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Search: Author = M.P.Fewell

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1992LI14      Nucl.Phys. A548, 308 (1992)

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

Measurements of Static Electric Quadrupole Moments of the 2+1, 2+2, 4+1 and 6+1 States of 196Pt

NUCLEAR REACTIONS 196Pt(α, α), E=14.2-15.8 MeV; 196Pt(7Li, 7Li), E=22, 22.5 MeV; 196Pt(12C, 12C), E=42-46 MeV; 196Pt(58Ni, 58Ni), E=214-226 MeV; measured (particle)γ-coin, Eγ, Iγ, γγ(θ), Coulomb excitation probabilities. 196Pt levels deduced B(E2), B(E4), static quadrupole moments.

doi: 10.1016/0375-9474(92)90013-A
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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1988FE01      Phys.Rev. C37, 101 (1988)

M.P.Fewell, N.R.Johnson, F.K.McGowan, J.S.Hattula, I.Y.Lee, C.Baktash, Y.Schutz, J.C.Wells, L.L.Riedinger, M.W.Guidry, S.C.Pancholi

Lifetimes of Yrast and Near-Yrast States of 159,160,161Yb

NUCLEAR REACTIONS 116Cd(48Ti, xn), E=205 MeV; 48Ti(116Cd, xn), E=495 MeV; measured Eγ, Iγ, total energy spectra, recoil distance. 159,160,161Yb deduced levels, J, π, sidefeeding Iγ, transition quadrupole moments, band structure.

doi: 10.1103/PhysRevC.37.101
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1988FE04      Nucl.Instrum.Methods Phys.Res. A269, 202 (1988)

M.P.Fewell

Hexadecapole Reorientation in Coulomb Excitation

NUCLEAR REACTIONS 192Os(120Sn, 120Sn'), E=300-495 MeV; 184W(58Ni, 58Ni'), E=100-300 MeV; 194Pt(208Pb, 208Pb'), E=0.2-1 GeV; calculated Coulomb excitation probability, hexadecapole moment dependence; deduced hexadecapole reorientation effects.

doi: 10.1016/0168-9002(88)90878-9
Citations: PlumX Metrics


1988FE08      Aust.J.Phys. 41, 37 (1988)

M.P.Fewell, G.J.Gyapong, R.H.Spear

Coulomb Excitation of the 41+ States of 194,196,198Pt

NUCLEAR REACTIONS 194,196Pt(α, α'), E=14.199-15.599; 198Pt(α, α'), E=15.599 MeV; 194,198Pt(12C, 12C'), E=40.998-49.998 MeV; 196Pt(12C, 12C'), E=40.985-55.996 MeV; 194Pt(16O, 16O'), E=54.998-62.998 MeV; 196Pt(16O, 16O'), E=54.993-60.994 MeV; 198Pt(16O, 16O'), E=56.997-62.998 MeV; measured Coulomb excitation probability. 194,196,198Pt levels deduced E2, E4 transition matrix elements, deformation parameters.

doi: 10.1071/PH880037
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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
Citations: PlumX Metrics


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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1987LE01      Phys.Rev. C35, 605 (1987)

I.Y.Lee, C.Baktash, J.R.Beene, M.P.Fewell, M.L.Halbert, N.R.Johnson, F.K.McGowan, W.T.Milner, H.J.Kim, R.O.Sayer, D.G.Sarantites

Distributions of the Total Energy and Multiplicity of Gamma Rays feeding the Discrete Yrast States in Heavy-Ion-Induced Fusion Reactions

NUCLEAR REACTIONS 150Sm(12C, 4n), (12C, 3n), E=65 MeV; 100Mo(34S, 4n), E=144 MeV; 70Zn(50Ti, 4n), (50Ti, 3n), E=170 MeV; measured γ-multiplicities, total energy distributions. 158,159Er, 130Ce, 116,117Te deduced entry state distribution width vs yrast transition spin. Ge, NaI detectors, spin spectrometer.

doi: 10.1103/PhysRevC.35.605
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1986FE02      Phys.Lett. 167B, 6 (1986)

M.P.Fewell

Plantinum-196 as a U(5) Nucleus

NUCLEAR STRUCTURE 196Pt; calculated levels, B(E2); deduced U(5) limit validity. Interacting boson model.

doi: 10.1016/0370-2693(86)90534-4
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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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1986MC01      Phys.Rev. C33, 855 (1986)

F.K.McGowan, N.R.Johnson, I.Y.Lee, W.T.Milner, C.Roulet, J.Hattula, M.P.Fewell, Y.A.Ellis-Akovali, R.M.Diamond, F.S.Stephens, M.W.Guidry

Test of the Triaxial Rotor Model and the Interacting Boson Fermion Approximation Model Description of Collective States in 191Ir

NUCLEAR REACTIONS 191Ir(40Ar, 40Ar'), E=160 MeV; 191Ir(136Xe, 136Xe'), E=617 MeV; measured Eγ, Iγ(θ) following Coulomb excitation. 191Ir deduced levels, J, π, B(λ).

doi: 10.1103/PhysRevC.33.855
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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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1985BA06      Phys.Rev.Lett. 54, 978 (1985)

C.Baktash, Y.Schutz, I.Y.Lee, F.K.McGowan, N.R.Johnson, M.L.Halbert, D.C.Hensley, M.P.Fewell, L.Courtney, A.J.Larabee, L.L.Riedinger, A.W.Sunyar, E.der Mateosian, O.C.Kistner, D.G.Sarantites

Quasivibrational Bands at High Spins in 158Yb

NUCLEAR REACTIONS 98Mo(64Ni, 4n), E=285 MeV; 144Sm(18O, 4n), E=100 MeV; 142Nd(20Ne, 4n), E=115 MeV; measured γγ-coin, γγ(θ), γ(θ). 158Yb deduced levels, J, π, γ-branching, moment of inertia, band structure.

doi: 10.1103/PhysRevLett.54.978
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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.


1985CA12      Phys.Rev. C31, 1049 (1985)

J.L.S.Carvalho, F.M.Bernthal, R.M.Ronningen, N.R.Johnson, J.S.Hattula, I.Y.Lee, M.P.Fewell, L.L.Riedinger, J.C.Wells

High Spin States in 128Ce

NUCLEAR REACTIONS 112Cd(20Ne, 4n), E=103 MeV; measured γγ-coin, γ(θ). 128Ce deduced levels, J, π, γ-branching, backbending plots. Compared with theory.

doi: 10.1103/PhysRevC.31.1049
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1985FE02      Phys.Rev. C31, 1057 (1985)

M.P.Fewell, N.R.Johnson, F.K.McGowan, J.S.Hattula, I.Y.Lee, C.Baktash, Y.Schutz, J.C.Wells, L.L.Riedinger, M.W.Guidry, S.C.Pancholi

Collectivity of 160,161Yb at High Spin

NUCLEAR REACTIONS 116Cd(48Ti, xn), 48Ti(116Cd, xn), E(cm)=145 MeV; measured γ-spectra, recoil distance. 160,161Yb levels deduced T1/2, γ-branching, quadrupole moments, yrast sequence, quasiparticle alignment role, induced triaxiality.

doi: 10.1103/PhysRevC.31.1057
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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
Citations: PlumX Metrics


1985FE05      Aust.J.Phys. 38, 555 (1985)

M.P.Fewell, R.H.Spear, G.K.Adam, M.T.Esat

Determination of B(E3; 0+1 → 3-1) Values for the Stable Isotopes of Cadmium

NUCLEAR REACTIONS 106,116,108,110,112,114Cd(16O, 16O'), E=40-44 MeV; measured σ(E(16O)) following Coulomb excitation. 106,108,110,112,114,116Cd deduced transition B(E3), no shell effects.

doi: 10.1071/PH850555
Citations: PlumX Metrics


1984FE08      Nucl.Phys. A425, 373 (1984)

M.P.Fewell

First-Order Relativistic Corrections to the Theory of Coulomb Excitation

NUCLEAR REACTIONS 194Pt(16O, 16O'), E=63 MeV; 194Pt(58Ni, 58Ni'), E=230 MeV; 194Pt(136Xe, 136Xe'), E=550 MeV; calculated Coulomb excitation probability, relativistic corrections. 198Hg(16O, 16O'), E=63 MeV; 198Hg(58Ni, 58Ni'), E=230 MeV; 198Hg(136Xe, 136Xe'), E=550 MeV; analyzed Coulomb excitation data. 198Hg level deduced B(E2), quadrupole moment relativistic corrections.

doi: 10.1016/0375-9474(84)90081-2
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1984LA11      Phys.Rev. C29, 1934 (1984)

A.J.Larabee, L.H.Courtney, S.Frauendorf, L.L.Riedinger, J.C.Waddington, M.P.Fewell, N.R.Johnson, I.Y.Lee, F.K.McGowan

Shape Effects in h11/2 and g7/2 Bands in 159Tm

NUCLEAR REACTIONS 148Sm(14N, 3n), 141Pr(22Ne, 4n), E not given; measured γγ-, γγγ-coin, γ(θ), γγ(θ). 159Tm deduced levels, J, π, γ-branching, B(λ) ratios, rotational band structure, δ, backbend characteristics, configuration.

doi: 10.1103/PhysRevC.29.1934
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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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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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1984WE17      Phys.Rev. C30, 1532 (1984)

J.C.Wells, N.R.Johnson, J.Hattula, M.P.Fewell, D.R.Haenni, I.Y.Lee, F.K.McGowan, J.W.Johnson, L.L.Riedinger

Evidence for Collective Behavior in 128Ce from Lifetime Measurements

NUCLEAR REACTIONS 92Zr(40Ar, 4n), E=159 MeV; measured Eγ, Iγ, γ(t), Doppler shift, recoil. 128Ce deduced yrast level T1/2, J, π, band characteristics, B(E2). Cranked self-consistent theory.

doi: 10.1103/PhysRevC.30.1532
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1983GR10      Nucl.Phys. A401, 362 (1983)

E.E.Gross, J.R.Beene, K.A.Erb, M.P.Fewell, D.Shapira, M.J.Rhoades-Brown, G.R.Satchler, C.E.Thorn

Elastic and Inelastic Scattering of 120 MeV 18O from 208Pb and the Spin Alignment of the 2+ State of 18O

NUCLEAR REACTIONS 208Pb(18O, 18O), (18O, 18O'), E=120 MeV; measured σ(E(18O), θ), Doppler broadened line shapes. 18O deduced substate population, excited state hexadecapole moment. Enriched target. Coupled-channels analysis.

doi: 10.1016/0375-9474(83)90533-X
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1983GR28      Nucl.Phys. A411, 329 (1983)

E.E.Gross, M.P.Fewell

Resolution of a Coulomb Reorientation Ambiguity in 18O

NUCLEAR REACTIONS 208Pb(18O, 18O), (18O, 18O'), E=120 MeV; analyzed σ(θ). 18O level deduced quadrupole moment, resolved Coulomb excitation ambiguities.

doi: 10.1016/0375-9474(83)90395-0
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1982DR03      Nucl.Phys. A383, 119 (1982)

G.D.Dracoulis, C.Fahlander, M.P.Fewell

High-Spin Yarst and Non-Yarst Bands in 176Os, 178Os, and 180Os

NUCLEAR REACTIONS 164,166,168Er(16O, 4n), E=80-105 MeV; measured σ(E, θ), γγ-coin, γγ(t). 176,178,180Os deduced levels, J, π, T, rotational bands, ICC. 180Os deduced isomer, configuration. Ge, Ge(Li), Compton-suppressed detector. Band-mixing calculations.

doi: 10.1016/0375-9474(82)90080-X
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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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1980DR10      Phys.Rev.Lett. 45, 1831 (1980)

G.Dracoulis, C.Fahlander, M.P.Fewell

Mass Dependence of the Yrast-Yrare Interaction and Backbending in the Light Osmium Isotopes

NUCLEAR REACTIONS Er(16O, 4n), (16O, 5n), E not given; measured Eγ, Iγ, γγ(t), γ(θ). 176,178,180,182Os deduced levels, J, π, rotational band structure, backbending. 178,180Os deduced yrast-yrare matrix elements.

doi: 10.1103/PhysRevLett.45.1831
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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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1980SP09      Aust.J.Phys. 33, 509 (1980); Corrigendum Aust.J.Phys. 34, 609 (1981)

R.H.Spear, M.P.Fewell

Static Quadrupole Moment of the First Excited State of 28Si

NUCLEAR REACTIONS 208Pb(28Si, 28Si'), E=94.88-104.86, 109.85-139.81 MeV; measured σ(E(28Si'), θ), reorientation effect in Coulomb excitation. 28Si level deduced B(E2), static quadrupole momement. Si surface barrier detectors. Hartree-Fock, shell model interpretation.

doi: 10.1071/PH800509
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1979FE05      Nucl.Phys. A319, 214 (1979)

M.P.Fewell, S.Hinds, D.C.Kean, T.H.Zabel

Static Quadrupole Moment of the First Excited State of 24Mg

NUCLEAR REACTIONS 208Pb(24Mg, 24Mg'), E=80-110 MeV, θ(lab)=90°, 172°; measured Coulomb excitation probability of 24Mg first 2+ state; deduced quadrupole moment, B(E2;0+→2+). Enriched target.

doi: 10.1016/0375-9474(79)90182-9
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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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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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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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