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Search: Author = D.G.Burke

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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
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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
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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
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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
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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
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2005BU02      Nucl.Phys. A747, 131 (2005)

D.G.Burke

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
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2005BU07      Nucl.Phys. A750, 185 (2005)

D.G.Burke, G.Lovhoiden

(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
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2005BU21      Nucl.Phys. A756, 308 (2005)

D.G.Burke, I.G.Nowikow

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
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2003BU12      Nucl.Phys. A724, 274 (2003)

D.G.Burke, P.E.Garrett, T.Qu

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
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2002BU21      Phys.Rev. C66, 024312 (2002)

D.G.Burke

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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14057.


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
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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
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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
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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
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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
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1997BU10      Phys.Lett. 406B, 200 (1997)

D.G.Burke

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
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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
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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
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1995BU13      Phys.Rev. C51, 3525 (1995)

D.G.Burke, P.C.Sood

Nature of the Lowest Excited K(π) = 0+ States of Even-Even Deformed Nuclei

doi: 10.1103/PhysRevC.51.3525
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1995GA04      Nucl.Phys. A581, 267 (1995)

P.E.Garrett, D.G.Burke

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0259.


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
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1995SO02      Phys.Rev. C51, 2226 (1995)

P.C.Sood, D.G.Burke

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
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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
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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
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1994BU16      Phys.Rev.Lett. 73, 1899 (1994)

D.G.Burke

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
Citations: PlumX Metrics


1994GA05      Nucl.Phys. A568, 445 (1994)

P.E.Garrett, D.G.Burke

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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1454.


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
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1993GA13      J.Phys.(London) G19, 1021 (1993)

P.E.Garrett, D.G.Burke

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0259.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1807.


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
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1992BU12      Nucl.Phys. A550, 179 (1992)

D.G.Burke, P.E.Garrett

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
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1992BU16      Nucl.Phys. A550, 21 (1992)

D.G.Burke, P.E.Garrett

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
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1992GA15      Nucl.Phys. A550, 1 (1992)

P.E.Garrett, D.G.Burke

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
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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
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1992TA22      Can.J.Phys. 70, 1236 (1992)

Q.Tao, D.G.Burke

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
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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
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1990BU26      Nucl.Phys. A517, 1 (1990)

D.G.Burke, G.Kajrys

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1984BU14      Phys.Rev. C29, 2339 (1984)

D.G.Burke

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
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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
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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
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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
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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
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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
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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)

D.G.Burke, J.W.Blezius

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
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1982HA17      Z.Phys. A305, 143 (1982)

E.Hammaren, D.G.Burke

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1980SH14      Can.J.Phys. 58, 832 (1980)

M.A.M.Shahabuddin, D.G.Burke

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
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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
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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
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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
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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
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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
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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
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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
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1979PA15      Can.J.Phys. 57, 1999 (1979)

J.D.Panar, D.G.Burke

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
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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
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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
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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
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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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1978BU21      Phys.Lett. 78B, 48 (1978)

D.G.Burke, M.A.M.Shahabuddin, R.N.Boyd

Hexadecapole Vibrations in Osmium Isotopes

NUCLEAR REACTIONS 188,190,192Os(α, α'), E=24 MeV; measured σ(θ). 188,190,192Os deduced β(L).

doi: 10.1016/0370-2693(78)90344-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2736.


1978FL02      Phys.Rev. C17, 501 (1978)

E.R.Flynn, D.G.Burke

188,190,192Os(t, p) Reaction at 15 MeV

NUCLEAR REACTIONS 188,190,192Os(t, p), E=15 MeV; measured σ(Ep, θ). 190,192,194Os deduced levels, J, π.

doi: 10.1103/PhysRevC.17.501
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1978LO07      Nucl.Phys. A302, 51 (1978)

G.Lovhoiden, O.Straume, D.G.Burke

Levels in 189Ir and 191Ir Studied with the (p, t) Reaction

NUCLEAR REACTIONS 191,193Ir(p, t), E=18 MeV; measured σ(Et, θ); deduced Q. 189,191Ir deduced levels, J, π, L. Enriched targets.

doi: 10.1016/0375-9474(78)90286-5
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1978LO08      Nucl.Phys. A303, 1 (1978)

G.Lovhoiden, D.G.Burke, C.R.Hirning, E.R.Flynn, J.W.Sunier

Levels in 165Ho Populated in the 166Er(t, α) Reaction

NUCLEAR REACTIONS 166Er(polarized t, α), E=17 MeV; measured σ(Eα, θ), A(Eα, θ). 165Ho deduced levels, J, π, K. Enriched target.

doi: 10.1016/0375-9474(78)90038-6
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1978SH17      Nucl.Phys. A307, 239 (1978)

M.A.M.Shahabuddin, J.C.Waddington, D.G.Burke, O.Straume, G.Lovhoiden

A Comparison of the (p, α) and (t, α) Reactions in the Shape Transitional Region Near N = 90

NUCLEAR REACTIONS 150,152,154Sm(p, α), 156,158Gd(p, α), E=17.0 MeV; measured σ(Eα, θ). Results compared with sequential-, direct-transfer calculations. Enriched targets.

doi: 10.1016/0375-9474(78)90615-2
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