Nuclear Science References (NSR)

NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of April 27, 2024.

Search: Author = R.H.Spear

Found 89 matches.

Back to query form

2005KI02 At.Data Nucl.Data Tables 89, 77 (2005)

T.Kibedi, R.H.Spear

Electric monopole transitions between 0⁺ states for nuclei throughout the periodic table

COMPILATION A=4-250; compiled, analyzed 0⁺ → 0⁺ transition energies, T_1/2, ICC, electric monopole transition strengths.

doi: 10.1016/j.adt.2004.11.002
Citations: PlumX Metrics

2002KI06 At.Data Nucl.Data Tables 80, 35 (2002)

T.Kibedi, R.H.Spear

Reduced Electric-Octupole Transition Probabilities, B(E3;0₁⁺ → 3₁^-) - An Update

COMPILATION Z=4-98; compiled transitions B(E3), octupole deformation parameters.

doi: 10.1006/adnd.2001.0871
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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

1991LI03 Nucl.Phys. A522, 635 (1991)

C.S.Lim, W.N.Catford, R.H.Spear

Measurements of E3 Transition Strength in the Stable Even-Mass Hg Isotopes

NUCLEAR REACTIONS ¹⁹⁸Hg(¹²C, ¹²C'), E=54 MeV; ^202,204,200Hg(¹²C, ¹²C'), E=54, 55 MeV; measured Coulomb excitation probabilities. ^{200,198,202,204}Hg levels deduced B(E3). Enriched targets.

doi: 10.1016/0375-9474(91)90086-L
Citations: PlumX Metrics

1990SP01 Phys.Rev. C41, R1351 (1990)

R.H.Spear, W.N.Catford

Information on Octupole Deformation from Systematics of B(E3;0₁⁺ → 3₁^-) Values

NUCLEAR STRUCTURE N ≤ 150; analyzed B(E3) data; deduced octupole deformation role.

doi: 10.1103/PhysRevC.41.R1351
Citations: PlumX Metrics

1989BA80 Aust.J.Phys. 42, 597 (1989)

F.C.Barker, Y.Kondo, R.H.Spear

Static and Dynamic Moments of the ⁷Li Nucleus

NUCLEAR REACTIONS ⁵⁸Ni(polarized ⁷Li, ⁷Li), (polarized ⁷Li, ⁷Li'), E=8-10 MeV; ¹²⁰Sn(polarized ⁷Li, ⁷Li), (polarized ⁷Li, ⁷Li'), E=11-15.3 MeV; analyzed σ(θ), analyzing power data following Coulomb excitation. ⁷Li deduced B(E2), quadrupole, other moments.

doi: 10.1071/PH890597
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
Citations: PlumX Metrics

1989SP01 At.Data Nucl.Data Tables 42, 55 (1989)

R.H.Spear

Reduced Electric-Octupole Transition Probabilities, B(E3;0₁⁺ → 3₁^-), for Even-Even Nuclides Throughout the Periodic Table

COMPILATION Z=4-98; compiled adopted B(E3).

doi: 10.1016/0092-640X(89)90032-6
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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

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
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
Citations: PlumX Metrics

1986BA38 Astrophys.J. 307, 847 (1986)

F.C.Barker, R.H.Spear

A Comment on the ⁷Be(p, γ)⁸B Cross Section and the Solar Neutrino Problem

NUCLEAR REACTIONS, ICPND ⁷Li(d, p), E=0.77 MeV; analyzed σ. ⁷Be(p, γ), E=0.1-4 MeV; analyzed σ, ratio to ⁷Li(d, p), S-factor vs E data; deduced inaccuracies, consequences to solar neutrino problem.

doi: 10.1086/164471
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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 ^{132,134,136,138}Ba using Coulomb Excitation

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

doi: 10.1016/0375-9474(85)90257-X
Citations: PlumX Metrics

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

doi: 10.1016/0375-9474(85)90146-0
Citations: PlumX Metrics
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
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 ^{106,116,108,110,112,114}Cd(¹⁶O, ¹⁶O'), E=40-44 MeV; measured σ(E(¹⁶O)) following Coulomb excitation. ^{106,108,110,112,114,116}Cd deduced transition B(E3), no shell effects.

doi: 10.1071/PH850555
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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 ^{198,200,202,204}Hg, ^204,206,208Pb(α, α'), E=24, 27 MeV; measured σ(Eα'). ^{198,200,202,204}Hg, ^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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0862.

1981ES02 Phys.Rev. C23, 1822 (1981)

M.T.Esat, R.H.Spear, J.L.Zyskind, M.H.Shapiro, W.A.Fowler, J.M.Davidson

Test of Global Hauser-Feshbach Calculations for Proton-Induced Reactions on ⁶⁸Zn

NUCLEAR REACTIONS ⁶⁸Zn(p, γ), E=1.67-4.97 MeV; ⁶⁸Zn(p, α), E=3.36-5.48 MeV; ⁶⁸Zn(p, n), E=3.77-5.03 MeV; measured σ(E). Hauser-Feshbach calculations. Enriched targets.

doi: 10.1103/PhysRevC.23.1822
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0650.

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
Citations: PlumX Metrics

1981MO03 Phys.Rev. C23, 932 (1981)

I.Morrison, R.H.Spear

Triaxiality in the Even-Mass Hg Isotopes: A Discontinuity at ²⁰⁰Hg

NUCLEAR STRUCTURE ^{196,198,200,202,204}Hg; analyzed level systematics, B(E2) data; ²⁰⁰Hg deduced change in neutron, proton density distributions. Extended interacting boson approximation.

doi: 10.1103/PhysRevC.23.932
Citations: PlumX Metrics

1981SP07 Phys.Rep. 73, 369 (1981)

R.H.Spear

Static Quadrupole Moments of the First 2⁺ States in the 2s-1d Shell: A review of experiment and theory

COMPILATION ¹⁸O, ^20,22Ne, ^24,26Mg, ^28,30Si, ^32,34S, ^36,40Ar; compiled, analyzed quadrupole moments.

doi: 10.1016/0370-1573(81)90177-0
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1979SP01 Nucl.Phys. A318, 21 (1979)

R.H.Spear, Z.E.Switkowski, D.L.Kennedy, J.C.P.Heggie

Resonance Strength of the 1175 keV Resonance in ⁶Li(α, γ)¹⁰B

NUCLEAR REACTIONS ⁶Li(α, γ), E=1140-1250 keV; measured σ(E). ¹⁰B 5166 keV level deduced resonance strength. Enriched target.

doi: 10.1016/0375-9474(79)90466-4
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0855.

1979SW02 Nucl.Phys. A331, 50 (1979)

Z.E.Switkowski, J.C.P.Heggie, D.L.Kennedy, D.G.Sargood, F.C.Barker, R.H.Spear

Cross Section of the Reaction ⁶Li(p, γ)⁷Be

NUCLEAR REACTIONS ⁶Li(p, γ), E=200-1200 keV; measured σ(E). Enriched target.

doi: 10.1016/0375-9474(79)90300-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0032.

1979ZY01 Nucl.Phys. A315, 430 (1979)

J.L.Zyskind, J.M.Davidson, M.T.Esat, R.H.Spear, M.H.Shapiro, W.A.Fowler, C.A.Barnes

Cross Section Measurements and Thermonuclear Reaction Rates for ⁴⁸Ca(p, γ)⁴⁹Sc and ⁴⁸Ca(p, n)⁴⁸Sc

NUCLEAR REACTIONS ⁴⁸Ca(p, γ), ⁴⁸Ca(p, n), E=0.58-2.67 MeV; measured σ(E); deduced thermonuclear reaction rates as function of temperature. Hauser-Feshbach calculations. Enriched target. Ge(Li), BF₃ long counter.

doi: 10.1016/0375-9474(79)90620-1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0670.

1979ZY04 Nucl.Phys. A331, 180 (1979)

J.L.Zyskind, J.M.Davidson, M.T.Esat, M.H.Shapiro, R.H.Spear

Competition Cusps in (α, γ) Reactions

NUCLEAR REACTIONS ³⁷Cl(α, γ), E=2.9-5.23 MeV; ⁶²Ni(α, γ), E=5.07-8.64 MeV; ⁶²Ni(α, n), E=6.95-8.76 MeV; ⁶⁴Ni(α, γ), E=4.5-7.45 MeV; ⁶⁴Ni(α, n), E=5.3-7.45 MeV; measured σ(E). Hauser-Feshbach calculations. Enriched target, Ge(Li) detector, BF₃ long counter.

doi: 10.1016/0375-9474(79)90308-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0669.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1978ZY03 Nucl.Phys. A301, 179 (1978)

J.L.Zyskind, J.M.Davidson, M.T.Esat, M.H.Shapiro, R.H.Spear

A cusp in the ⁵⁴Cr(p, γ)⁵⁵Mn reaction

NUCLEAR REACTIONS ⁵⁴Cr(p, γ), ⁵⁴Cr(p, n), E=796 keV-3.7 MeV; measured products, ⁵⁵Mn, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry C0671.

doi: 10.1016/0375-9474(78)90136-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0136.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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

doi: 10.1071/PH770133
Citations: PlumX Metrics

1976ES01 Phys.Lett. 61B, 242 (1976)

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

Quadrupole Moments in the Cadmium Isotopes

NUCLEAR REACTIONS ^{106,110,112,114,116}Cd(α, α'γ), E=8.5 MeV; ^{106,110,112,114,116}Cd(¹⁶O, ¹⁶O'γ), E=44 MeV; measured Coulomb excitation. ^{106,110,112,114,116}Cd levels deduced B(E2).

doi: 10.1016/0370-2693(76)90139-8
Citations: PlumX Metrics

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

doi: 10.1016/0375-9474(76)90239-6
Citations: PlumX Metrics

1975BA53 Nucl.Instrum.Methods 127, 269 (1975)

J.N.Barrandon, J.L.Debrun, A.Kohn, R.H.Spear

Etude du Dosage de Ti, V, Cr, Fe, Ni, Cu et Zn par Activation avec des Protons d'Energie Limitee a 20 MeV

NUCLEAR REACTIONS Ti, V, Cr, Fe, Ni, Cu, Zn(p, xnγ), E=0-20 MeV; measured activation yields.

doi: 10.1016/0029-554X(75)90499-1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0086.

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
Citations: PlumX Metrics

1973FR07 Can.J.Phys. 51, 1155 (1973)

G.G.Frank, R.V.Elliott, R.H.Spear, J.A.Kuehner

High-Spin States in ²³Na

NUCLEAR REACTIONS ¹²C(¹²C, pγ), E=27-29 MeV; measured Eγ, Iγ, σ(Ep), DSA, pγ(θ). ²³Na deduced levels, γ-branching, T_1/2, J, π.

doi: 10.1139/p73-154
Citations: PlumX Metrics

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
Citations: PlumX Metrics
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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1972GA43 Aust.J.Phys. 25, 659 (1972)

P.R.Gardner, C.E.Moss, R.H.Spear, L.E.Carlson

The 5.80 MeV State of ³²S

NUCLEAR REACTIONS ²⁹Si(α, nγ), E=8.7, 8.8, 9.8 MeV; measured σ(E, Eγ, θ), Doppler shift; ³²S(p, p'γ), E=8.63 MeV; measured Eγ, Iγ. ³²S level deduced J, π, T_1/2, γ-branching.

doi: 10.1071/PH720659
Citations: PlumX Metrics

1972PI03 Can.J.Phys. 50, 1286 (1972)

A.A.Pilt, R.H.Spear, R.V.Elliott, D.T.Kelly, J.A.Kuehner, G.T.Ewan, C.Rolfs

Band Structure in ²¹Ne

NUCLEAR REACTIONS ¹⁸O(α, nγ), E=5.2, 6.1 MeV; measured γγ-coin, γ-linear polarization, Iγ(θ). ²¹Ne levels deduced J, π, γ-mixing, γ-branching. Ge(Li) detectors.

doi: 10.1139/p72-176
Citations: PlumX Metrics

1971BA27 Aust.J.Phys. 24, 1 (1971)

F.C.Barker, K.W.Carter, D.C.Kean, C.J.Piluso, R.H.Spear

A Study of the Energy Levels of ²⁷Si

NUCLEAR REACTIONS ²⁸Si(³He, α), E=11 MeV; measured σ(Eα). ²⁷Si deduced levels.

1971CA38 Aust.J.Phys. 24, 471 (1971)

K.W.Carter, D.C.Kean, C.J.Piluso, R.H.Spear

A Search for High-Spin State in ²⁷Al

NUCLEAR REACTIONS ¹²C(¹⁶O, pγ), ²⁴Mg(α, pγ), E(¹⁶O) < 30 MeV, Eα=11-16 MeV; measured σ(Ep, Eγ, θ(γ), θ(pγ)). ²⁷Al deduced levels, J, π, γ-branching.

1971DO04 Can.J.Phys. 49, 483 (1971)

C.Doekes, D.C.Kean, R.V.Elliott, R.H.Spear

High Resolution Study of the Energy Levels of ²⁷Al

NUCLEAR REACTIONS ²⁷Al(p, p'), E=15 MeV; measured σ(Ep', θ). ²⁷Al deduced levels.

doi: 10.1139/p71-062
Citations: PlumX Metrics

1971PI03 Can.J.Phys. 49, 1263 (1971)

A.A.Pilt, R.H.Spear, R.V.Elliott, J.A.Kuehner

Positive-Parity Bands in ²⁹Si

NUCLEAR REACTIONS ²⁶Mg(α, nγ), E=5.54, 6.30 MeV; measured σ(Eγ, θ), γ-linear polarization. ²⁹Si deduced levels, J, π, γ-branching, γ-mixing.

doi: 10.1139/p71-151
Citations: PlumX Metrics

1971PI06 Aust.J.Phys. 24, 459 (1971)

C.J.Piluso, R.H.Spear, K.W.Carter, D.C.Kean, F.C.Barker

Magnetic Analysis of the Reactions ⁷Li(³He, d)⁸Be and ⁷Li(³He, t)⁷Be

NUCLEAR REACTIONS ⁷Li(³He, d), (³He, t), E=15 MeV; measured σ(Ed, θ), σ(Et, θ). ^7,8Be deduced levels, level-width.

1971SP02 Can.J.Phys. 49, 355 (1971)

R.H.Spear, J.E.Cairns, R.V.Elliott, J.A.Kuehner, A.A.Pilt

Concerning a Possible K = 7/2 Negative Parity Band in ²⁹Si

NUCLEAR REACTIONS ²⁶Mg(α, nγ), E=5.54, 6.30 MeV; measured σ(Eγ;θ(γ)), γ-linear polarization. ²⁹Si levels deduced J, π, γ-mixing.

doi: 10.1139/p71-041
Citations: PlumX Metrics

1969CA04 Nucl.Phys. A126, 49(1969)

K.W.Carter, R.V.Elliott, D.C.Kean, R.H.Spear

Angular-Correlation Studies of the Reaction ²⁴Mg(α, pγ)²⁷Al

NUCLEAR REACTIONS ²⁴Mg(α, pγ), E=9.1, 13.0 MeV; measured σ(Ep, Eγ, θ(pγ)). ²⁷Al levels deduced γ-branching, J, π, delta. Enriched target.

doi: 10.1016/0375-9474(69)90399-6
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0684.

1969CA12 Nucl.Phys. A134, 505(1969)

K.W.Carter, D.C.Kean, C.J.Piluso, R.H.Spear

The 4.41 and 4.51 MeV Levels of ²⁷Al

NUCLEAR REACTIONS ²⁴Mg(α, pγ), E = 10.51 MeV; measured α, pγ(θ), Eγ, Iγ. ²⁷Al levels deduced γ-branching, J, delta. Enriched target.

doi: 10.1016/0375-9474(69)90017-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0604.

1969KE01 Nucl.Phys. A123, 430(1969)

D.C.Kean, K.W.Carter, R.H.Spear

Gamma-Ray Branching Ratios of the Low-Lying Levels of ²⁹Al

NUCLEAR REACTIONS ²⁶Mg(α, pγ), E=10.4-10.9 MeV; measured σ(Eγ, Ep). ²⁹Al levels deduced γ-branchings. Enriched target.

doi: 10.1016/0375-9474(69)90511-9
Citations: PlumX Metrics

1969KE08 Nucl.Phys. A132, 241 (1969)

D.C.Kean, K.W.Carter, C.J.Piluso, R.H.Spear

Angular Correlation Studies of the Low-Lying Levels of ²⁹Al

NUCLEAR REACTIONS ²⁶Mg(α, pγ), E=10.6, 11.3 MeV; measured σ(Ep, Eγ, θ), Eγ, Iγ. ²⁹Al levels deduced γ-branching, J, delta. Enriched target.

doi: 10.1016/0375-9474(69)90481-3
Citations: PlumX Metrics

1968EL05 Nucl.Phys. A115, 673(1968)

R.V.Elliott, T.R.Ophel, R.H.Spear

Branching Ratios of ²⁷Al Bound States

NUCLEAR REACTIONS ²⁴Mg(α, pγ), E = 9.0 MeV; ²⁷Al(p, p'γ), E = 5.8, 7.0 MeV; measured Eγ, Iγ. ²⁷Al levels deduced γ-branching. Enriched target.

doi: 10.1016/0375-9474(68)90758-6
Citations: PlumX Metrics

1968EL10 Nucl.Instr.Methods 59, 29 (1968)

R.V.Elliott, K.W.Carter, R.H.Spear

The Use of Position-Sensitive Solid State Detector to Measure Properties of a Magnetic Spectrometer

RADIOACTIVITY ²¹²Bi; measured Eα.

doi: 10.1016/0029-554X(68)90340-6
Citations: PlumX Metrics

1968KE07 Australian J. Phys. 21, 405 (1968)

D.C.Kean, R.V.Elliott, R.H.Spear

A Study of the 3.00 MeV Level of ²⁷Al via ²⁴Mg(α, pγ)²⁷Al

NUCLEAR STRUCTURE ²⁷Al; measured not abstracted; deduced nuclear properties.

doi: 10.1071/PH680405
Citations: PlumX Metrics

1968SP04 Australian J. Phys. 21, 307 (1968)

R.H.Spear, I.F.Wright

Gamma Radiation from the Reactions ²⁰Ne(α, α'γ₁. ₆₃)²⁰Ne and ²⁰Ne(α, pγ₀. ₄₄)²³Na

NUCLEAR STRUCTURE ²⁴Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1071/PH680307
Citations: PlumX Metrics

1966EL06 Nucl.Phys. 84, 209(1966)

R.V.Elliott, R.H.Spear

Proton Scattering from ²⁷Al in the Energy Range from 3.5 to 11.3 MeV

NUCLEAR REACTIONS ²⁷Al(p, p), (p, p'), E=3.5-11.3 MeV; measured σ(E;Ep'). ²⁸Si deduced mean level width.

doi: 10.1016/0029-5582(66)90443-3
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0391.

1965BU04 Nucl.Phys. 65, 655 (1965)

I.F.Bubb, J.M.Poate, R.H.Spear

Excitation Function of the Reaction Al²⁷(p, n)Si²⁷

NUCLEAR REACTIONS ²⁷Al(p, n), E=5.8-11.2 MeV; measured σ(E). ²⁸Si deduced mean level width. ²⁷Si[from ²⁷Al(p, n)]; measured T_1/2. Natural target.

doi: 10.1016/0029-5582(65)90332-9
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetP0027.

1964LA16 Nucl.Phys. 56, 497(1964)

J.D.Larson, R.H.Spear

Gamma Radiation from the Alpha Particle Bombardment of C¹²

NUCLEAR REACTIONS ¹²C(α, γ), (α, α'γ), Eα=2.8-8.3 MeV; measured σ(E, θ), γ-spectrum. ¹⁶O deduced levels, J, π, resonance parameters.

doi: 10.1016/0029-5582(64)90498-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1056.

1964PE05 Nucl.Phys. 54, 434(1964)

J.D.Pearson, R.H.Spear

A Study of the Gamma Radiation Produced in the Alpha-Particle Bombardment of O¹⁶

NUCLEAR REACTIONS ¹⁶O(α, γ), Eα=4.8-9.9 MeV; measured σ(E), γ-spectrum, αγ(θ), γγ(θ). ¹⁶O(α, α'γ), Eα=8.9-9.9 MeV; measured σ(E). ²⁰Ne deduced levels, J, π, level-width, level-width γ.

doi: 10.1016/0029-5582(64)90425-0
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0910.

1963SP02 Nucl.Phys. 41, 353 (1963)

R.H.Spear, J.D.Larson, J.D.Pearson

Excitation Function for the Reaction C¹³(α, nγ)O¹⁶

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

doi: 10.1016/0029-5582(63)90514-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0993.

1962SP01 Bull.Amer.Phys.Soc. 7, 4, 286, FB8 (1962)

R.H.Spear, J.D.Larson

Excitation Function for C¹³(α, nγ)O¹⁶

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

1961LA13 Bull.Am.Phys.Soc. 6, No.6, 505, E1 (1961)

J.D.Larson, R.H.Spear

Excitation Function for Gamma Radiation from C¹² + α

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

1961PE17 Bull.Am.Phys.Soc. 6, No.6, 505, E2 (1961)

J.D.Pearson, R.H.Spear

Excitation Function of Gamma Radiation from O¹⁶ + α

NUCLEAR STRUCTURE ¹⁶O; measured not abstracted; deduced nuclear properties.