Windowless hydrogen gas target; deduced energies of resonances, resonance strengths for the 386-, 515- and 689-keV proton resonances, astrophysical reaction rates for temperature range of 150-500 MK, abundances of 38Ar, 39K, and 40Ca in the hottest oxygen-neon novae.
doi: 10.1103/PhysRevC.97.025802
2016LO03 Phys.Rev.Lett. 116, 132701 (2016) G.Lotay, G.Christian, C.Ruiz, C.Akers, D.S.Burke, W.N.Catford, A.A.Chen, D.Connolly, B.Davids, J.Fallis, U.Hager, D.A.Hutcheon, A.Mahl, A.Rojas, X.Sun Direct Measurement of the Astrophysical 38K(p, γ)39Ca Reaction and Its Influence on the Production of Nuclides toward the End Point of Nova Nucleosynthesis NUCLEAR REACTIONS 1H(38K, γ), E=386, 515, 689 keV; measured reaction products, Eγ, Iγ; deduced yields, resonance parameters, astrophysical reaction rates. Comparison with available data.
doi: 10.1103/PhysRevLett.116.132701
2010PH01 Phys.Rev. C 82, 034321 (2010) A.A.Phillips, P.E.Garrett, N.Lo Iudice, A.V.Sushkov, L.Bettermann, N.Braun, D.G.Burke, G.A.Demand, T.Faestermann, P.Finlay, K.L.Green, R.Hertenberger, K.G.Leach, R.Krucken, M.A.Schumaker, C.E.Svensson, H.-F.Wirth, J.Wong Structure of the Kπ=4+ bands in 186, 188Os NUCLEAR REACTIONS 185,187Re(3He, d), E=30 MeV; measured E(d), I(d), σ, σ(θ); DWBA analysis of σ(θ) data. 186,188Os; deduced levels, J, π, L-transfers, spectroscopic factors, bands and amplitudes of two-quasiparticle components. Comparison with quasiparticle-phonon model (QPM) predictions.
doi: 10.1103/PhysRevC.82.034321
2009GA04 Phys.Rev. C 79, 017601 (2009) P.E.Garrett, A.A.Phillips, G.A.Demand, P.Finlay, K.L.Green, K.G.Leach, M.A.Schumaker, C.E.Svensson, J.Wong, R.Hertenberger, H.-F.Wirth, T.Faestermann, R.Krucken, D.G.Burke, L.Bettermann, N.Braun Scattering of 30 MeV 3He from 185Re NUCLEAR REACTIONS 185Re(3He, 3He), (3He, 3He'), E=30 MeV; measured σ(θ). Comparison with results of ECISO3 calculations.
doi: 10.1103/PhysRevC.79.017601
2008BU14 Nucl.Phys. A809, 129 (2008) D.G.Burke, P.E.Garrett, T.Qu, R.A.Naumann Nuclear structure of 229, 231Th studied with the 230, 232Th(d, t) reactions NUCLEAR REACTIONS 230,232Th(d, t), E=17 MeV; measured triton-spectra, σ(E, θ). 229,231Th deduced levels, J, π, bands. Enriched target, magnetic spectrograph. Quasi-particle configurations. DWBA analysis.
doi: 10.1016/j.nuclphysa.2008.06.009
2007BU29 Nucl.Phys. A794, 149 (2007) D.G.Burke, P.E.Garrett, P.C.Sood Nuclear level structures in 160, 162Tb studied with 161, 163Dy(t, α) reactions NUCLEAR REACTIONS 161,163Dy(3H, α), E=17 MeV; measured Eα, Iα, σ(θ), Q-value. 160,162Tb deduced levels, J, π, atomic masses. Enriched targets, magnetic spectrograph, DWBA analysis.
doi: 10.1016/j.nuclphysa.2007.08.006
2006BU19 Nucl.Phys. A778, 125 (2006) D.G.Burke, W.P.Alford, D.Elmore Nuclear structure studies of 177, 178, 179, 181Ta using (3He, d) and (α, t) reactions NUCLEAR REACTIONS 176,178,180Hf(3He, d), E=32 MeV; measured σ(E, θ). 177Hf(3He, d), E = 32 MeV; 176,177,178,180Hf(α, t), E=30 MeV; measured σ(E). 177,178,179,181Ta deduced levels, ℓ-values, spectroscopic strengths, Nilsson band assignments. 178Ta deduced proton separation energy. Enriched targets, magnetic spectrograph.
doi: 10.1016/j.nuclphysa.2006.08.010
2005BU02 Nucl.Phys. A747, 131 (2005) Single-proton-transfer studies of 153Eu levels NUCLEAR REACTIONS 154Gd(t, α), E=15 MeV; 152Sm(3He, d), E=24 MeV; 152Sm(α, t), E=25 MeV; measured particle spectra, σ(E, θ). 153Eu deduced levels, l-values, spectroscopic strengths, configurations. Nilsson model with Coriolis mixing.
doi: 10.1016/j.nuclphysa.2004.10.001
2005BU07 Nucl.Phys. A750, 185 (2005) (t, p) reaction studies of 165Dy and 179Hf NUCLEAR REACTIONS 163Dy, 177Hf(t, p), E=17 MeV; measured σ(Ep, θ). 165Dy, 179Hf deduced levels, L-values, L=0 strengths. Enriched targets, magnetic spectrograph. Systematic trends in neighboring nuclides discussed.
doi: 10.1016/j.nuclphysa.2004.12.066
2005BU21 Nucl.Phys. A756, 308 (2005) Nuclear structure studies and particle-rotor model tests for 151, 153Sm using 149, 151Sm(t, p) reactions NUCLEAR REACTIONS 149,151Sm(t, p), E=15 MeV; measured proton spectra, σ(E, θ); deduced L=0 transition strengths. 151,153Sm deduced levels, L, J, π, configurations.
doi: 10.1016/j.nuclphysa.2005.03.088
2003BU12 Nucl.Phys. A724, 274 (2003) Levels in 227Ac populated in the 230Th(p, α) reaction NUCLEAR REACTIONS 230,232Th(p, α), E=20 MeV; measured reaction products, Eα, Iα. 227Ac; deduced levels, J, π, proton hole-state admixtures, σ(E, θ). Enriched target, magnetic spectrograph, comparison with previous results.
doi: 10.1016/S0375-9474(03)01542-2
2002BU21 Phys.Rev. C66, 024312 (2002) Search for experimental evidence supporting the multiphonon description of excited states in 152Sm NUCLEAR STRUCTURE 152Sm; analyzed transitions B(E2), related data; deduced single-phonon interpretation.
doi: 10.1103/PhysRevC.66.024312
2002GU15 Nucl.Phys. A703, 45 (2002) K.Gulda, W.Kurcewicz, A.J.Aas, M.J.G.Borge, D.G.Burke, B.Fogelberg, I.S.Grant, E.Hagebo, N.Kaffrell, J.Kvasil, G.Lovhoiden, H.Mach, A.Mackova, T.Martinez, G.Nyman, B.Rubio, J.L.Tain, O.Tengblad, T.F.Thorsteinsen, and the ISOLDE Collaboration The Nuclear Structure of 229Th RADIOACTIVITY 229Ac(β-) [from 232Th(p, 4p) and 238U(p, 6p4n) and subsequent decay]; measured Eγ, Iγ, E(ce), I(ce), T1/2, βγ(t), (ce)γ-, γγ-coin. 229Th deduced levels, J, π, ICC, multipolarities, rotational bands, B(E1), B(E2), B(M1), dipole moments. Mini-orange spectrometer, advanced fast-timing techniques. Comparison with quasiparticle-phonon model predictions.
doi: 10.1016/S0375-9474(01)01456-7
2001BU17 Nucl.Phys. A688, 716 (2001) D.G.Burke, J.C.Waddington, O.P.Jolly (3He, d) and (α, t) Reaction Studies of 154Gd: Nature of Kπ = 4+ Bands in Heavy Deformed Nuclei NUCLEAR REACTIONS 153Eu(3He, d), E=24 MeV; measured σ(E, θ=30° and 60°). 153Eu(α, t), E=27 MeV; measured σ(E, θ=45° and 60°). 154Gd deduced levels, two-quasiproton admixtures. Enriched targets, magnetic spectrograph. Double-γ-phonon vs hexadecapole interpretations compared.
doi: 10.1016/S0375-9474(00)00597-2
2000GA03 Nucl.Phys. A662, 235 (2000) P.E.Garrett, H.Baltzer, M.Bertschy, D.G.Burke, M.Deleze, S.Drissi, C.Gunther, J.Jolie, J.Kern, H.Lehmann, S.J.Mannanal, J.Manns, U.Muller, J.P.Vorlet, N.Warr, T.Weber Nuclear Levels in 190Ir Studied with the 192Os(p, 3nγ) and 192Os(d, 4ne-) Reactions NUCLEAR REACTIONS 192Os(p, 3n), E=18.6, 20.8, 24.2, 27.2, 31.1 MeV; measured Eγ, Iγ(t), γγ-coin. 192Os(d, 4n), E=27.8 MeV; measured E(ce), I(ce), e-e--coin. 190Ir deduced levels J, π, T1/2. Two-quasiparticle-rotor calculations. Enriched targets, Ge detectors, orange spectrometers. NUCLEAR STRUCTURE 189Os, 190,191Ir; calculated levels, J, π. Particle-rotor calculations.
doi: 10.1016/S0375-9474(99)00365-6
2000PR03 Phys.Rev. C61, 044305 (2000) P.Prokofjevs, L.I.Simonova, M.Balodis, J.Berzins, V.Bondarenko, H.F.Wirth, T.von Egidy, C.Doll, J.Ott, W.Schauer, R.W.Hoff, R.F.Casten, R.L.Gill, J.Honzatko, I.Tomandl, S.Boneva, V.A.Khitrov, A.M.Sukhovoj, D.G.Burke, J.Kvasil, A.Mackova Nuclear Structure of 166Ho Studied in Neutron-Capture, (d, p), and (d, 3He) Reactions NUCLEAR REACTIONS 165Ho(n, γ), E ≈ 2 keV; measured Eγ, Iγ following averaged resonance capture. 165Ho(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin. 165Ho(d, p), E=17 MeV; 167Er(d, 3He), E=27 MeV; measured σ(E, θ). 166Ho deduced levels, J, π, rotational bands. Comparison with quasiparticle phonon model.
doi: 10.1103/PhysRevC.61.044305
1999BU25 Nucl.Phys. A656, 287 (1999) D.G.Burke, V.G.Soloviev, A.V.Sushkov, N.Yu.Shirikova Nuclear Structure of 172Yb NUCLEAR REACTIONS 173Yb(d, t), E=15 MeV; measured σ(E(t), θ). 171Yb(t, d), E=15 MeV; measured σ(E(d), θ). 172Yb deduced levels, J, π, spectroscopic strengths. Enriched targets, magnetic spectrograph. Comparison with quasiparticle-phonon model predictions with Coriolis mixing.
doi: 10.1016/S0375-9474(99)00318-8
1998GA40 Phys.Rev. C58, 3734 (1998) P.E.Garrett, D.G.Burke, M.Deleze, S.Drissi, J.Jolie, J.Kern, H.Lehmann, S.J.Mannanal, N.Warr States in 191Os Observed with the 192Os(p, pnγ) Reaction NUCLEAR REACTIONS 192Os(p, np), E=18.6, 20.8, 24.2, 27.2, 31.1 MeV; measured Eγ, Iγ(θ), γγ-coin. 191Os deduced levels, J, π, configurations.
doi: 10.1103/PhysRevC.58.3734
1998HE20 At.Data Nucl.Data Tables 69, 239 (1998) D.M.Headly, R.K.Sheline, P.C.Sood, R.W.Hoff, I.Hrivnacova, J.Kvasil, D.Nosek, A.K.Jain, D.G.Burke Intrinsic Structures and Associated Rotational Bands in Medium-Heavy Deformed Odd-Odd Nuclei, I COMPILATION Z=57-81; compiled rotational band levels energies, J, π for odd-odd nuclei.
doi: 10.1006/adnd.1998.0783
1998JA07 Rev.Mod.Phys. 70, 843 (1998) A.K.Jain, R.K.Sheline, D.M.Headly, P.C.Sood, D.G.Burke, I.Hrivnacova, J.Kvasil, D.Nosek, R.W.Hoff Nuclear Structure in Odd-Odd Nuclei, 144 ≤ A ≤ 194 NUCLEAR STRUCTURE A=144-194; compiled, analyzed levels, J, π, rotational bands for odd-odd nuclei.
doi: 10.1103/RevModPhys.70.843
1997BU03 Nucl.Phys. A612, 91 (1997) D.G.Burke, W.Kurcewicz, G.Lovhoiden, M.J.G.Borge, M.Cronqvist, H.Gabelmann, H.Gietz, P.Hill, N.Kaffrell, S.Mattsson, R.A.Naumann, K.Nybo, G.Nyman, J.Rogowski, G.L.Struble, T.F.Thorsteinsen, and the ISOLDE Collaboration Search for Stable Octupole Deformation in 225Fr RADIOACTIVITY 225Rn(β-) [from 232Th(p, 3n5p), mass separation]; measured Eγ, Iγ, I(ce), T1/2, γγ-, eγ-coin. 225Fr deduced levels, J, π, ICC, γ multipolarity, B(λ). Other data input. NUCLEAR REACTIONS 226Ra(t, α), E=18 MeV; measured σ(Eα). 225Fr deduced levels, Q-value, ICC, γ-multipolarity, J, π, rotational bands, B(λ). Ge, Si(Li) detectors, mini-orange spectrometer, magnetic spectrograph, other data input.
doi: 10.1016/S0375-9474(96)00311-9
1997BU10 Phys.Lett. 406B, 200 (1997) Controversy of the 43+ States in Even Osmium Isotopes NUCLEAR STRUCTURE 190,192Os; analyzed data, analyses; deduced two-phonon vibrational nature of 43+ states related features.
doi: 10.1016/S0370-2693(97)00658-8
1997KU20 Nucl.Phys. A621, 827 (1997) W.Kurcewicz, I.S.Grant, K.Gulda, A.J.Aas, J.Billowes, M.J.G.Borge, D.G.Burke, P.A.Butler, J.F.C.Cocks, B.Fogelberg, S.J.Freeman, G.D.Jones, E.Hagebo, P.Hoff, J.Honsi, A.Lindroth, G.Lovhoiden, H.Mach, T.Martinez, R.A.Naumann, K.Nybo, G.Nyman, H.Ravn, B.Rubio, J.Simpson, A.G.Smith, J.F.Smith, K.Steffensen, J.L.Tain, O.Tengblad, T.F.Thorsteinsen, and the ISOLDE Collaboration The Nuclear Structure of 227Fr RADIOACTIVITY 227Rn(β-) [from 232Th(p, n5p), E=1 GeV]; measured Eγ, Iγ, I(ce), T1/2, βγγ(t), γγ-coin. 227Fr deduced levels, J, π, ICC, γ-multipolarity, rotational bands, B(λ). Ge, Si(Li), BGO, plastic, BaF2 detectors, mini-orange spectrometer.
doi: 10.1016/S0375-9474(97)00190-5
1996GA30 Nucl.Phys. A611, 68 (1996) P.E.Garrett, N.Warr, H.Baltzer, S.Boehmsdorff, D.G.Burke, M.Deleze, S.Drissi, J.Groger, C.Gunther, J.Kern, S.J.Mannanal, J.Manns, U.Muller, J.-P.Vorlet, T.Weber Long-Lived Isomers in 190Ir NUCLEAR REACTIONS 192Os(p, 3n), E=18.6-31.1 MeV; 192Os(d, 4n), E=27.8 MeV; measured Eγ, Iγ vs Ep, (e-e-)-, (eγ)-coin. 190Ir deduced isomers T1/2, J, π, ICC, γ multipolarity. Enriched targets, Ge detector, β-ray spectrometer. RADIOACTIVITY 190mIr [from 192Os(p, 3n), E=18.6-31.1 MeV]; 192Os(d, 4n), E=27.8 MeV; measured Eγ, Iγ, I(ce), (e-e-)-, (e-γ)-coin, T1/2; deduced log ft. Enriched targets, Ge detector, β-ray spectrometer.
doi: 10.1016/S0375-9474(96)00330-2
1995BU13 Phys.Rev. C51, 3525 (1995) Nature of the Lowest Excited K(π) = 0+ States of Even-Even Deformed Nuclei
doi: 10.1103/PhysRevC.51.3525
1995GA04 Nucl.Phys. A581, 267 (1995) Study of 190Ir via Single-Proton and Single-Neutron Transfer Reactions NUCLEAR REACTIONS 191Ir(d, t), E=18 MeV; 189Os(α, t), E=30 MeV; measured σ(θ, Et). 189Os(3He, d), E=28 MeV; measured σ(θ, Ed). 190Ir deduced levels, J, π, L, spectroscopic strengths. Comparison with Nilsson-model predictions. Enriched targets, magnetic spectrograph.
doi: 10.1016/0375-9474(94)00447-U
1995SH38 Int.J.Mod.Phys. E4, 411 (1995) A.A.Shihab-Eldin, J.O.Rasmussen, M.A.Stoyer, D.G.Burke, P.E.Garrett Comparison of Two-Neutron Transfer Intensities in Rare Earth Nuclei with Predictions of Microscopic Models NUCLEAR STRUCTURE 144,146,148,150,152Nd, 154,156,158,160Gd, 146,150,152,154,156Sm, 158,160,162,164,166Dy, 166,168Er, 172,174,176,178Yb, 180,182Hf, 182,184,186W, 190,192,194Os, 196,198,200Pt; analyzed σ(t, p) data; deduced microscopic models suitability. Data on (p, t) reactions also included for some isotopes.
doi: 10.1142/S0218301395000134
1995SO02 Phys.Rev. C51, 2226 (1995) Revised Interpretations for K(π) = 1+ Bands in 166Ho NUCLEAR REACTIONS 165Ho(d, p), E=12 MeV; analyzed data. 166Ho levels deduced two-quasiparticle configurations. DWIA, Nilsson model, Coriolis mixing.
doi: 10.1103/PhysRevC.51.2226
1995SO11 Phys.Rev. C52, 88 (1995) P.C.Sood, A.Gizon, D.G.Burke, B.Singh, C.F.Liang, R.K.Sheline, M.J.Martin, R.W.Hoff β Decay of 228Ra and Possible Level Structures in 228Ac RADIOACTIVITY 228Ra(β-); measured Eβ, Iβ, I(ce), Eγ, Iγ, γγ-coin; deduced log ft; 228Ac deduced levels, J, π. Magnetic spectrometer, Si(Li) detectors and intrinsic Ge detector. Two-quasiparticle rotor model.
doi: 10.1103/PhysRevC.52.88
1994BU02 Nucl.Phys. A569, 523 (1994) D.G.Burke, O.Straume, G.Lovhoiden, T.F.Thorsteinsen, A.Graue The Nuclear Structure of 178Hf Studied by the 181Ta(p, α)178Hf Reaction NUCLEAR REACTIONS 181Ta(p, α), E=17 MeV; measured σ(Eα, θ). 178Hf deduced levels, J, π, Nilsson configurations. Natural Ta target, magnetic spectrograph.
doi: 10.1016/0375-9474(94)90317-4
1994BU16 Phys.Rev.Lett. 73, 1899 (1994) Hexadecapole-Phonon Versus Double-γ-Phonon Interpretation for K(π) = 4+ Bands in Deformed Even-Even Nuclei NUCLEAR REACTIONS 153Eu(3He, d), E=24 MeV; measured deuteron spectra. 154Gd deduced Kπ=4+ bands configuration characteristics, resolution of conflict with other data interpretation.
doi: 10.1103/PhysRevLett.73.1899
1994GA05 Nucl.Phys. A568, 445 (1994) Nuclear Structure of 192Ir Studied with Direct Transfer Reactions NUCLEAR REACTIONS 191Ir(d, p), E=16 MeV; measured σ(θ, Ep); 193Ir(d, t), E=18 MeV; measured σ(θ, Et); 193Ir(3He, α), E=25.5 MeV; measured σ(Eα); 195Pt(p, α), E=18 MeV; measured σ(Eα). 192Ir deduced levels, J, π, L, spectroscopic strengths. Comparison with interacting boson-fermion-fermion model, Nilsson predictions. Enriched targets, magnetic spectrograph.
doi: 10.1016/0375-9474(94)90390-5
1994GA30 Nucl.Phys. A579, 103 (1994) P.E.Garrett, D.G.Burke, T.Qu, V.Paar, S.Brant The Nuclear Structure of 194Ir Studied with the 193Ir(d, p)194Ir Reaction NUCLEAR REACTIONS 193Ir(d, p), E=16 MeV; measured σ(θ, Ep). 194Ir deduced levels, J, π, L, spectroscopic strengths, model assignments. Nilsson-model, interacting boson-fermion-fermion model predictions. Enriched targets, magnetic spectrograph.
doi: 10.1016/0375-9474(94)90796-X
1993BU02 Phys.Rev. C47, 131 (1993) D.G.Burke, P.C.Sood, P.E.Garrett, Q.Tao, R.K.Sheline, R.W.Hoff Nuclear Structure of 178Lu NUCLEAR REACTIONS 179Hf(t, α), E=17 MeV; measured σ(Eα), σ(θ). 178Lu deduced levels, J, π, configurations, isomer features.
doi: 10.1103/PhysRevC.47.131
1993GA13 J.Phys.(London) G19, 1021 (1993) Mixed Target Ground-State Effects in Single-Nucleon Transfer to Odd-Odd Nuclei NUCLEAR REACTIONS 189Os(3He, d), E=28 MeV; 189Os(α, t), E=30 MeV; measured σ(Ed), σ(Et). 190Ir deduced levels, J, π, Nilsson assignments.
doi: 10.1088/0954-3899/19/7/012
1993SH15 Phys.Rev. C48, 911 (1993) R.K.Sheline, D.G.Burke, M.M.Minor, P.C.Sood K(π) = 3+ Band at 1862 KeV in 178Hf NUCLEAR REACTIONS 177Hf(d, p), E=12 MeV; analyzed σ(Ep), σ(θ). 178Hf deduced revised level scheme. Other data input.
doi: 10.1103/PhysRevC.48.911
1993SH30 Pramana 41, 151 (1993) R.K.Sheline, M.M.Minor, P.C.Sood, D.G.Burke Deuteron-Induced Reaction Studies of the Nuclear Structure of 178Hf NUCLEAR REACTIONS 178Hf(d, d'), 177Hf(d, p), E=12 MeV; measured particle spectra, σ(θ). 179Hf(d, t), E not given; measured σ(θ). 178Hf deduced levels, J, π, K, band structure, configuration.
doi: 10.1007/BF02847586
1992BO05 Nucl.Phys. A539, 249 (1992) M.J.G.Borge, D.G.Burke, H.Gietz, P.Hill, N.Kaffrell, W.Kurcewicz, G.Lovhoiden, S.Mattsson, R.A.Naumann, K.Nybo, G.Nyman, T.F.Thorsteinsen, and the ISOLDE Collaboration On the Nuclear Structure of 229Ra RADIOACTIVITY 229Fr(β-); measured T1/2, Eγ, Iγ, E X-ray, I X-ray, I(ce), γγ-coin. 229Ra deduced levels, J, π, γ-multipolarity, ICC, Nilsson assignments.
doi: 10.1016/0375-9474(92)90269-P
1992BU12 Nucl.Phys. A550, 179 (1992) Single-Proton States in Neutron-Rich Lutetium Isotopes Relevant to the 180mTa Nucleosynthesis Puzzle NUCLEAR REACTIONS 178,180Hf(t, α), E=17 MeV; measured σ(Eα, θ). 177,179Lu deduced levels, J, π, Nilsson assignment. Enriched targets, magnetic spectrograph.
doi: 10.1016/0375-9474(92)91138-F
1992BU16 Nucl.Phys. A550, 21 (1992) New I(π) = 0+ States Below 2 MeV in 166Er NUCLEAR REACTIONS 164Er(t, p), E=17 MeV; measured σ(Ep, θ); 168Er(p, t), E=18 MeV; measured σ(E, θ). 166Er deduced levels, J, π. Enriched targets, magnetic spectrograph.
doi: 10.1016/0375-9474(92)91130-H
1992GA15 Nucl.Phys. A550, 1 (1992) Nuclear Structure of 159Tb, 161Tb and 163Tb Studied with the (t, α) Reaction NUCLEAR REACTIONS 160,162,164Dy(t, α), E=17 MeV; measured σ(θ), σ(Eα). 162Dy(p, α), E=17 MeV; measured σ(Eα). 159,161,163Tb deduced levels, J, π, L, Nilsson assignments. Enriched targets.
doi: 10.1016/0375-9474(92)91129-D
1992KU03 Nucl.Phys. A539, 451 (1992) W.Kurcewicz, G.Lovhoiden, T.F.Thorsteinsen, M.J.G.Borge, D.G.Burke, M.Cronqvist, H.Gabelmann, H.Gietz, P.Hill, N.Kaffrell, R.A.Naumann, K.Nybo, G.Nyman, J.Rogowski, and the ISOLDE Collaboration The Nuclear Structure of 223Fr RADIOACTIVITY 223Rn(β-) [from 232Th(p, 5n5p), mass separation]; measured Eγ, Iγ, I(ce), γγ-coin. 223Fr deduced levels, ICC, γ-multipolarity, J, π, rotational bands, dipole moment. Ge, Si(Li) detectors, mini-orange spectrometer.
doi: 10.1016/0375-9474(92)90287-T
1992TA22 Can.J.Phys. 70, 1236 (1992) Restrictions on Shape-Coexistence Descriptions of A ≈ 150 Nuclei from the 156Dy(p, t)154Dy Reaction NUCLEAR REACTIONS 156Dy(p, t), E=20 MeV; measured triton spectra, σ(θ). 154Dy deduced levels, L, shape features.
doi: 10.1139/p92-167
1990BU17 Phys.Rev. C42, R499 (1990) D.G.Burke, P.E.Garrett, Q.Tao, R.A.Naumann Additional Evidence for the Proposed Excited State at ≤ 5 eV in 229Th NUCLEAR REACTIONS 230Th(d, t), E=17 MeV; measured σ(Et), σ(θ). 229Th deduced levels, L-values, spectroscopic strengths, Nilsson assignments. Magnetic spectrograph, enriched target. DWBA analysis.
doi: 10.1103/PhysRevC.42.R499
1990BU26 Nucl.Phys. A517, 1 (1990) Single-Nucleon-Transfer Tests of the U(6/12) Supersymmetry in Plantinum Isotopes NUCLEAR REACTIONS 198Pt(polarized d, t), E=18 MeV; measured σ(Et, θ), iT1(Et, θ); 198Pt(polarized d, p), E=18 MeV; measured σ(Ep, θ), iT1(Ep, θ); 196,198Pt(t, d), E=18 MeV; measured σ(Ed, θ). 197,199Pt deduced levels, J, π, spectroscopic strengths. Comparison with U(6/12) supersymmetry predictions. Enriched targets, magnetic spectrograph. NUCLEAR STRUCTURE 193,195,197,199Pt; analyzed single nucleon transfer strengths; deduced supersymmetry model applicability.
doi: 10.1016/0375-9474(90)90258-N
1990MA68 Z.Phys. A337, 301 (1990) L.G.Mann, D.J.Decman, H.E.Martz, T.N.Massey, G.L.Struble, P.Kleinheinz, H.J.Scheerer, D.G.Burke, G.Kajrys Occupancy of Single-Proton Orbitals in 148Gd NUCLEAR REACTIONS 148Gd(3He, d), E=30 MeV; 148Gd(t, α), E=18 MeV; measured σ(θ), σ(Ed), σ(Eα); deduced model parameters. 149Tb levels deduced L, spectroscopic factors. 147Eu deduced levels, L, spectroscopic factors. 148Gd deduced ground state proton pair probability. DWBA analysis.
1989AN02 Nucl.Phys. A491, 290 (1989) E.Andersen, M.J.G.Borge, D.G.Burke, H.Gietz, P.Hill, N.Kaffrell, W.Kurcewicz, G.Lovhoiden, S.Mattsson, R.A.Naumann, K.Nybo, G.Nyman, T.F.Thorsteinsen, and the ISOLDE Collaboration Measurements of Multipolarities in 225Ra RADIOACTIVITY 225Fr(β-) [from Th, U(p, X)]; measured I(ce), γγ-, eγ-coin. 225Ra deduced levels, ICC, γ multipolarity, J, π. On-line mass separation, UC2, ThC2 targets, Ge, Si(Li) detectors, mini-orange spectrometer.
doi: 10.1016/0375-9474(89)90704-5
1989BO11 Z.Phys. A333, 109 (1989) M.J.G.Borge, D.G.Burke, H.Gabelmann, P.Hill, O.C.Jonsson, N.Kaffrell, W.Kurcewicz, G.Lovhoiden, K.Nybo, G.Nyman, H.L.Ravn, J.Rogowski, T.F.Thorsteinsen, and the ISOLDE Collaboration The New Neutron-Rich Isotope 228Rn NUCLEAR REACTIONS 232Th(p, X), E=600 MeV; measured Eγ, Iγ, K X-ray spectra; deduced evidence for 228,227Rn. RADIOACTIVITY 228,227Rn(β-) [from 232Th(p, xnyp), E=600 MeV]; measured Eγ, Iγ, K X-ray spectra; deduced T1/2.
1989BU03 Nucl.Phys. A492, 68 (1989) D.G.Burke, G.Kajrys, D.Beachey The Nuclear Structure of 158Tb NUCLEAR REACTIONS 159Tb(d, t), E=15 MeV; measured σ(E(t), θ); 159Tb(3He, α), E=28 MeV; measured σ(E(α)); 161Dy(p, α), E=17 MeV; measured σ(E(α), θ). 158Tb deduced levels, J, π, band structure, Gallagher-Moszkowski splittings. Enriched target, magnetic spectrograph.
doi: 10.1016/0375-9474(89)90509-5
1989BU09 Z.Phys. A333, 131 (1989) D.G.Burke, H.Folger, H.Gabelmann, E.Hagebo, P.Hill, P.Hoff, O.Jonsson, N.Kaffrell, W.Kurcewicz, G.Lovhoiden, K.Nybo, G.Nyman, H.Ravn, K.Riisager, J.Rogowski, K.Steffensen, T.F.Thorsteinsen, and the ISOLDE Collaboration New Neutron-Rich Isotopes of Astatine and Bismuth RADIOACTIVITY 218,219,220,221,222,223At [from 232Th(p, X), E=600 MeV]; measured βγ-coin, β-activity, K X-ray spectra; deduced T1/2. 216Bi [from 220At(α-decay)]; measured α-spectra; deduced T1/2, Qα, α-branching ratio. NUCLEAR REACTIONS 232Th(p, X), E=600 MeV; measured At isotope production rates. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0004. 1989LO07 Nucl.Phys. A494, 157 (1989) G.Lovhoiden, T.F.Thorsteinsen, E.Andersen, M.F.Kiziltan, D.G.Burke A (t, p) Study of Levels in 156Gd, 157Gd, 158Gd and 159Gd NUCLEAR REACTIONS 154,155,156,157Gd(t, p), E=17 MeV; measured σ(θ); deduced reaction mechanism. 156,157,158,159Gd deduced levels, transfer L.
doi: 10.1016/0375-9474(89)90017-1
1988BU08 Nucl.Phys. A483, 221 (1988) D.G.Burke, G.Lovhoiden, T.F.Thorsteinsen Studies of 158,160,162,164,166Dy Levels with the (t, p) Reaction NUCLEAR REACTIONS 156,158,160,162,164Dy(t, p), E=17 MeV; measured σ(E(p), θ). 158,160,162,164,166Dy deduced levels, J, π, L=0 strengths. Enriched targets.
doi: 10.1016/0375-9474(88)90533-7
1988MA18 Phys.Rev. C37, 1407 (1988) H.E.Martz, R.K.Sheline, R.G.Lanier, R.W.Hoff, G.L.Struble, D.J.Decman, D.G.Burke, R.R.Chasman, R.A.Naumann Octupole Deformation in 227Ac by Single-Proton Stripping Reactions: 226Ra(α, t)227Ac and 226Ra(3He, d)227Ac NUCLEAR REACTIONS 226Ra(α, t), (3He, d), E=30 MeV; measured σ(θ). 227Ac deduced levels, J, π. Nilsson model reflection-symmetric and Leander model reflection-asymmetric calculations. Radioactive target.
doi: 10.1103/PhysRevC.37.1407
1987BO04 Nucl.Phys. A464, 189 (1987) M.J.G.Borge, D.G.Burke, H.Gietz, P.Hill, N.Kaffrell, W.Kurcewicz, G.Lovhoiden, S.Mattsson, R.A.Naumann, K.Nybo, G.Nyman, T.F.Thorsteinsen, and the ISOLDE Collaboration Measurements of Multipolarities in 227Ra as Tests of Evidence for Stable Octupole Deformation RADIOACTIVITY 227Fr(β-) [from U(p, X)]; measured I(ce), γγ-, eγ-coin. 227Ra deduced levels, ICC, γ-multipolarity. Uranium carbide target, on-line mass separation, Ge, Si-Li detector, mini-orange spectrometer.
doi: 10.1016/0375-9474(87)90334-4
1987CI06 Phys.Rev. C36, 822 (1987) J.A.Cizewski, D.G.Burke, R.E.Brown, J.W.Sunier Ir(t(pol), α)Os Reaction and Implications for Tests of Supersymmetries NUCLEAR REACTIONS 191,193Ir(polarized t, α), E=17 MeV; measured σ(θ), analyzing powers. 190,192Os levels deduced population mechanism, possible supersymmetry model inadequancies. Enriched targets. DWBA calculations.
doi: 10.1103/PhysRevC.36.822
1986BO35 Z.Phys. A325, 429 (1986) M.J.G.Borge, D.G.Burke, F.Calaprice, O.C.Jonsson, G.Lovhoiden, R.A.Naumann, K.Nybo, G.Nyman, H.L.Ravn, T.F.Thorsteinsen, and the ISOLDE collaboration New Isotope 227Rn and Revised Halflives for 223Rn and 226Rn RADIOACTIVITY 223Rn(β-), (EC); 226Rn(β-); 227Rn(β-) [from Th(p, X), E=600 MeV]; measured Eγ, Iγ, I(ce), T1/2. 223Fr deduced γ transition energies, multipolarity. 4π plastic scintillation counter. NUCLEAR REACTIONS Th(p, X)199Rn/200Rn/201Rn/202Rn/203Rn/204Rn/205Rn/206Rn/207Rn/208Rn/209Rn/210Rn/211Rn/218Rn/219Rn/220Rn/222Rn/223Rn/224Rn/225Rn/226Rn/227Rn/228Rn, E=600 MeV; measured production yields. On-line separator. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0835. 1986LO01 Nucl.Phys. A452, 30 (1986) G.Lovhoiden, T.F.Thorsteinsen, K.Nybo, D.G.Burke Indication of an Octupole Shape Revealed in the (τ, α) Population of High-Spin States in 225Ra NUCLEAR REACTIONS 226Ra(3He, α), E=30 MeV; measured Eα, Iα, σ(θ). 225Ra deduced levels, J, π, octupole shape characteristics.
doi: 10.1016/0375-9474(86)90506-3
1986LO15 Phys.Scr. 34, 691 (1986) G.Lovhoiden, T.F.Thorsteinsen, D.G.Burke States in 160,162Gd Studied with the (t, p) Reaction NUCLEAR REACTIONS 160,158Gd(t, p), E=17 MeV; measured σ(Ep), σ(θ). 160,162Gd deduced levels, J, π, band structure, L. Enriched targets, Si detector. Coupled-channels, DWBA calculations.
doi: 10.1088/0031-8949/34/6A/025
1985BU12 Nucl.Phys. A442, 424 (1985) D.G.Burke, B.L.W.Maddaock, W.F.Davidson Two-Quasineutron States in 168Er Populated by the 167Er(d, p) and 167Er(t, d) Reactions NUCLEAR REACTIONS 167Er(d, p), E=12 MeV; measured σ(E(p), θ); 167Er(t, d), E=15 MeV; measured σ(E(d), θ). 168Er deduced levels, J, π, band structure two-quasineutron assignments. Enriched targets.
doi: 10.1016/S0375-9474(85)80025-7
1985BU18 Nucl.Phys. A445, 70 (1985) D.G.Burke, W.F.Davidson, J.A.Cizewski, R.E.Brown, J.W.Sunier Two-Quasiproton States in 168Er Studied by the 169Tm(t(pol), α)168Er Reaction NUCLEAR REACTIONS 169Tm(polarized t, α), E=17 MeV; measured σ(θ), σ(E(α), θ). 168Er deduced levels, J, π, K, two-quasiparticle Nilsson assignments.
doi: 10.1016/0375-9474(85)90361-6
1985BU19 Can.J.Phys. 63, 1309 (1985) D.G.Burke, W.F.Davidson, J.A.Cizewski, R.E.Brown, E.R.Flynn, J.W.Sunier The Nuclear Structure of 168Er Studied with the 170Er(p, t)168Er and 166Er(t, p)168Er Reactions NUCLEAR REACTIONS 170Er(p, t), E=18 MeV; 166Er(t, p), E=17 MeV; measured σ(Et), σ(Ep), σ(θ). 168Er deduced levels, J, π, configurations.
doi: 10.1139/p85-216
1985DE35 Z.Phys. A322, 37 (1985) D.J.Decman, R.K.Sheline, D.K.Burke A Proton Stripping Study of 92Nb NUCLEAR REACTIONS 91Zr(3He, d), E=25.5 MeV; measured σ(θ), σ(Ed). 92Nb deduced levels, transfer L, spectroscopic factors, configurations. DWBA analysis, shell model.
doi: 10.1007/BF01412015
1985LO19 Nucl.Phys. A437, 47 (1985) G.Lovhoiden, T.F.Thorsteinsen, L.A.Dossland, T.Kristiansen, D.G.Burke States in 163Dy and 169Er Populated in the (t, p) Reaction NUCLEAR REACTIONS 161Dy(t, p), E=15 MeV; 167Er(t, p), E=17 MeV; measured σ(Ep), σ(θ). 163Dy, 169Er deduced levels, L, J, π, configurations, Nilsson assignments.
doi: 10.1016/0375-9474(85)90226-X
1984BU05 Can.J.Phys. 62, 192 (1984) D.G.Burke, J.C.Waddington, G.Lovhoiden, T.F.Thorsteinsen A New Assignment for the (9/2)+[624] State in 181Hf from the 179Hf(t, p)181Hf Reaction NUCLEAR REACTIONS 179Hf(t, p), E=15 MeV; measured σ(Ep), σ(θ), pγ-coin. 181Hf deduced level, rotational band head level J, π, Nilsson assignment, decay characteristics.
doi: 10.1139/p84-030
1984BU14 Phys.Rev. C29, 2339 (1984) 158Tb Electron Capture Decay May Not Easily Yield a Neutrino Mass NUCLEAR REACTIONS 158Gd, 159Tb, 164Dy(d, t), E=15 MeV; 157,158Gd, 164Dy(α, t), E=27 MeV; measured σ(Et), Q-value differences. 158Tb, 158Gd deduced mass difference, unlikely K-capture branching.
doi: 10.1103/PhysRevC.29.2339
1984BU30 Phys.Lett. 146B, 392 (1984) D.G.Burke, Y.S.Liang, J.C.Waddington A Revised Level Scheme for 158Tb NUCLEAR REACTIONS 154Sm(7Li, 3n), E=27 MeV; measured γγ-coin, Eγ, Iγ. 159Tb(d, t), E=15 MeV; 159Tb(3He, α), E=28 MeV; 161Dy(p, α), E=17 MeV; measured σ(θ), σ(Et), σ(Eα). 158Tb deduced levels, J, π, configurations, isomer decay transition strength, γ-multipolarity, ICC.
doi: 10.1016/0370-2693(84)90146-1
1983BU03 Can.J.Phys. 61, 460 (1983) D.G.Burke, I.Nowikow, Y.K.Peng, J.C.Yanch Systematics of the (t, p) Reaction in Yb and Hf Isotopes near the N = 108 ' Subshell Closure ' NUCLEAR REACTIONS 170,174,176Yb, 178,180Hf(t, p), E=15 MeV; measured σ(Ep), σ(θ). 172Yb levels deduced L=0 transition relative strength. 176Yb, 180Hf deduced levels, L=0 transition strength. 178Yb, 182Hf deduced levels, L=0 transition relative strength, two-neutron separation energies.
doi: 10.1139/p83-058
1983CI01 Phys.Rev. C27, 1040 (1983) J.A.Cizewski, D.G.Burke, E.R.Flynn, R.E.Brown, J.W.Sunier Single Proton Structure of 193,195,197Ir and Perturbed Spin(6) Symmetry NUCLEAR STRUCTURE 194,196,198Pt, 193,195,197Ir; calculated levels, proton pickup S. Interacting boson fermion model, perturbed spin(6) symmetry. NUCLEAR REACTIONS 194,196,198Pt(polarized t, α), E=17 MeV; measured σ(Eα, θ), A(Eα, θ). 193,195,197Ir deduced levels, J, π, S.
doi: 10.1103/PhysRevC.27.1040
1983DA21 Phys.Lett. 130B, 161 (1983) W.F.Davidson, W.R.Dixon, D.G.Burke, J.A.Cizewski Identification and Decay Properties of the Fourth K(π) = 0+ Band in 168Er NUCLEAR REACTIONS 167Er(n, γ), E=thermal; measured Eγ, Iγ. 167Er(n, e-), E=thermal; measured I(ce). 166Er(t, p), E=17 MeV; measured σ(Ep), σ(θ). 168Er deduced levels, J, π, K, γ-branching, δ, ICC, band structure.
doi: 10.1016/0370-2693(83)91033-X
1983NY01 Nucl.Phys. A408, 127 (1983) K.Nybo, T.F.Thorsteinsen, G.Lovhoiden, E.R.Flynn, J.A.Cizewski, R.K.Sheline, D.Decman, D.G.Burke, G.Sletten, P.Hill, N.Kaffrell, W.Kurcewicz, G.Nyman The Nuclear Structure of 225Ra NUCLEAR REACTIONS 226Ra(d, t), E=12 MeV; measured Q, σ(θ). 226Ra(polarized d, t), E=17 MeV; measured σ(Et, θ), A(Et, θ). 225Ra deduced levels, J, π. Nilsson model. RADIOACTIVITY 225Fr [from 238U(p, 6p8n), mass separation]; measured Eγ, Iγ, γγ-coin, T1/2. 225Ra deduced levels, γ-multipolarity. Magnetic spectrometers and Ge(Li) detectors. Nilsson model.
doi: 10.1016/0375-9474(83)90353-6
1983SH37 Phys.Lett. 133B, 13 (1983) R.K.Sheline, D.Decman, K.Nybo, T.F.Thorsteinsen, G.Lovhoiden, E.R.Flynn, J.A.Cizewski, D.K.Burke, G.Sletten, P.Hill, N.Kaffrell, W.Kurcewicz, G.Nyman, G.Leander Evidence for Near-Stable Octupole Deformation in 225Ra RADIOACTIVITY 225Fr(β-) [from 238U(p, X), E=600 MeV]; measured Eγ, Iγ, γγ-coin. 225Ra deduced levels J, π, K, Nilsson assignment, band decoupling parameter. NUCLEAR REACTIONS 226Ra(d, t), E=12 MeV; 226Ra(polarized d, t), E=17 MeV; measured σ(θ), analyzing power vs θ. 225Ra deduced levels, J, π, K, Nilsson assignment, band decoupling parameter.
doi: 10.1016/0370-2693(83)90094-1
1982AR13 Can.J.Phys. 60, 1534 (1982) J.Ardal, J.R.Lien, G.Lovhoiden, D.G.Burke, J.C.Waddington Levels in 145Nd Studied with the (d, t) Reaction NUCLEAR REACTIONS 146Nd(polarized d, t), E=16 MeV; measured σ(Et), σ(θ), analyzing power vs (θ). 145Nd levels deduced J, π. DWBA analysis.
1982BU23 Can.J.Phys. 60, 1751 (1982) Direct Evidence for Mixing of Two-Quasiproton and Two-Quasineutron Configurations in 172Yb NUCLEAR REACTIONS 175Lu(p, α), E=17 MeV; measured σ(Eα), σ(θ). 172Yb deduced levels, J, π, K, Nilsson configurations, band structure.
doi: 10.1139/p82-235
1982HA17 Z.Phys. A305, 143 (1982) Single-Proton States of 159Ho Studied with the (p, α) Reaction. Spectroscopic Evidence for the Unusual Coriolis Strengths in 159,161,163Ho Nuclei NUCLEAR REACTIONS 162,164Er(p, α), E=17 MeV; measured σ(Eα), σ(θ). 161Ho levels deduced normalization factors. 159Ho deduced levels, J, π, S, rotational bands, Nilsson assignments. Enriched targets. Triton cluster transfer DWBA, Coriolis mixing calculations.
1982KA07 Nucl.Instrum.Methods 193, 495 (1982) J.Kantele, E.Hammaren, D.G.Burke, J.C.Waddington A Test of the Feasibility of γp-Coincidence Techniques in Conjunction with the (t, pγ) Reaction NUCLEAR REACTIONS 150Sm(t, pγ), E=15 MeV; measured Eγ, Iγ, pγ-coin. Ge(Li), Si-Au detectors.
doi: 10.1016/0029-554X(82)90241-5
1981BU03 Nucl.Phys. A359, 36 (1981) D.G.Burke, E.Hammaren, G.Lovhoiden, J.A.Cizewski, E.R.Flynn, J.W.Sunier The Nuclear Structure of 161,163Ho Studied with the (t(pol), α) Reaction NUCLEAR REACTIONS 162,164Er(polarized t, α), E=17 MeV; measured σ(Eα, θ), A(Eα, θ). 161,163Ho deduced levels, J, π, Nilsson assignments. Enriched targets.
doi: 10.1016/0375-9474(81)90210-4
1981BU10 Nucl.Phys. A366, 202 (1981) D.G.Burke, E.Hammaren, C.L.Swift, J.A.Cizewski, E.R.Flynn, J.W.Sunier, G.Lovhoiden The 159Tb(t, α)158Gd Reaction with 17 MeV Polarized Tritons NUCLEAR REACTIONS 159Tb(polarized t, α), E=17 MeV; measured σ(Eα, θ), A(Eα, θ). 158Gd deduced levels, J, π, two-quasiparticle Nilsson assignments.
doi: 10.1016/0375-9474(81)90284-0
1981CI02 Phys.Rev.Lett. 46, 1264 (1981) J.A.Cizewski, D.G.Burke, E.R.Flynn, R.E.Brown, J.W.Sunier Dynamical Supersymmetries and Single-Particle Strengths in Iridium Nuclei NUCLEAR REACTIONS 194,196,198Pt(polarized t, α), 191,193Ir(t, p), E=17 MeV; measured σ(θ). 193,195,197Ir deduced levels, J, π, S. 195,197Ir deduced no evidence for dynamical supersymmetry. Spin(6) supersymmetry scheme.
doi: 10.1103/PhysRevLett.46.1264
1981FL05 Phys.Lett. 105B, 125 (1981) E.R.Flynn, R.E.Brown, J.W.Sunier, J.M.Gursky, J.A.Cizewski, D.G.Burke Proton-Hole Excitations in 201,203Au from 202,204Hg(t(pol), α) Reactions NUCLEAR REACTIONS 202,204Hg(polarized t, α), E=17 MeV; measured σ(θ), analyzing power vs θ. 203,201Au deduced levels, J, π, C2S, Q.
doi: 10.1016/0370-2693(81)91004-2
1981HA39 Can.J.Phys. 59, 1183 (1981) L.Haugen, J.R.Lien, G.Lovhoiden, O.Straume, D.G.Burke, J.C.Waddington Levels in 149Nd Studied with the (d(pol), t) Reaction NUCLEAR REACTIONS 150Nd(polarized d, t), E=16 MeV; measured σ(θ), σ(Et), iT11(θ). 149Nd deduced levels, L, J, π, structure factors. DWBA ananysis.
doi: 10.1139/p81-156
1981TH05 Nucl.Phys. A363, 205 (1981) T.F.Thorsteinsen, G.Lovhoiden, J.S.Vaagen, A.Bjornberg, D.G.Burke High-Spin Positive-Parity States in 179Hf Studied by the 180Hf(τ, α) Reaction at 32 MeV NUCLEAR REACTIONS 180Hf(3He, α), E=32 MeV; measured σ(θ, Eα). 179Hf deduced levels, J, π, L. Quasiparticle-rotor model, CCBA calculation, deformed Woods-Saxon orbitals, nonadiabatic Coriolis mixing effects.
doi: 10.1016/0375-9474(81)90462-0
1981VE02 Phys.Rev.Lett. 46, 584 (1981) M.Vergnes, G.Rotbard, J.Kalifa, G.Berrier-Ronsin, J.Vernotte, R.Seltz, D.G.Burke Test of Supersymmetry in the 193Ir → 194Pt Proton-Stripping Reactions NUCLEAR REACTIONS 193Ir(3He, d), E=25.5, 36 MeV; 193Ir(α, t), E=27 MeV; measured σ(Ed, θ), σ(Et, θ). 194Pt levels deduced supersymmetry model selection rule breakdown.
doi: 10.1103/PhysRevLett.46.584
1981VO03 Nucl.Phys. A365, 26 (1981) T.Von Egidy, G.Barreau, H.G.Borner, W.F.Davidson, J.Larysz, D.D.Warner, P.H.M.Van Assche, K.Nybo, T.F.Thorsteinsen, G.Lovhoiden, E.R.Flynn, J.A.Cizewski, R.K.Sheline, D.Decman, D.G.Burke, G.Sletten, N.Kaffrell, W.Kurcewicz, T.Bjornstad, G.Nyman The Rotational Structure of 227Ra NUCLEAR REACTIONS 226Ra(n, γ), E=thermal; measured Eγ, Iγ; 226Ra(d, p), E=13 MeV; measured σ(Ep, θp); 226Ra(polarized t, d), E=17 MeV; measured σ(Ed, θd), analyzing power vs θ; deduced neutron binding energy. 227Ra deduced levels, configuration. Nilsson model. RADIOACTIVITY 227Fr; measured Eγ, Iγ, γγ-coin, T1/2; deduced log ft. 227Ra deduced levels, J, π. Nilsson model.
doi: 10.1016/0375-9474(81)90386-9
1980BA69 Verh.Deut.Phys.Ges. 15, 1232 G9.3 (1980) G.Barreau, T.Bjornstad, H.G.Borner, D.G.Burke, J.A.Cizewski, W.F.Davidson, D.Decman, T.Von Egidy, E.R.Flynn, N.Kaffrell, W.Kurcewicz, J.Larysz, G.Lovhoiden, K.Nybo, B.Nyman, R.K.Sheline, G.Sletten, T.F.Thorsteinsen, P.H.M.Van Assche, D.D.Warner The rotational structure of 227Ra
1980LO10 Phys.Scr. 22, 203 (1980) G.Lovhoiden, D.G.Burke, E.R.Flynn, J.W.Sunier Single-Proton States in 185Ta Studied with the (t, α) Reaction NUCLEAR REACTIONS 186W(polarized t, α), E=17 MeV; measured σ(Eα, θ), A(Eα, θ), Q. 185Ta deduced levels, J, π, Nilsson assignment. Enriched target, DWBA.
doi: 10.1088/0031-8949/22/3/004
1980SH08 Nucl.Phys. A340, 109 (1980) M.A.M.Shahabuddin, D.G.Burke, I.Nowikow, J.C.Waddington The (t, p) Reaction Across the Shape Transitional Gd Nuclei NUCLEAR REACTIONS 152Gd(t, p), E=15 MeV; measured σ(Ep, θ). 154Gd deduced levels, J, π. Enriched target. DWBA.
doi: 10.1016/0375-9474(80)90325-5
1980SH14 Can.J.Phys. 58, 832 (1980) The 170Er(t, p)172Er Reaction at 15 MeV NUCLEAR REACTIONS 170Er(t, p), E=15 MeV; measured σ(Ep, θp); deduced Q. 172Er deduced levels, L, J, π.
doi: 10.1139/p80-114
1980ST10 Z.Phys. A295, 259 (1980) O.Straume, G.Lovhoiden, D.G.Burke Proton States in 143Pm and 145Pm Populated in the (3He, d) Reaction NUCLEAR REACTIONS 142,144Nd, Nd(3He, d), E=24 MeV; measured σ(Ed, θ); deduced Q. 143,145Pm levels deduced L, S. Enriched targets, magnetic spectrograph. Shell model, pairing theory.
doi: 10.1007/BF01412206
1980TH04 Phys.Lett. 93B, 223 (1980) T.F.Thorsteinsen, J.S.Vaagen, G.Lovhoiden, D.G.Burke, E.R.Flynn Examination of Anomalous (t, α) Angular Distributions for the 5/2- (532) Band in 153Pm. A Case Study of Multistep Population of h11/2 Dominated Bands NUCLEAR REACTIONS 154Sm(t, α), E=17 MeV; analyzed σ(θ). 153Pm levels deduced band structure. CCBA, rotational model form factors, multistep processes.
doi: 10.1016/0370-2693(80)90499-2
1979BA25 Phys.Rev. C20, 42 (1979) R.D.Bagnell, Y.Tanaka, R.K.Sheline, D.G.Burke, J.D.Sherman Two-Quasiproton States in 190Os and 192Os Studied with the (t, α) Reaction NUCLEAR REACTIONS 191,193Ir(t, α), E=15 MeV; measured σ(Eα, θ). 190,192Os deduced levels, J, π, K assignments. DWBA, strong coupling model, RPA.
doi: 10.1103/PhysRevC.20.42
1979BU03 Can.J.Phys. 57, 271 (1979) D.G.Burke, G.Lovhoiden, O.Straume, E.R.Flynn, J.W.Sunier Single-Proton States in 155Eu NUCLEAR REACTIONS 156Gd(polarized t, α), E=17 MeV; 154Sm(α, t), E=25 MeV; measured σ(Eα), σ(Et), σ(θ), A(θ). 155Eu deduced levels, J, π, S. DWBA analysis. Nilsson model with pairing, Coriolis mixing effects.
doi: 10.1139/p79-035
1979BU05 Nucl.Phys. A318, 77 (1979) D.G.Burke, G.Lovhoiden, E.R.Flynn, J.W.Sunier Single-Proton States in 157Eu and 159Eu Studied with the (t, α) Reaction NUCLEAR REACTIONS 158,160Gd(polarized t, α), E=17 MeV; measured σ(Eα, θ), Ay(Eα, θ), Q. 157,159Eu deduced levels, J, π. Nilsson assignments. Enriched targets.
doi: 10.1016/0375-9474(79)90471-8
1979LO02 Nucl.Phys. A315, 90 (1979) G.Lovhoiden, D.G.Burke, E.R.Flynn, J.W.Sunier Levels in 167,169Ho Populated in the (t, α) Reaction NUCLEAR REACTIONS 168,170Er(polarized t, α), E=17 MeV; measured σ(Eα, θ), Ay(Eα, θ). 167,169Ho deduced levels, J, π. Nilsson assignments. Enriched targets.
doi: 10.1016/0375-9474(79)90635-3
1979LO09 Nucl.Phys. A327, 64 (1979) G.Lovhoiden, P.H.Andersen, D.G.Burke, E.R.Flynn, J.W.Sunier Single-Proton States in 175Tm Studied with the (t, α) Reaction NUCLEAR REACTIONS 176Yb(polarized t, α), E=17 MeV; measured σ(Eα, θ), A(Eα, θ). 175Tm deduced levels, J, π, K. Enriched target.
doi: 10.1016/0375-9474(79)90318-X
1979PA15 Can.J.Phys. 57, 1999 (1979) The Nuclear Structure of 166Er NUCLEAR REACTIONS 167Er(d, t), E=15 MeV; 165Ho(3He, d), E=24 MeV; measured σ(θ). 167Er(3He, α), E=24 MeV; 165Ho(α, t), E=27 MeV; measured σ(Eα), σ(Et). 166Er deduced levels, J, π. Unified model, pairing effects.
doi: 10.1139/p79-273
1979ST01 Z.Phys. A290, 67 (1979) O.Straume, G.Lovhoiden, D.G.Burke Proton States in the N = 86 Nuclei 147Pm and 149Eu Populated in the (3He, d), (α, t) and (t, α) Reactions NUCLEAR REACTIONS 146Nd, 148Sm(3He, d), E=24 MeV; 146Nd, 148Sm(α, t), E=27 MeV; 148Sm(t, α), E=17 MeV; measured σ(Ed, θd), σ(Et), σ(Eα). 147Pm, 149Eu deduced levels, L, J, π, S. Compared with shell model.
doi: 10.1007/BF01408481
1979ST06 Nucl.Phys. A322, 13 (1979) O.Straume, G.Lovhoiden, D.G.Burke, E.R.Flynn, J.W.Sunier Single-Proton States in 151Pm NUCLEAR REACTIONS 152Sm(polarized t, α), E=17 MeV; measured σ(θ, Eα), Ay(θ, Eα). 150Nd(3He, d), E=24 MeV; measured σ(θ, Ed). 151Pm deduced levels, J, π, L, Nilsson assignments. Enriched targets.
doi: 10.1016/0375-9474(79)90330-0
1979ST18 Z.Phys. A293, 75 (1979) O.Straume, G.Lovhoiden, D.G.Burke, E.R.Flynn, J.W.Sunier Single-Proton States in 149Pm NUCLEAR REACTIONS 150Sm(polarized t, α), E=17 MeV; measured σ(Eα, θ). 149Pm deduced levels, S, J, π, fragmentation of g7/2, d3/2 shell model states.
doi: 10.1007/BF01414786
1978BU18 Phys.Rev. C18, 693 (1978) D.G.Burke, G.Lovhoiden, E.R.Flynn, J.W.Sunier Nuclear Structure of 153Pm Studied with the (t, α) Reaction NUCLEAR REACTIONS 154Sm(polarized t, α), E=17 MeV; measured (Eα, θ), A(Eα, θ); deduced Q. 153Pm deduced levels, J, π, Nilsson assignments. Enriched target.
doi: 10.1103/PhysRevC.18.693
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