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Search: Author = W.J.Vermeer

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1996UR03      Phys.Rev. C54, 2264 (1996)

W.Urban, T.Rzaca-Urban, J.L.Durell, Ch.P.Hess, C.J.Pearson, W.R.Phillips, B.J.Varley, W.J.Vermeer, Ch.Vieu, J.S.Dionisio, M.Pautrat, J.C.Bacelar

Excited Levels in 145Pm

NUCLEAR REACTIONS 134Xe(15N, 4n), E=78 MeV; measured Eγ, Iγ, γγ(θ), linear polarization. 146Nd(d, 3n), E=18 MeV; measured γγ-, (electron)γ-coin. 145Pm deduced high-spin levels, J, π, single-particle configurations, ICC, γ-multipolarity.

doi: 10.1103/PhysRevC.54.2264
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1995RZ02      Nucl.Phys. A588, 767 (1995)

T.Rzaca-Urban, W.Urban, J.L.Durell, W.R.Phillips, B.J.Varley, Ch.P.Hess, C.J.Pearson, W.J.Vermeer, Ch.Vieu, J.S.Dionisio, M.Pautrat, J.C.Bacelar

Study of the High-Spin Structure of 146Pm

NUCLEAR REACTIONS 136Xe(15N, 5n), E=78 MeV; 146Nd(d, 2n), E=18 MeV; measured γγ(t), DCO ratios, Iγ, (e)(γ)-coin. 146Pm deduced levels, J, π, ICC, Iγ, branchings. Solid 136Xe target. Shell-model calculations.

doi: 10.1016/0375-9474(95)00065-9
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1995UR01      Nucl.Phys. A587, 541 (1995)

W.Urban, J.L.Durell, W.R.Phillips, B.J.Varley, Ch.P.Hess, M.A.Jones, C.J.Pearson, W.J.Vermeer, Ch.Vieu, J.S.Dionisio, M.Pautrat, J.C.Bacelar

Study of Excited Levels in 147Pm

NUCLEAR REACTIONS 136Xe(15N, 4n), E=78 MeV; 148Nd(d, 3n), E=18 MeV; measured γγ(t), DCO ratios, Iγ, Eγ. 147Pm deduced levels, J, π, T1/2, ICC, Iγ, branching, configurations, octupole deformation.

doi: 10.1016/0375-9474(95)00018-V
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1994KH01      Nucl.Phys. A567, 495 (1994)

M.K.Khan, W.J.Vermeer, W.Urban, J.B.Fitzgerald, A.S.Mowbray, B.J.Varley, J.L.Durell, W.R.Phillips

Band Structures and Octupole Correlation Effects in 151Sm

NUCLEAR REACTIONS 150Nd(α, 3n), E=35 MeV; measured γγ-coin, γγ(θ). 151Sm deduced levels, J, π, Iγ, γ-branching.

doi: 10.1016/0375-9474(94)90021-3
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1994PE03      Phys.Rev. C49, R1239 (1994)

C.J.Pearson, W.R.Phillips, J.L.Durell, B.J.Varley, W.J.Vermeer, W.Urban, M.K.Khan

Opposite-Parity Bands in 153Eu

NUCLEAR REACTIONS 150Nd(7Li, 4n), E=40 MeV; measured Eγ, Iγ, γγ(θ). 153Eu deduced levels, J, π, B(E1), B(E2), δ, band structure.

doi: 10.1103/PhysRevC.49.R1239
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1994SM15      Nucl.Instrum.Methods Phys.Res. A350, 314 (1994)

A.G.Smith, W.J.Vermeer

Automated Peak Searching and Fitting of Data from Gamma-Ray Coincidence Experiments

RADIOACTIVITY 248Cm(SF); 160Er(EC); analyzed γγ-, γγγ-coin data. Automated peak searching codes.

NUCLEAR REACTIONS 116Cd(48Ca, xnp), E=210 MeV; analyzed γγ-, γγγ-coin data. Automated peak searching codes.

doi: 10.1016/0168-9002(94)91180-0
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1993RO05      Nucl.Phys. A554, 322 (1993)

B.A.Robson, R.H.Spear, W.J.Vermeer, M.Zielinska-Pfabe

Low-Energy Behaviour of the Heavy-Ion Optical Model Potentials for 12C and 16O Scattering from 208Pb

NUCLEAR REACTIONS 208Pb(12C, 12C), (12C, 12C'), E=42-61 MeV; measured σ(θ); deduced model parameters. Coupled-channels analysis, other data analyzed.

doi: 10.1016/0375-9474(93)90344-W
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1993VE04      Nucl.Phys. A559, 422 (1993)

W.J.Vermeer, W.Urban, M.K.Khan, C.J.Pearson, A.B.Wiseman, B.J.Varley, J.L.Durell, W.R.Phillips

Gamma-Decays of 151Eu Levels Populated in the 150Nd(6Li, 5n) Reaction

NUCLEAR REACTIONS 150Nd(6Li, 5n), E=47 MeV; measured γγ-coin, γγ(θ), Iγ. 151Eu deduced levels, J, π, Iγ, branchings.

doi: 10.1016/0375-9474(93)90161-P
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1990VE02      Phys.Lett. 234B, 219 (1990)

W.J.Vermeer

Shape Isomerism in 22Na ( Question )

NUCLEAR STRUCTURE 22Na; calculated levels, B(λ), spectroscopic quadrupole moments. Shell model.

doi: 10.1016/0370-2693(90)91917-Z
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1990VE14      Phys.Rev. C42, R1183 (1990)

W.J.Vermeer, M.K.Khan, A.S.Mowbray, J.B.Fitzgerald, J.A.Cizewski, B.J.Varley, J.L.Durell, W.R.Phillips

Octupole Correlation Effects in 151Pm

NUCLEAR REACTIONS 150Nd(α, 2np), E=35 MeV; measured Eγ, Iγ, γγ-coin. 151Pm deduced levels, J, π, ICC, γ-multipolarity.

doi: 10.1103/PhysRevC.42.R1183
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1989LI05      Phys.Rev. C39, 1142 (1989)

C.S.Lim, R.H.Spear, W.J.Vermeer, M.P.Fewell

Possible Discontinuity in Octupole Behavior in the Pt-Hg Region

NUCLEAR REACTIONS 194,196,198Pt(α, α'), E=14.6 MeV; 194,196,198Pt(12C, 12C'), E=43 MeV; 194,196,198Pt(7Li, 7Li'), E not given; measured particle spectra following Coulomb excitation. 194,196,198Pt levels deduced B(λ).

doi: 10.1103/PhysRevC.39.1142
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1989PR01      Nucl.Phys. A499, 117 (1989)

D.M.Pringle, W.J.Vermeer

Alpha-Particle Decay Widths of Levels in 19F

NUCLEAR REACTIONS 12C(11B, α), E=33, 35, 38, 48 MeV; measured σ(Eα), σ(Eα, E(19F)). 19F deduced levels, Γγ/Γ, Γα.

doi: 10.1016/0375-9474(89)90273-X
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1989SP07      Aust.J.Phys. 42, 345 (1989)

R.H.Spear, W.J.Vermeer, S.M.Burnett, G.J.Gyapong, C.S.Lim

Coulomb Excitation of 142Ce and 144Nd

NUCLEAR REACTIONS 142Ce(α, α'), E=10, 12, 11.8 MeV; 142Ce, 144Nd(12C, 12C'), E=35 MeV; 142Ce(16O, 16O'), E=46 MeV; 144Nd(16O, 16O'), E=48 MeV; measured particle spectra following Coulomb excitation. 142Ce, 144Nd levels deduced B(λ), static quadrupole moments.

doi: 10.1071/PH890345
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1989VE01      Phys.Lett. 217B, 28 (1989)

W.J.Vermeer, D.M.Pringle, E.F.Garman, I.F.Wright

Yrast 8+ and 9+ States of 22Na

NUCLEAR REACTIONS 12C(14N, α), E=32, 33 MeV; measured σ(Eα), αγ-coin. 22Na deduced levels, T1/2, Γγ/Γ, possible J, π.

doi: 10.1016/0370-2693(89)91510-4
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1989VE07      Nucl.Phys. A500, 212 (1989)

W.J.Vermeer, R.H.Spear, F.C.Barker

The Value of B(E2;3/2- → 1/2-) for 7Li

NUCLEAR STRUCTURE 7Li; analyzed Coulomb excitation reaction data; deduced transition B(E2).

doi: 10.1016/0375-9474(89)90138-3
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1988LI01      Phys.Lett. 200B, 263 (1988)

C.S.Lim, M.D.Rebgetz, R.H.Spear, W.J.Vermeer, M.P.Fewell, B.A.Robson, R.Smith

Energy Dependence of the 16O-208Pb Effective Interaction

NUCLEAR REACTIONS 208Pb(16O, 16O), (16O, 16O'), E=57-79 MeV; measured σ(ratio). 208Pb level deduced excitation probability. Effective interaction description, Coulomb-nuclear interference effects.

doi: 10.1016/0370-2693(88)90768-X
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1988LI22      Nucl.Phys. A485, 399 (1988)

C.S.Lim, R.H.Spear, W.J.Vermeer, M.P.Fewell, G.J.Gyapong

Electric Quadrupole Moments of the First Excited State of 192Os

NUCLEAR REACTIONS 192Os(α, α'), E=14.2-16.5 MeV; 192Os(12C, 12C'), E=40-55 MeV; 192Os(12C, 12C'), E=44-47 MeV; measured Coulomb excitation probabilities. 192Os levels deduced B(E2), static quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(88)90110-8
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1988VE06      Nucl.Phys. A485, 380 (1988)

W.J.Vermeer, D.M.Pringle, I.F.Wright

Measurements of Γ(γ)/Γ for States of 24Mg in the Excitation Region 10 < E(x) < 12 MeV

NUCLEAR REACTIONS 12C(16O, α), E=31.73, 32.80, 33.85, 34.70 MeV; measured σ(E(α)), σ(E(α), E(24Mg)). 24Mg deduced levels, Γ(γ)/Γ, Γ(α), Γ(γ).

doi: 10.1016/0375-9474(88)90109-1
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1988VE08      Phys.Rev. C38, 2982 (1988)

W.J.Vermeer, C.S.Lim, R.H.Spear

Mixed Symmetry in the Vibrational Nucleus 142Ce

NUCLEAR REACTIONS 142Ce(α, α'), E=10-12 MeV; 142Ce(12C, 12C'), E=31-38 MeV; 142Ce(16O, 16O'), E=44-50 MeV; measured particle spectra following Coulomb excitation. 142Ce levels deduced B(λ), quadrupole moment.

doi: 10.1103/PhysRevC.38.2982
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1987FI01      Nucl.Phys. A463, 644 (1987)

L.K.Fifield, D.M.Pringle, W.J.Vermeer

Gamma-Ray Decaying States at High Excitation in 20Ne

NUCLEAR REACTIONS 12C(12C, α), E=37.1 MeV; measured σ(Eα, E(20Ne)). 20Ne deduced levels, γ-branching ratios.

doi: 10.1016/0375-9474(87)90636-1
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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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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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1983VE03      Phys.Rev. C28, 432 (1983)

W.J.Vermeer, R.K.Bhalla, A.R.Poletti

Mean Life of 10B(718 keV) and Its Role in Determining the Giant Dipole Resonance Contribution to Coulomb Excitation of 10B

NUCLEAR REACTIONS 10B(p, p'), E=4.5 MeV; measured pγ-coin. 10B level deduced T1/2. Enriched target.

doi: 10.1103/PhysRevC.28.432
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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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1982VE04      J.Phys.(London) G8, 743 (1982)

W.J.Vermeer, A.R.Poletti

Determination of Partial Decay Widths for the 2-, 8.87 MeV Level in 16O

NUCLEAR REACTIONS 19F(p, α), E=7.4 MeV; measured Eγ, Iγ, αγ-coin. 16O levels deduced transition strength, γ-branching, δ.

doi: 10.1088/0305-4616/8/5/014
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1982VE05      J.Phys.(London) G8, 851 (1982)

W.J.Vermeer, A.R.Poletti

Branching Ratio for the Isoscalar Transition 2+, T=1, 1.95 MeV → 0+, T=1, 0.66 MeV in 22Na

NUCLEAR REACTIONS 19F(α, n), (α, α'), E=5 MeV; measured γγ-coin. 19F deduced γ-branching upper limits. 22Na transition deduced branching ratio, B(E2).

doi: 10.1088/0305-4616/8/6/014
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1982VE09      Nucl.Phys. A389, 185 (1982)

W.J.Vermeer, M.T.Esat, R.H.Spear

Quadrupole Moment of the First Excited State of 32S

NUCLEAR REACTIONS 208Pb(32S, 32S'), E=122-160 MeV; measured Coulomb excitation probabilities. 32S level deduced quadrupole moment, B(E2). Enriched target.

doi: 10.1016/0375-9474(82)90297-4
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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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