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NSR database version of May 24, 2024.

Search: Author = A.M.Baxter

Found 95 matches.

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2005BA51      Phys.Rev. C 71, 054302 (2005)

A.M.Baxter, A.P.Byrne, G.D.Dracoulis, P.M.Davidson, T.Kibedi, R.V.F.Janssens, M.P.Carpenter, C.N.Davids, T.L.Khoo, T.Lauritsen

Spherical and deformed structures in 189Pb

NUCLEAR REACTIONS 158Gd(36Ar, 5n), E=178 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin. 164Er(29Si, 4n), E=140 MeV; measured delayed Eγ, Iγ, γγ-coin. 189Pb deduced levels, J, π, configurations, deformation, isomer T1/2. Level systematics in neighboring isotopes discussed. Recoil mass spectrometer, pulsed beams.

doi: 10.1103/PhysRevC.71.054302
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2005DR11      Phys.Rev. C 72, 064319 (2005)

G.D.Dracoulis, G.J.Lane, T.M.Peaty, A.P.Byrne, A.M.Baxter, P.M.Davidson, A.N.Wilson, T.Kibedi, F.R.Xu

E3 strength of the 11- to 8+ isomeric decays in 194Pb and 196Pb and oblate deformation

NUCLEAR REACTIONS 170Er(29Si, 5n), E=147 MeV; 170Er(30Si, 4n), E=138 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 194,196Pb deduced levels, J, π, B(E1), B(E2), B(E3), isomer decay features. Caesar array, potential energy surface calculations.

doi: 10.1103/PhysRevC.72.064319
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2004DR04      Phys.Rev. C 69, 054318 (2004)

G.D.Dracoulis, G.J.Lane, A.P.Byrne, T.Kibedi, A.M.Baxter, A.O.Macchiavelli, P.Fallon, R.M.Clark

Spectroscopy of 18882Pb106: Evidence for shape coexistence

NUCLEAR REACTIONS 156Gd(36Ar, 4n), E=174 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 188Pb deduced levels, J, π, ICC, configurations, isomeric states, shape coexistence features. Gammasphere array.

doi: 10.1103/PhysRevC.69.054318
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2003BA07      Phys.Rev. C 67, 014320 (2003)

R.A.Bark, A.M.Baxter, A.P.Byrne, P.M.Davidson, G.D.Dracoulis, S.M.Mullins, T.R.McGoram, R.T.Newman

Two-quasiparticle configurations, signature inversion, and the πi13/2(X)νi13/2 band in 176Ir

NUCLEAR REACTIONS 149Sm(31P, 4n), E=140, 158 MeV; measured Eγ, Iγ, γγ-coin. 176Ir deduced high-spin levels, J, π, configurations, signature inversion. Comparison with neighboring nuclides and with model predictions.

doi: 10.1103/PhysRevC.67.014320
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2003DR02      Phys.Rev. C 67, 051301 (2003)

G.D.Dracoulis, G.J.Lane, A.P.Byrne, A.M.Baxter, T.Kibedi, A.O.Macchiavelli, P.Fallon, R.M.Clark

Isomer bands, E0 transitions, and mixing due to shape coexistence in 18882Pb106

NUCLEAR REACTIONS 156Gd(36Ar, 4n), E=174 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 188Pb deduced levels, J, π, δ, ICC, quadrupole moments, E2 and E0 transition strengths, band-mixing features. Gammasphere array.

doi: 10.1103/PhysRevC.67.051301
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2003EL11      Acta Phys.Pol. B34, 2301 (2003)

H.M.El-Masri, P.M.Walker, Zs.Podolyak, M.Caamano, G.D.Dracoulis, A.P.Byrne, T.Kibedi, A.M.Baxter, J.Hazel, A.M.Bruce, J.N.Orce, A.Emmanouilidis, D.M.Cullen, C.Wheldon

High-K states in 180Re

NUCLEAR REACTIONS 174Yb(11B, 5n), E=71 MeV; measured Eγ, Iγ, γγ-coin, E(ce), I(ce). 180Re deduced high-spin levels, J, π, ICC, configurations, isomer T1/2, g(K)-g(R).

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2003MO22      J.Korean Phys.Soc. 43, S100 (2003)

C.-B.Moon, G.D.Dracoulis, R.A.Bark, A.P.Byrne, P.A.Davidson, A.N.Wilson, A.M.Baxter, T.Kibedi, G.J.Lane

Collective Bands Built on the Proton h11/2 and the Neutron h11/2 Orbitals in Odd-Odd I

NUCLEAR REACTIONS 120,122Sn(7Li, 5n), E=54, 58 MeV; 118Sn(6Li, 4n), E=48 MeV; measured Eγ, Iγ, γγ-coin. 120,122,124I deduced high-spin levels, J, π, configurations. Cranked mean-field calculations, level systematics in neighboring isotopes compared.

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2002RO12      Phys.Lett. 530B, 74 (2002)

M.P.Robinson, A.E.Stuchbery, R.A.Bark, A.P.Byrne, G.D.Dracoulis, S.M.Mullins, A.M.Baxter

High-Spin g Factors and Proton Alignment in 180, 182, 184Pt

NUCLEAR REACTIONS Gd(29Si, X)180Pt/182Pt/184Pt, E=145 MeV; measured Eγ, Iγ(θ, H, t) following implantation into a cold ferromagnetic Gd host and under the presence of a variable magnetic field. 180,182,184Pt deduced average g factors for high-spin states. Transient field technique, comparison with nearby nuclei.

NUCLEAR STRUCTURE 166Hf, 184Pt; calculated high-spin rotational band g factors as a function of angular momentum; deduced effect of proton and neutron alignment. Comparison with data.

doi: 10.1016/S0370-2693(02)01265-0
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2002WH01      Nucl.Phys. A699, 415 (2002)

C.Wheldon, G.D.Dracoulis, R.T.Newman, P.M.Walker, C.J.Pearson, A.P.Byrne, A.M.Baxter, S.Bayer, T.Kibedi, T.R.McGoram, S.M.Mullins, F.R.Xu

Competing Phenomena: High-seniority excitations and γ-softness in 184Os

NUCLEAR REACTIONS 176Yb(13C, 5n), E=80 MeV; measured Eγ, Iγ, γγ-coin. 184Os deduced high-spin levels, J, π, configurations, mean lifetimes, g-factors. Two-band mixing, blocked BCS, potential-energy-surface calculations. Pulsed beam.

doi: 10.1016/S0375-9474(01)01274-X
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2001BA75      Nucl.Phys. A691, 577 (2001)

R.A.Bark, A.M.Baxter, A.P.Byrne, G.D.Dracoulis, T.Kibedi, T.R.McGoram, S.M.Mullins

Candidate Chiral Band in 134La

NUCLEAR REACTIONS 124Sn(15N, 5n), E=82 MeV; measured Eγ, Iγ, γγ-coin. 134La deduced high-spin levels, J, π, rotational band structure, configurations, alignments, B(M1)/B(E2) ratios, signature inversion, possible chiral band. Potential energy surface, rotor model calculations.

doi: 10.1016/S0375-9474(01)00592-9
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2001BA79      Nucl.Phys. A694, 3 (2001)

S.Bayer, A.P.Byrne, G.D.Dracoulis, A.M.Baxter, T.Kibedi, F.G.Kondev

Core-Excited States and Core-Polarization Effects in 210At and 211At

NUCLEAR REACTIONS 208Pb(7Li, 4n), (7Li, 5n), E=32-44, 53-56 MeV; measured Eγ, Iγ, γγ(t), (X-ray)γ(t). 210,211At deduced levels, J, π, T1/2, isomeric states, reduced transition probabilities. Pulsed beam.

NUCLEAR STRUCTURE 210,211At; calculated levels, configurations, B(λ). Semi-empirical shell model, yrast configurations, core excitation and polarization, residual interactions, enhanced transitions, octupole coupling.

doi: 10.1016/S0375-9474(01)00922-8
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2001DR05      Phys.Rev. C63, 061302 (2001)

G.D.Dracoulis, T.Kibedi, A.P.Byrne, A.M.Baxter, S.M.Mullins, R.A.Bark

Effect of Oblate Deformation on E3 Strengths in Light Lead and Polonium Isotopes

NUCLEAR REACTIONS 166,168Er(28Si, 4n), E=140 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin, E(ce), I(ce). 190,192Pb deduced levels, J, π, ICC, isomeric states T1/2, configurations. Comparisons with neighboring polonium isotopes.

doi: 10.1103/PhysRevC.63.061302
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2000BY02      Eur.Phys.J. A 7, 41 (2000)

A.P.Byrne, A.M.Baxter, G.D.Dracoulis, S.M.Mullins, T.Kibedi, T.R.McGoram, K.Helariutta, J.F.C.Cocks, P.Jones, R.Julin, S.Juutinen, H.Kankaanpaa, H.Kettunen, P.Kuusiniemi, M.Leino, M.Muikku, P.Nieminen, P.Rahkila, A.Savelius

Microsecond Isomers in 187Tl and 188Pb

NUCLEAR REACTIONS 155Gd(36Ar, 4n), (36Ar, 3n), (36Ar, 3np), 157Gd(36Ar, 5n), E=176 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin. 159Tb(32S, 4n), E=158 MeV; measured Eγ, Iγ, delayed γγ-coin. 187Tl deduced levels, J, π. 187Tl, 187,188Pb deduced isomers T1/2. Recoil separator.

RADIOACTIVITY 182,183,184Hg, 186,187,188Pb(α) [from 155,157Gd(36Ar, X)]; measured Eα, Iα.

doi: 10.1007/s100500050008
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2000DR11      Phys.Rev. C62, 037301 (2000)

G.D.Dracoulis, T.Kibedi, A.P.Byrne, R.A.Bark, A.M.Baxter

Conversion Coefficients and Band Assignments in 180Ta

NUCLEAR REACTIONS 176Yb(7Li, 3n), E=28 MeV; measured Eγ, Iγ(t), E(ce), I(ce). 180Ta deduced high-spin levels, J, π, ICC, configurations. Pulsed beam, superconducting solenoid electron detector.

doi: 10.1103/PhysRevC.62.037301
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2000MC03      Phys.Rev. C62, 031303 (2000)

T.R.McGoram, G.D.Dracoulis, T.Kibedi, A.P.Byrne, R.A.Bark, A.M.Baxter, S.M.Mullins

Normal and Anomalous K-Hindered Decays from Four-Quasiparticle Isomers in 176Lu

NUCLEAR REACTIONS 176Yb(7Li, 3nα), E=45 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin, E(ce), I(ce). 176Lu deduced levels, J, π, configurations, isomers T1/2, hindrance factors.

doi: 10.1103/PhysRevC.62.031303
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1999BA30      Nucl.Phys. A650, 3 (1999)

S.Bayer, A.P.Byrne, G.D.Dracoulis, A.M.Baxter, T.Kibedi, F.G.Kondev, S.M.Mullins, T.R.McGoram

High-Spin States, Yrast Isomers and Residual Interactions in the Odd-Odd Nucleus 212At

NUCLEAR REACTIONS 208Pb(7Li, 3n), E=32-44 MeV; measured Eγ, Iγ, γγ(t), (X-ray)γ(t), E(ce), I(ce)(t). 212At deduced levels, J, π, T1/2, B(λ). Enriched targets, pulsed beam, Compton supressed Ge detectors, superconducting solenoidal spectrometer, Si(Li) detector.

NUCLEAR STRUCTURE 212At; calculated B(λ), yrast configurations, core excitation, residual interactions, blocking, enhanced transitions, octupole coupling. Semi-empirical shell model.

doi: 10.1016/S0375-9474(99)00103-7
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1999DA18      Nucl.Phys. A657, 219 (1999)

P.M.Davidson, G.D.Dracoulis, T.Kibedi, A.P.Byrne, S.S.Anderssen, A.M.Baxter, B.Fabricius, G.J.Lane, A.E.Stuchbery

Non-Yrast States and Shape Co-Existence in Light Pt Isotopes

RADIOACTIVITY 176,178,180,182Au(β+), (EC) [from 144Sm(35Cl, xn)]; measured Eγ, Iγ, γγ(t), γγ(θ), E(ce), (ce)γ-coin. 178,180,182Pt deduced levels, J, π, ICC, γ-ray branching ratios.

NUCLEAR STRUCTURE 178,180,182Pt; calculated levels, J, π, branching ratios, transition quadrupole moments. Band mixing model.

doi: 10.1016/S0375-9474(99)00340-1
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1999DR10      Phys.Rev. C60, 014303 (1999)

G.D.Dracoulis, A.P.Byrne, A.M.Baxter, P.M.Davidson, T.Kibedi, T.R.McGoram, R.A.Bark, S.M.Mullins

Spherical and Deformed Isomers in 188Pb

NUCLEAR REACTIONS 164Er(28Si, 4n), E not given; measured delayed Eγ, Iγ, γγ-coin. 188Pb deduced levels, J, π, isomeric states T1/2, deformation. Recoil-shadow technique.

doi: 10.1103/PhysRevC.60.014303
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1998BA88      Phys.Rev. C58, 2671 (1998)

A.M.Baxter, A.P.Byrne, G.D.Dracoulis, P.M.Davidson, T.R.McGoram, P.H.Regan, C.Chandler, W.Gelletly, C.Wheldon, R.Julin, J.F.C.Cocks, K.Helariutta, P.Jones, S.Juutinen, H.Kankaanpaa, H.Kettunen, P.Kuusiniemi, M.Leino, M.Muikku, A.Savelius, R.V.F.Janssens, T.Brown, M.P.Carpenter, C.N.Davids, T.Lauritsen, D.Nisius, P.T.Greenlees

Identification of Yrast States in 187Pb

NUCLEAR REACTIONS 155Gd(36Ar, 4n), E=174, 176 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin. 187Pb deduced levels, possible J, π. Level scheme systematics in Pb isotopes discussed. Recoil separators.

RADIOACTIVITY 186,187,188Pb(α) [from 155Gd(36Ar, xn)]; measured Eα, Iα.

doi: 10.1103/PhysRevC.58.2671
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1998DR06      Phys.Lett. 432B, 37 (1998)

G.D.Dracoulis, A.P.Byrne, A.M.Baxter

Interference between Spherical and Deformed States in 190Pb

NUCLEAR REACTIONS 166Er(28Si, 4n), E=140 MeV; measured Eγ, Iγ(t), γγ-coin. 190Pb deduced high-spin levels, J, π, isomeric states, configurations, shape coexisitence. Systematics of light lead isotopes discussed.

doi: 10.1016/S0370-2693(98)00620-0
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1998ST24      Nucl.Phys. A641, 401 (1998)

A.E.Stuchbery, G.D.Dracoulis, T.Kibedi, A.P.Byrne, B.Fabricius, A.R.Poletti, G.J.Lane, A.M.Baxter

Spectroscopy of 215Ra: The shell model and enhanced E3 transitions

NUCLEAR REACTIONS 206Pb(13C, 4n), E=66-84 MeV; measured Eγ, Iγ(θ), Iγ(θ, H, t), γγ(t), (X-ray)γ(t), I(ce)(t). 215Ra deduced levels J, π, g, T1/2, reduced transition probabilities, ICC. Enriched targets, pulsed beam, Ge hyper-pure, planar Ge, Compton-supressed detectors, superconducting solenoidal electron spectrometer, Si(Li) detector.

NUCLEAR STRUCTURE 215Ra; calculated levels, B(λ), g. Semi-empirical shell model, octupole coupling.

doi: 10.1016/S0375-9474(98)00484-9
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1995LA08      Nucl.Phys. A586, 316 (1995)

G.J.Lane, G.D.Dracoulis, A.P.Byrne, P.M.Walker, A.M.Baxter, J.A.Sheikh, W.Nazarewicz

Shape Coexistence in 185Tl and 187Tl - Investigation of the Deformed Minima

NUCLEAR REACTIONS 154Gd(35Cl, 4n), E=166 MeV; 159Tb(32S, 4n), E=154 MeV; measured Eγ, Iγ, γγ(t), γγ(θ). 154Gd(36Ar, 4np), E=184 MeV; 155Gd(36Ar, 3np), E=174 MeV; measured Eγ, Iγ. 185,187Tl deduced high-spin levels, J, π, T1/2, ICC, rotational bands, configurations, alignments, g(K)-g(R), shape features, occupation probabilities, blocking, Nilsson parameters. Model comparison.

doi: 10.1016/0375-9474(94)00515-O
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1995LA10      Nucl.Phys. A589, 129 (1995)

G.J.Lane, G.D.Dracoulis, A.P.Byrne, S.S.Anderssen, P.M.Davidson, B.Fabricius, T.Kibedi, A.E.Stuchbery, A.M.Baxter

High-Spin States in 183Hg and Shape Coexistence in the Odd-Mass Mercury Isotopes

NUCLEAR REACTIONS 155Gd(32S, 4n), E=159 MeV; measured Eγ, Iγ, γγ(t), γγ(θ). 183Hg deduced high-spin levels, J, π, rotational bands, configurations, alignments, g(K)-g(R), B(E2) ratios. 185,187Hg levels deduced B(E2) ratios, band-mixing, shape features, prolate-oblate energy differences.

doi: 10.1016/0375-9474(95)00080-K
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1994BY01      Nucl.Phys. A567, 445 (1994)

A.P.Byrne, G.J.Lane, G.D.Dracoulis, B.Fabricius, T.Kibedi, A.E.Stuchbery, A.M.Baxter, K.J.Schiffer

Octupole Coupling and Proton-Neutron Interactions in 214Fr

NUCLEAR REACTIONS 205Tl(13C, 4n), E=75-84 MeV; 208Pb(11B, 5n), E=68-84 MeV; measured γγ(t), (X-ray)γ(t), Eγ, Iγ(θ), I(ce)(t), Iγ(θ, H, t). 214Fr deduced levels J, π, T1/2, g, reduced B(λ), ICC. Enriched targets, pulsed-beam, Ge hyperpure, planar Ge, Compton suppressed detectors, superconducting solenoidal electron spectrometer, Si(Li) detector.

NUCLEAR STRUCTURE 214Fr; calculated levels, B(λ), g. Semi-empirical shell model, yrast configurations, core-excitation, octupole coupling.

doi: 10.1016/0375-9474(94)90158-9
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1994DA02      Nucl.Phys. A568, 90 (1994)

P.M.Davidson, G.D.Dracoulis, T.Kibedi, A.P.Byrne, S.S.Anderssen, A.M.Baxter, B.Fabricius, G.J.Lane, A.E.Stuchbery

Non-Yrast States and Shape Co-Existence in 172Os

RADIOACTIVITY 172Ir(α), (EC) [from 144Sm(31P, 3n), E=150 MeV]; measured Eγ, Iγ, γγ(t), γγ(θ), I(ce), (ce)γ-coin. 172Os deduced levels, J, π, ICC, B(λ), branching ratios, configurations, band structure.

doi: 10.1016/0375-9474(94)90005-1
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1994LA04      Phys.Lett. 324B, 14 (1994)

G.J.Lane, G.D.Dracoulis, A.P.Byrne, P.M.Walker, A.M.Baxter, R.G.Henry, D.Nisius, C.N.Davids, T.Lauritsen, H.Penttila, D.J.Henderson, J.A.Sheikh, W.Nazarewicz

Deformed i13/2 Bands and Prolate-Oblate Shape Coexistence in 185Tl and 187Tl

NUCLEAR REACTIONS 154Gd(35Cl, 4n), E=166 MeV; 159Tb(32S, 4n), E=154 MeV; measured γγ(t), γ(θ), DCO ratios. 154Gd(36Ar, 3np), E=174 MeV; 154Gd(36Ar, 4np), E=184 MeV; measured mass gated γ-spectra. 185,187Tl deduced levels, J, π, band structure, isomer T1/2.

doi: 10.1016/0370-2693(94)00073-5
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1993BA52      Phys.Rev. C48, R2140 (1993)

A.M.Baxter, A.P.Byrne, G.D.Dracoulis, R.V.F.Janssens, I.G.Bearden, R.G.Henry, D.Nisius, C.N.Davids, T.L.Khoo, T.Lauritsen, H.Penttila, D.J.Henderson, M.P.Carpenter

Spectroscopy of 186Pb with Mass Identification

NUCLEAR REACTIONS 154Gd(36Ar, 4n), E=174 MeV; measured Eγ, Iγ, (evaporation residue)γγ-coin, evaporation residue mass. 186Pb deduced levels, band features. Fragment mass analyser, Compton suppressed Ge detectors, enriched target.

doi: 10.1103/PhysRevC.48.R2140
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1993BY01      Nucl.Phys. A553, 519c (1993)

A.P.Byrne, G.D.Dracoulis, G.J.Lane, B.Fabricius, T.Kibedi, A.E.Stuchbery, A.M.Baxter, K.Schiffer

Proton-Neutron Interactions in Odd-Odd Nucleus 214Fr

NUCLEAR REACTIONS 205Tl(13C, 4n), 208Pb(11B, 5n), E not given; measured γγ-coin, γγ(t), γ(θ), σ(Eγ, E). 214Fr deduced levels, J, π, band structure.

doi: 10.1016/0375-9474(93)90651-D
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1993DA10      Nucl.Phys. A560, 822 (1993)

P.M.Davidson, G.D.Dracoulis, A.P.Byrne, T.Kibedi, B.Fabricius, A.M.Baxter, A.E.Stuchbery, A.R.Poletti, K.J.Schiffer

Spectroscopy of 211Rn Approaching the Valence Limit

NUCLEAR REACTIONS 198Pt(18O, 5n), E=96 MeV; measured γγ(t), Eγ, Iγ(E, t), I(ce). 211Rn deduced levels J, π, T1/2, ICC. Enriched target, pulse beam, Ge hyperpure, Compton-suppressed detectors, Si(Li), superconducting electron spectrometer.

NUCLEAR STRUCTURE 211Rn; calculated levels, B(λ). Multi-particle octupole-coupling model, shell model.

doi: 10.1016/0375-9474(93)90173-U
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1992BA60      Nucl.Instrum.Methods Phys.Res. A317, 101 (1992)

A.M.Baxter, T.L.Khoo, M.E.Bleich, M.P.Carpenter, I.Ahmad, R.V.F.Janssens, E.F.Moore, I.G.Bearden, J.R.Beene, I.Y.Lee

Compton-Suppression Tests on Ge and BGO Prototype Detectors for GAMMASPHERE

RADIOACTIVITY 241Am(α); 60Co(β-); 137Cs(β-); 88Y(EC), (β+); measured Eγ, Iγ; deduced peak-to-total ratio for 60Co source. Compton suppression tests, GAMMASPHERE, Ge, BGO prototype detectors.

doi: 10.1016/0168-9002(92)90597-W
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1992BE18      Z.Phys. A341, 491 (1992)

I.G.Bearden, R.V.F.Janssens, M.P.Carpenter, E.F.Moore, I.Ahmad, A.M.Baxter, Ph.Benet, P.J.Daly, M.W.Drigert, P.B.Fernandez, U.Garg, Z.W.Grabowski, T.L.Khoo, T.Lauritsen, W.Reviol, D.Ye

Characterization of the Superdeformed Band in 189Hg

NUCLEAR REACTIONS 160Gd(34S, 5n), E=165 MeV; measured γγ-coin. 189Hg deduced superdeformed band, levels, J, π.

doi: 10.1007/BF01301395
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1992ST09      Nucl.Phys. A548, 159 (1992)

A.E.Stuchbery, G.D.Dracoulis, T.Kibedi, A.P.Byrne, B.Fabricius, A.R.Poletti, G.J.Lane, A.M.Baxter

Spectroscopy and Shell Model Interpretation of High-Spin States in the N = 126 Nucleus 214Ra

NUCLEAR REACTIONS 206Pb(12C, 4n), E=66-84 MeV; 206Pb(13C, 5n), E=66-84 MeV; measured γγ(t), (X-ray)γ(t), Eγ, Iγ(θ), I(ce)(t), Iγ(E, t), Iγ(θ, H, t). 214Ra deduced levels J, π, T1/2, g, B(λ), ICC. Enriched targets, pulsed-beam, Ge hyper-pure, planar Ge, Compton suppressed detectors, superconducting solenoidal electron spectrometer, Si(Li) detector.

NUCLEAR STRUCTURE 214Ra; calculated levels, B(λ), g. Semi-empirical shell model, octupole coupling.

doi: 10.1016/0375-9474(92)90081-T
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1991DR02      Phys.Lett. 257B, 21 (1991)

G.D.Dracoulis, B.Fabricius, A.P.Byrne, A.E.Stuchbery, A.M.Baxter, K.P.Lieb, K.J.Schiffer, T.Kibedi

Contrasting Behaviour of Proton h9/2 and h11/2 Bands in 175,177,179,181Ir Interpreted in an Intruder Model

NUCLEAR REACTIONS 149Sm(32S, 3np), E=163 MeV; 150Sm(31P, 4n), E not given; 147Sm(32S, 3np), E=150 MeV; 152Sm(31P, 4n), E=146 MeV; 169Tm(16O, 4n), E=91 MeV; measured γ-spectra, γγ(t), γ(X-ray)-coin. 175,177,179,181Ir deduced levels, B(λ) ratios, J, π, band structure.

doi: 10.1016/0370-2693(91)90851-G
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1991DR06      Nucl.Phys. A534, 173 (1991)

G.D.Dracoulis, B.Fabricius, T.Kibedi, A.M.Baxter, A.P.Byrne, K.P.Lieb, A.E.Stuchbery

Spectroscopy of 175Ir and 177Ir and Deformation Effects in Odd Iridium Nuclei

NUCLEAR REACTIONS 149Sm(32S, 3np), E=163 MeV; 150Sm(31P, 4n), E=148 MeV; 144Sm(35Cl, 2n2p), E=180 MeV; 147Sm(32S, 3np), E=159 MeV; measured γγ-coin, γ(θ), γγ(t). 177,175Ir deduced levels, J, π, one-quasiparticle states, configurations, rotational bands, alignments, B(M1)/B(E2) ratios. Particle-rotor cranked shell-model analyses, phenomenological three-band mixing.

doi: 10.1016/0375-9474(91)90562-K
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1991DR08      J.Phys.(London) G17, 1795 (1991)

G.D.Dracoulis, F.Riess, A.M.Baxter, A.E.Stuchbery

Lifetimes in 216Ra and 217Ra; Development of Collectivity in Trans-Lead Nuclei

RADIOACTIVITY 216,217Ra [from 208Pb(12C, X), (13C, X), E=78, 80 MeV]; measured Eγ, Iγ, γ(t).

NUCLEAR REACTIONS 208Pb(12C, xn), (13C, xn), E=78, 80 MeV; measured Eγ, Iγ, γ(t). 216,217Ra levels deduced T1/2, B(E2), collectivity features. Model comparison.

doi: 10.1088/0954-3899/17/12/003
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1991FA06      Nucl.Phys. A523, 426 (1991)

B.Fabricius, G.D.Dracoulis, T.Kibedi, A.E.Stuchbery, A.M.Baxter

Multi-Quasi-Particle States in 173Hf

NUCLEAR REACTIONS 160Gd(18O, 5n), E=88 MeV; measured γγ-coin, γγ(t), γ(θ). 173Hf deduced levels, K, J, π, T1/2, configurations, rotational bands, alignments, g-factors. Model comparison.

doi: 10.1016/0375-9474(91)90011-T
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1991MO11      Phys.Lett. 258B, 284 (1991)

E.F.Moore, R.V.F.Janssens, I.Ahmad, M.P.Carpenter, A.M.Baxter, M.E.Bleich, P.B.Fernandez, T.Lauritsen, T.L.Khoo, I.G.Bearden, Ph.Benet, P.J.Daly, U.Garg, W.Reviol, D.Ye

K X-Ray Yields Associated with the Superdeformed Band of 192Hg

NUCLEAR REACTIONS 160Gd(36S, 4n), E=159 MeV; measured γ-, X-ray spectra, γ(X-ray)-coin, X-ray yields. 192Hg; deduced no strong superdeformed band E0 decay.

doi: 10.1016/0370-2693(91)91086-B
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1990BA31      Nucl.Phys. A515, 493 (1990)

A.M.Baxter, A.P.Byrne, G.D.Dracoulis, R.A.Bark, F.Riess, A.E.Stuchbery, M.C.Kruse, A.R.Poletti

Spectroscopy of High-Spin States of 206Po

NUCLEAR REACTIONS 198Pt(13C, 5n), E=70-80 MeV; measured γγ(t), (13C)γ(t), Eγ, Iγ, Iγ(E), Iγ(θ), I(ce). 206Po deduced levels, J, π, T1/2, B(λ), ICC. Enriched targets, Ge, Si(Li) detectors, pulsed beam. Empirical shell model calculations.

doi: 10.1016/0375-9474(90)90595-D
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1990BY02      Phys.Rev. C42, R6 (1990)

A.P.Byrne, G.D.Dracoulis, K.J.Schiffer, P.M.Davidson, T.Kibedi, B.Fabricius, A.M.Baxter, A.E.Stuchbery

34 μs Isomer at High Spin in 212Fr: Evidence for a many-particle octupole coupled state

NUCLEAR REACTIONS 205Tl(12C, 5n), E=90 MeV; measured γγ-coin. 212Fr deduced levels, B(E3), T1/2. Hyperpure Ge, LEPS detectors. Multiparticle octupole vibration coupling model.

doi: 10.1103/PhysRevC.42.R6
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1990DR07      Phys.Lett. 246B, 31 (1990)

G.D.Dracoulis, P.M.Davidson, A.P.Byrne, B.Fabricius, T.Kibedi, A.M.Baxter, A.E.Stuchbery, A.R.Poletti, K.J.Schiffer

High-Spin Yrast Isomers in 211Rn and 212Rn with Enhanced E3 Decays

NUCLEAR REACTIONS 198Pt(18O, 5n), (18O, 4n), E ≈ 96 MeV; 204Hg(13C, 5n), E not given; measured γγ-coin, γγ(t), Iγ(θ). 211,212Rn deduced levels, J, π, isomers, T1/2, B(λ), ICC. Multiparticle octupole-vibration coupled model.

doi: 10.1016/0370-2693(90)91303-S
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1990DR12      Nucl.Phys. A520, 353c (1990)

G.D.Dracoulis, P.M.Davidson, A.P.Byrne, B.Fabricius, T.Kibedi, A.M.Baxter, A.E.Stuchbery, A.R.Poletti, K.J.Schiffer

High-Spin Yrast Isomers in 211Rn and 212Rn with Enhanced E3 Decays

NUCLEAR REACTIONS 198Pt(18O, 4n), (18O, 5n), E=96 MeV; 204Hg(13C, 5n), E not given; measured γγ(t), I(ce), Eγ, Iγ. 211,212Rn deduced levels, J, π, yrast isomers, T1/2, ICC, B(λ).

doi: 10.1016/0375-9474(90)91159-O
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1990FA02      Nucl.Phys. A511, 345 (1990)

B.Fabricius, G.D.Dracoulis, R.A.Bark, A.E.Stuchbery, T.Kibedi, A.M.Baxter

High-Spin States and Intrinsic Structure in 174Os and 175Os: Alignments and strong interaction

NUCLEAR REACTIONS 150Sm(29Si, xn), E=147 MeV; 150Sm(28Si, 4n), E=138 MeV; measured γγ-coin, γ(θ), γγ(t). 174,175Os deduced levels, J, π, T1/2, configurations, rotational bands, alignments, B(M1)/B(E2) ratios, g-factors. Cranked shell model analyses.

doi: 10.1016/0375-9474(90)90164-H
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1990SC21      Z.Phys. A336, 239 (1990)

K.Schiffer, A.P.Byrne, A.M.Baxter, G.D.Dracoulis, B.Fabricius, A.E.Stuchbery

High Spin States in 129Ba

NUCLEAR REACTIONS 116Cd(18O, 5n), E=82, 86 MeV; measured γγ-coin. 129Ba deduced levels, J, π, band structure.


1989BA29      J.Phys.(London) G15, L169 (1989)

R.A.Bark, G.D.Dracoulis, A.E.Stuchbery, A.P.Byrne, A.M.Baxter, F.Riess, P.K.Weng

Low-Frequency Band Crossing in 171Re: A deformed intruder interpretation

NUCLEAR REACTIONS 144Sm(30Si, 2np), E=145 MeV; 140Ce(35Cl, 4n), E=170 MeV; measured γγ-coin, γ(θ). 171Re deduced levels, J, π, Nilsson assignments, B(λ) ratios, band structure.

doi: 10.1088/0954-3899/15/8/005
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1989BA49      Nucl.Phys. A501, 157 (1989)

R.A.Bark, G.D.Dracoulis, A.E.Stuchbery, A.P.Byrne, A.M.Baxter, F.Riess, P.K.Weng

Configuration-Dependent Deformations in 171Re

NUCLEAR REACTIONS 144Sm(30Si, 2np), E=145 MeV; 140Ce(35Cl, 4n), E=170 MeV; 149Sm(28Si, 3np), E=145 MeV; measured γγ-coin, γ(θ). 171,173Re deduced levels, J, π, configurations, alignments, B(M1)/B(E2) ratios. Particle-rotor, cranked shell-model analyses, three-band mixing.

doi: 10.1016/0375-9474(89)90570-8
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1989BU07      Nucl.Phys. A494, 102 (1989)

S.M.Burnett, A.M.Baxter, G.J.Gyapong, M.P.Fewell, R.H.Spear

Electric Quadrupole Moments of the First Excited States of 130,134,138Ba

NUCLEAR REACTIONS 130,134,138Ba(α, α'), E=10.8-11.8 MeV; 130,134Ba(12C, 12C'), E=32-38 MeV; 130,134,138Ba(16O, 16O'), E=43-49 MeV; measured Coulomb excitation probabilities of first 2+ states. 130,134,138Ba levels deduced B(E2), static electric quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(89)90200-5
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1989DR02      Nucl.Phys. A493, 145 (1989)

G.D.Dracoulis, F.Riess, A.E.Stuchbery, R.A.Bark, S.L.Gupta, A.M.Baxter, M.Kruse

Properties of (15/2)- States in 215Ra and 217Th; Evaluation of the (15/2)- to (9/2)+ E3 strength in N = 127 isotones

NUCLEAR REACTIONS 208Pb(12C, 5n), E=80 MeV; 206Pb(13C, 4n), E=78 MeV; 204Pb(16O, 3n), E=84 MeV; measured Eγ, Iγ(t), I(ce)(t). 215Ra, 217Th deduced levels, ICC, T1/2, B(E3). Enriched targets, pulsed beams, Ge, Si(Li), Compton suppressed detector. Model comparison.

NUCLEAR STRUCTURE 209Pb, 211Po, 213Rn, 215Ra, 217Th; calculated levels, B(E3). Particle-octupole vibration coupling.

doi: 10.1016/0375-9474(89)90537-X
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1989SP03      Aust.J.Phys. 42, 41 (1989)

R.H.Spear, A.M.Baxter, S.M.Burnett, C.L.Miller

Measurement of Reduced Electric Octupole Transition Probabilities, B(E3;01+ → 31-), for 118,120,122Sn

NUCLEAR REACTIONS 118,120,122Sn(12C, 12C'), E=37, 38 MeV; measured projectile spectra following Coulomb excitation. 118,120,122Sn levels deduced B(λ). Shell model comparison.

doi: 10.1071/PH890041
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1988DR06      Nucl.Phys. A486, 414 (1988)

G.D.Dracoulis, R.A.Bark, A.E.Stuchbery, A.P.Byrne, A.M.Baxter, F.Riess

Band Crossing in 170Os

NUCLEAR REACTIONS 144Sm(29Si, 3n), E=142 MeV; 115In(58Ni, 2np), E=250 MeV; measured γγ-coin, γ(θ). 170Os deduced levels, J, π. Deformation systematics, cranked shell model interpretation, three band mixing in 170,172Os.

doi: 10.1016/0375-9474(88)90244-8
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1987GY01      Nucl.Phys. A470, 415 (1987)

G.J.Gyapong, R.H.Spear, M.P.Fewell, A.M.Baxter, S.M.Burnett

Experimental Determination of the Electric Quadrupole Moment of the First Excited State of 192Pt

NUCLEAR REACTIONS 192Pt(α, α'), E=14.4-15.2 MeV; 192Pt(12C, 12C'), E=41-48 MeV; 192Pt(16O, 16O'), E=55-60 MeV; measured Coulomb excitation probabilities of the first 2+ state. 192Pt levels deduced B(E2), quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(87)90011-X
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1986GY04      Nucl.Phys. A458, 165 (1986)

G.J.Gyapong, R.H.Spear, M.T.Esat, M.P.Fewell, A.M.Baxter, S.M.Burnett

Electric Quadrupole Moments of the First Excited States of 194Pt, 196Pt and 198Pt

NUCLEAR REACTIONS 194,196,198Pt(α, α'), E=14-15.6 MeV; 196Pt(α, α'), E=16.8-18.6 MeV; 194,196,198Pt(12C, 12C'), E=41-45 MeV; 194,196,198Pt(16O, 16O'), E=55-63 MeV; measured Coulomb excitation probabilities. 194,196,198Pt levels deduced B(E2), quadrupole moments. Enriched targets.

doi: 10.1016/0375-9474(86)90289-7
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1986RO15      Phys.Rev. C34, 732 (1986)

P.J.Rothschild, A.M.Baxter, S.M.Burnett, M.P.Fewell, G.J.Gyapong, R.H.Spear

Quadrupole Moment of the First Excited State of 136Ba

NUCLEAR REACTIONS 136Ba(α, α'), E=11-11.8 MeV; 136Ba(7Li, 7Li'), E=15, 16 MeV; 136Ba(16O, 16O'), E=45-49 MeV; measured Coulomb excitation probabilities. 136Ba level deduced quadrupole moment, B(E2). Enriched targets.

doi: 10.1103/PhysRevC.34.732
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1985BU01      Nucl.Phys. A432, 514 (1985)

S.M.Burnett, A.M.Baxter, S.Hinds, F.Pribac, R.H.Spear, W.J.Vermeer

A Measurement of B(E3; 0+ → 31-) and Some E2 Transition Probabilities in 132,134,136,138Ba using Coulomb Excitation

NUCLEAR REACTIONS 132,134,136,138Ba(12C, 12C'), E=38-42 MeV; measured Coulomb excitation. 132,134,136,138Ba deduced B(E2), B(E3) values. Enriched targets.

doi: 10.1016/0375-9474(85)90257-X
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1985BU13      Nucl.Phys. A442, 289 (1985)

S.M.Burnett, A.M.Baxter, S.Hinds, F.Pribac, R.Smith, R.H.Spear, M.P.Fewell

Octupole Vibrational States in the Even-Mass Barium Isotopes

NUCLEAR REACTIONS 130,132,134,136,138Ba(α, α'), E=20 MeV; measured σ(E(α')). 132,134,136,138Ba(α, α'), E=20 MeV; measured σ(Eα, θ). 132,134,136,138Ba deduced levels, J, π, L, β2, β3. 130Ba deduced levels. Enriched targets.

doi: 10.1016/0375-9474(85)90146-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0829.


1985FE03      Phys.Lett. 157B, 353 (1985)

M.P.Fewell, G.J.Gyapong, R.H.Spear, M.T.Esat, A.M.Baxter, S.M.Burnett

The Quadrupole Moment of 196Pt - A Crucial Test of Nuclear Models

NUCLEAR REACTIONS 196Pt(16O, 16O'), E=55-61 MeV; 196Pt(12C, 12C'), E=41-56 MeV; measured Coulomb excitation, particle spectra. 196Pt level deduced B(E2), quadrupole moment. Bohr-Mottelson, O(6) interacting boson model limits.

doi: 10.1016/0370-2693(85)90379-X
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1984VE03      Phys.Lett. 138B, 365 (1984)

W.J.Vermeer, M.T.Esat, M.P.Fewell, R.H.Spear, A.M.Baxter, S.M.Burnett

An Experimental Verfication of the Validity of the Reorientation-Effect Technique for the Determination of Nuclear Quadrupole Moments

NUCLEAR REACTIONS 208Pb(7Li, 7Li'), E=16-30 MeV; 138Ba(7Li, 7Li'), E=12.5-22 MeV; measured Coulomb excitation reorientation effect. 7Li level deduced B(E2), quadrupole moment.

doi: 10.1016/0370-2693(84)91918-X
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1984VE07      Aust.J.Phys. 37, 123 (1984)

W.J.Vermeer, M.T.Esat, J.A.Kuehner, R.H.Spear, A.M.Baxter, S.Hinds

Coulomb Excitation of the 2.615 MeV (3-) and 4.086 MeV (2+) States of 208Pb

NUCLEAR REACTIONS 208Pb(12C, 12C'), E=53-58 MeV; 208Pb(16O, 16O'), E=57-76 MeV; measured Coulomb excitation. 208Pb levels deduced B(λ), quadrupole moment.

doi: 10.1071/PH840123
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1984VE08      Aust.J.Phys. 37, 273 (1984)

W.J.Vermeer, A.M.Baxter, S.M.Burnett, M.T.Esat, M.P.Fewell, R.H.Spear

Coulomb Excitation of 7Li

NUCLEAR REACTIONS 208Pb, 138Ba(7Li, 7Li'), E=12.5-30 MeV; measured σ(E(7Li)), Coulomb excitation. 7Li deduced GDR excitation, B(E2), ground state static electric quadrupole moment.

doi: 10.1071/PH840273
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1983SP02      Phys.Lett. 128B, 29 (1983)

R.H.Spear, W.J.Vermeer, M.T.Esat, J.A.Kuehner, A.M.Baxter, S.Hinds

An Improved Determination of the Quadrupole Moment of the First Excited State of 208Pb

NUCLEAR REACTIONS 208Pb(12C, 12C'), E=75, 90 MeV; 208Pb(16O, 16O'), E=80-171.6 MeV; analyzed Coulomb excitation data. 208Pb level deduced static quadrupole moment, B(E3).

doi: 10.1016/0370-2693(83)90067-9
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1983VE01      Phys.Lett. 122B, 23 (1983)

W.J.Vermeer, M.T.Esat, J.A.Kuehner, R.H.Spear, A.M.Baxter, S.Hinds

Electric Quadrupole Moment of the First Excited State of 12C

NUCLEAR REACTIONS 208Pb(12C, 12C'), E=53, 54, 56, 58 MeV; 208Pb(16O, 16O'), E=72 MeV; measured σ(E(12C)), σ(E(16O)), projectile Coulomb excitation. 12C level deduced quadrupole moment.

doi: 10.1016/0370-2693(83)91160-7
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1982BA55      Nucl.Phys. A390, 29 (1982)

A.M.Baxter, A.M.Mcdonald, P.G.Ikossi, J.A.Kuehner

Spin-Parity Determinations in 42K from the 44Ca(d(pol), α)42K Reaction near 0°

NUCLEAR REACTIONS 44Ca(polarized d, α), E=7, 7.25, 7.5, 7.75, 8, 8.25 MeV; measured T20(θ=4°). 42K deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(82)90604-2
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1982KU14      Phys.Lett. 115B, 437 (1982)

J.A.Kuehner, R.H.Spear, W.J.Vermeer, M.T.Esat, A.M.Baxter, S.Hinds

A Measurement of the Giant-Dipole-Resonance Contribution to the Coulomb Excitation of 17O

NUCLEAR REACTIONS 208Pb(17O, 17O'), E=66-88 MeV; measured σ(E(17O)), projectile Coulomb excitation probability. 17O level deduced GDR contribution parameter. Modified hydrodynamic model. 208Pb(17O, 16O), (17O, 18O), E=66-88 MeV; measured σ(E(16O)), σ(E(18O)).

doi: 10.1016/0370-2693(82)90387-2
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1982SP05      Nucl.Phys. A378, 559 (1982)

R.H.Spear, T.H.Zabel, M.T.Esat, A.M.Baxter, S.Hinds

The Quadrupole Moments of 26Mg as a Test of Shell-Model Interactions

NUCLEAR REACTIONS 208Pb(26Mg, 26Mg'), E=80-120 MeV; measured Coulomb excitation. 26Mg level deduced quadrupole moment, B(E2). Enriched target.

doi: 10.1016/0375-9474(82)90466-3
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1982VE11      Aust.J.Phys. 35, 283 (1982)

W.J.Vermeer, T.H.Zabel, M.T.Esat, J.A.Kuehner, R.H.Spear, A.M.Baxter

The Giant Dipole Resonance Effect in Coulomb Excitation of 10B

NUCLEAR REACTIONS 208Pb(10B, 10B'), (10B, 9B), (10B, 11B), E=32-38 MeV; measured σ(E(10B)), σ(E(9B)), σ(E(11B)), projectile Coulomb excitation. 10B deduced virtual GDR excitation.

doi: 10.1071/PH820283
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1981BA45      Nucl.Phys. A369, 25 (1981)

A.M.Baxter, S.Hinds, R.H.Spear, T.H.Zabel, R.Smith

Octupole Vibrations in the Even Mercury and Lead Isotopes

NUCLEAR REACTIONS 198,200,202,204Hg, 204,206,208Pb(α, α'), E=24, 27 MeV; measured σ(Eα'). 198,200,202,204Hg, 204,206,208Pb deduced levels. 204Hg, 204,206,208Pb(α, α'), E=27 MeV; measured σ(Eα, θ). 204Hg, 204,206,208Pb levels deduced J, π, L, β2, β3. Enriched targets.

doi: 10.1016/0375-9474(81)90004-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0862.


1981ES03      Nucl.Phys. A362, 227 (1981)

M.T.Esat, M.P.Fewell, R.H.Spear, T.H.Zabel, A.M.Baxter, S.Hinds

The Electric Quadrupole Moment of the First Excited State of 204Hg

NUCLEAR REACTIONS 204Hg(α, α'), E=13.5-16.5 MeV; 204Hg(12C, 12C'), E=45-56 MeV; 204Hg(16O, 16O'), E=63, 65 MeV; measured Coulomb excitation. 204Hg deduced B(E2), quadrupole moment. 204Hg(p, p'), E=18 MeV; measured σ(Ep). 204Hg deduced levels. Enriched targets.

doi: 10.1016/0375-9474(81)90678-3
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1980FE07      Aust.J.Phys. 33, 505 (1980); Corrigendum Aust.J.Phys. 37, 239 (1984)

M.P.Fewell, R.H.Spear, T.H.Zabel, A.M.Baxter

Electric Quadrupole Excitation of the First Excited State of 11B

NUCLEAR REACTIONS 208Pb(11B, 11B'), E=38 MeV; measured σ(E(11B')), Coulomb excitation. 11B transition deduced B(E2). Shell model, core excitation model.

doi: 10.1071/PH800505
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1980SP05      Nucl.Phys. A345, 252 (1980)

R.H.Spear, M.T.Esat, M.P.Fewell, D.C.Kean, T.H.Zabel, A.M.Baxter, S.Hinds

Static Quadrupole Moments of the First Excited States of 200Hg and 202Hg

NUCLEAR REACTIONS 200,202Hg(α, α'), E=13.5-16.5 MeV; 200,202Hg(12C, 12C'), E=40-60 MeV; 202,200Hg(16O, 16O'), E=59-65 MeV; measured Coulomb excitation probabilities. 200,202Hg level deduced B(E2), quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(80)90423-6
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1979FE06      Nucl.Phys. A321, 457 (1979)

M.P.Fewell, A.M.Baxter, D.C.Kean, R.H.Spear, T.H.Zabel

Electric Moments of the First Excited State of 18O

NUCLEAR REACTIONS 208Pb(18O, 18O'), E=57-86 MeV; measured Coulomb excitation. 18O level deduced quadrupole moment, B(E2). Enriched target.

doi: 10.1016/0375-9474(79)90138-6
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1979FE08      Phys.Rev.Lett. 43, 1463 (1979)

M.P.Fewell, D.C.Kean, R.H.Spear, T.H.Zabel, A.M.Baxter, S.Hinds

Static Quadrupole Moment of the First Excited State of 30Si

NUCLEAR REACTIONS 208Pb(30Si, 30Si'), E=106-136 MeV; measured reorientation effect in Coulomb excitation. 30Si level deduced static quadrupole moment.

doi: 10.1103/PhysRevLett.43.1463
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1978BA43      Nucl.Phys. A305, 213 (1978)

A.M.Baxter, P.G.Ikossi, A.M.McDonald, J.A.Kuehner

Spin-Parity Combinations in 16N from the 18O(d, α)16N Reaction

NUCLEAR REACTIONS 18O(polarized d, α), E=8.50, 9.25, 10.00, 10.30, 10.75, 11.30 MeV; measured A(Eα). 16N levels deduced J, π. Enriched target.

doi: 10.1016/0375-9474(78)90174-4
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1978JO04      Phys.Lett. 72B, 307 (1978)

A.M.R.Joye, A.M.Baxter, S.Hinds, D.C.Kean, R.H.Spear

Quadrupole Moments of the First Excited States of 204,206Pb

NUCLEAR REACTIONS 204,206Pb(α, α'), E=13.8-18.5 MeV; 204,206Pb(12C, 12C'), E=44-60 MeV; 204,206Pb(16O, 16O'), E=59-85 MeV; measured Coulomb excitation. 204,206Pb deduced quadrupole moment, B(E2).

doi: 10.1016/0370-2693(78)90125-9
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1978SP08      Aust.J.Phys. 31, 377 (1978)

R.H.Spear, T.H.Zabel, A.M.Baxter, M.P.Fewell, S.Hinds, A.M.R.Joye, D.C.Kean

Determination of Maximum Safe Bombarding Energies and B(E3) Values in Reorientation Experiments with 204Pb, 206Pb and 208Pb

NUCLEAR REACTIONS 204,206Pb(α, α), (α, α'), E=13.8 MeV; 204,206Pb(12C, 12C), (12C, 12C'), E=52 MeV; 204,206,208Pb(16O, 16O), (16O, 16O'), E=60 MeV; measured σ(elastic), σ(inelastic); deduced optimum E-projectile for onset of Coulomb, nuclear interference. 204,206Pb deduced B(E3).

doi: 10.1071/PH780377
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1977BA68      Nucl.Phys. A291, 282 (1977)

A.M.Baxter, P.G.Ikossi, A.M.McDonald, J.A.Kuehner

Spin-Parity Combinations in 32P from the 34S(d, α)32P Reaction

NUCLEAR REACTIONS 34S(polarized d, α), E=8.25, 8.50, 8.75, 9.25, 9.50 MeV; measured T20(4°). 32P levels deduced J, π. Enriched target.

doi: 10.1016/0375-9474(77)90320-7
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1977ES02      Phys.Lett. 72B, 49 (1977)

M.T.Esat, D.C.Kean, R.H.Spear, M.P.Fewell, A.M.Baxter

The Static Quadrupole Moment of the First Excited State of 198Hg

NUCLEAR REACTIONS 198Hg(α, α'γ), E=14.1-18 MeV; 198Hg(12C, 12C'γ), E=43-54 MeV; 198Hg(16O, 16O'γ), E=60-80 MeV; measured Coulomb excitation reorientation effect. 198Hg level deduced quadrupole moment, B(E2).

doi: 10.1016/0370-2693(77)90060-0
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1977FE04      J.Phys.(London) G3, L27 (1977)

M.P.Fewell, D.C.Kean, R.H.Spear, A.M.Baxter

The Quadrupole Moment of the First Excited State of 18O

NUCLEAR REACTIONS 208Pb(18O, 18O'), E=57-72 MeV; measured Coulomb excitation reorientation effect. 18O level deduced quadrupole moment.

doi: 10.1088/0305-4616/3/2/003
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1977JO04      Phys.Rev.Lett. 38, 807 (1977)

A.M.R.Joye, A.M.Baxter, M.P.Fewell, D.C.Kean, R.H.Spear

Quadrupole Moment of the First 3- State in 208Pb

NUCLEAR REACTIONS 208Pb(16O, 16O'), E=59-64 MeV; 208Pb(α, α'), E=15.3 MeV; measured Coulomb excitation. 208Pb level deduced quadrupole moment, B(E3).

doi: 10.1103/PhysRevLett.38.807
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1977SP05      Aust.J.Phys. 30, 133 (1977)

R.H.Spear, J.P.Warner, A.M.Baxter, M.T.Esat, M.P.Fewell, S.Hinds, A.M.R.Joye, D.C.Kean

Vibrational Excitations in the Even-Mass Cadmium Isotopes

NUCLEAR REACTIONS 106,108,110,112,114,116Cd(α, α), (α, α'), E=17.5 MeV; measured σ(Eα'). 106,108,110,112,114,116Cd deduced levels.

doi: 10.1071/PH770133
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1976ES02      Nucl.Phys. A274, 237 (1976)

M.T.Esat, D.C.Kean, R.H.Spear, A.M.Baxter

Mass Dependence of the Static Quadrupole Moments of the First 2+ States in the Cadmium Isotopes

NUCLEAR REACTIONS 106,108,110,112,114,116Cd(α, α'), E=8-17 MeV; 106,108,110,112,114,116Cd(16O, 16O'), E=40-44 MeV; measured Coulomb excitation probabilities of first 2+ states. 106,108,110,112,114,116Cd deduced B(E2), quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(76)90239-6
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1975SP02      Phys.Rev. C11, 742 (1975)

R.H.Spear, R.A.I.Bell, M.T.Esat, P.R.Gardner, D.C.Kean, A.M.Baxter

Electromagnetic Transitions in 22Na

NUCLEAR REACTIONS 23Na(3He, αγ), E=8.46 MeV; measured αγ-coin. 19F(α, nγ), E=4.7-6.1, 11.2 MeV; measured σ(E, Eγ, θ), nγ(θ). 22Na levels deduced J, π, γ-mixing, Q0, g K-gR.

doi: 10.1103/PhysRevC.11.742
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1973BA50      Nucl.Phys. A211, 7 (1973)

A.M.Baxter, S.Hinds

A Study of the States of 30Si with the 28Si(t, p)30Si and 29Si(d, p)30Si Reactions

NUCLEAR REACTIONS 28Si(t, p), E=6.0, 10.5, 12.1 MeV; 29Si(d, p), E=10.0 MeV; measured σ(θ, Ep). 29Si(d, d), E=10.0 MeV; measured σ(θ). 30Si deduced levels, L, in, J, π, S. Enriched targets.

doi: 10.1016/0375-9474(73)90761-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1756.


1973GA30      Aust.J.Phys. 26, 747 (1973)

P.R.Gardner, D.C.Kean, R.H.Spear, A.M.Baxter, R.A.I.Bell, L.E.Carlson

Spin-Parity Combinations in 32S

NUCLEAR REACTIONS 32S(α, α'), (p, p'), (p, p'γ), Eα=16.8-18.2 MeV, Ep=11.2, 9.16 MeV; measured σ(E, Eα', θ), σ(Ep', θ), p'γ-coin. 32S deduced levels, J, π.

doi: 10.1071/PH730747
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0663.


1973GA31      Aust.J.Phys. 26, 739 (1973)

P.R.Gardner, A.M.Baxter, R.A.I.Bell, L.E.Carlson, D.C.Kean, T.R.Ophel, R.H.Spear

Polarization Studies of Ground-State Radiation from the 2.21 and 2.73 MeV Levels of 27Al

NUCLEAR REACTIONS 27Al(p, p'γ), E=4.41 MeV; measured Eγ, Iγ, γ(θ), γγcoin, P(γ). 27Al levels deduced γ-mixing.

doi: 10.1071/PH730739
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1973MO06      Aust.J.Phys. 26, 17 (1973)

C.E.Moss, R.H.Spear, F.Ahmad, A.M.Baxter, L.E.Carlson, P.R.Gardner

Gamma Ray Decay Schemes of Levels at Intermediate Energies in 32S

NUCLEAR REACTIONS 32S(p, p'γ), E=8.03-9.17 MeV; measured pγ-coin. 32S levels deduced branching ratios.

doi: 10.1071/PH730017
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1971OL01      Can.J.Phys. 49, 594 (1971)

R.W.Ollerhead, G.F.R.Allen, A.M.Baxter, B.W.J.Gillespie, J.A.Kuehner

Spin-Parity Combinations in 22Ne

NUCLEAR REACTIONS 22Ne(α, α'), E=16.5-21.0 MeV; measured σ(Eα'). 22Ne deduced levels, J, π.

doi: 10.1139/p71-077
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1971OL06      Can.J.Phys. 49, 2589 (1971)

R.W.Ollerhead, G.F.R.Allen, A.M.Baxter, J.A.Kuehner

Spin-Parity Combinations in 18O

NUCLEAR REACTIONS 18O(α, α'), E=20-23.4 MeV; measured σ(E;Eα'). 18O deduced levels, J, π.

doi: 10.1139/p71-309
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1970BA47      Can.J.Phys. 48, 2434 (1970)

A.M.Baxter, B.W.J.Gillespie, J.A.Kuehner

Gamma-Ray Polarization Measurements in 22Na

NUCLEAR REACTIONS 19F(α, nγ), E=6.13, 7.00 MeV; measured σ(Eγ, θ(γ)), γ-linear polarization. 22Na levels deduced J, π, γ-mixing. Ge(Li) detectors.

doi: 10.1139/p70-305
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1969BA46      Can.J.Phys. 47, 2319 (1969)

A.M.Baxter, K.J.Cassell, J.A.Kuehner

Resonance Strengths and Decay Schemes in 23Na(p, γ)24Mg

NUCLEAR REACTIONS 23Na(p, γ), E = 0.5-1.5 MeV; measured σ(E;Eγ), Doppler shift attenuation. 24Mg deduced resonances, level-width. 24Mg deduced levels, J, π, branching ratios, T1/2.

doi: 10.1139/p69-282
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1969BA47      Can.J.Phys. 47, 2327 (1969)

A.M.Baxter, C.Mabey, B.W.J.Gillespie, J.A.Kuehner

Angular Correlations in 23Na(p, γ)24Mg

NUCLEAR REACTIONS 23Na(p, γ), E = 1.020, 1.318 MeV; measured γγ(θ). 24Mg deduced resonances, J. 24Mg level deduced J, π.

doi: 10.1139/p69-283
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1968BA17      Nucl.Phys. A112, 209(1968)

A.M.Baxter, J.A.R.Griffith, S.W.Oh, S.Roman

Polarization in the Elastic Scattering of 12 MeV Deuterons by 12C, 56Fe and 58Ni

NUCLEAR REACTIONS 12C, 56Fe, 58Ni(polarized d, d), Ed=12 MeV; measured vector polarization < iT11(θ) > . Enriched 56Fe, 58Ni targets.

doi: 10.1016/0375-9474(68)90231-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0264.


1968BA19      Phys.Rev.Letters 20, 1114 (1968)

A.M.Baxter, J.A.R.Griffith, S.Roman

Polarization-Vector Analyzing Power of the Reactions 9Be(d, p)10Be and 12C(d, p)13C

NUCLEAR STRUCTURE 12C, 9Be; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.20.1114
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1966SH10      Nucl.Phys. 83, 460(1966)

G.G.Shute, A.M.Baxter

Angular Correlations for 12C(p, p'γ)12C (II.) Overlapping Resonances and the Missing 5/2- Level in 13N

NUCLEAR REACTIONS 12C(p, p'γ), E = 5.9 MeV; measured σ(θ p', θ γ). 13N level deduced J, π. Natural target.

doi: 10.1016/0029-5582(66)90584-0
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1964BA14      Nucl. Phys. 52, 385 (1964)

A.M.Baxter, K.G.McIntyre, G.G.Shute, D.Robson

Angular Correlations for C12(p, p'γ)C12 in a Resonance-Free Region

NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(64)90702-3
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1961BA25      Australian J.Phys. 14, 196 (1961) Nuclear Sci.Abstr. 15, 2957, Abstr.22942 (1961); See Keynumber 1961MC11

V.R.McKenna, A.M.Baxter, G.G.Shute

Energy Levels in 13N

NUCLEAR STRUCTURE 12C, 13N; measured not abstracted; deduced nuclear properties.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0934.


1961MC11      Australian J.Phys. 14, 196 (1961) Nuclear Sci.Abstr. 15, 2957, Abstr.22942 (1961)

V.R.McKenna, A.M.Baxter, G.G.Shute

Energy Levels in 13N

NUCLEAR REACTIONS 12C(p, p), E=5-11.5 MeV; measured reaction products, Ep, Ip. 13N; deduced σ(θ), resonance structures, level energies.


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