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NSR database version of April 27, 2024.

Search: Author = J.D.MacArthur

Found 20 matches.

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1996OU01      Phys.Rev. C54, 1982 (1996)

J.M.L.Ouellet, M.N.Butler, H.C.Evans, H.W.Lee, J.R.Leslie, J.D.MacArthur, W.McLatchie, H.-B.Mak, P.Skensved, J.L.Whitton, X.Zhao

12C(α, γ)16O Cross Sections at Stellar Energies

NUCLEAR REACTIONS, ICPND 12C(α, γ), E=1.5-3 MeV; measured σ(θ); deduced E1, E2 σ, astrophysical S-factor. K-matrix, R-matrix, cluster models.

doi: 10.1103/PhysRevC.54.1982
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0439.

1992OU01      Phys.Rev.Lett. 69, 1896 (1992)

J.M.L.Ouellet, H.C.Evans, H.W.Lee, J.R.Leslie, J.D.MacArthur, W.McLatchie, H.-B.Mak, P.Skensved, J.L.Whitton, X.Zhao, T.K.Alexander

12C(α, γ)16O Cross Sections at Stellar Energies

NUCLEAR REACTIONS, ICPND 12C(α, γ), E(cm)=1.37-2.98 MeV; measured σ(E), Iγ(θ); deduced E1, E2 contributions, astrophysical S-factor. Three-level R-matrix method, cluster model analysis.

doi: 10.1103/PhysRevLett.69.1896
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0104.

1987PA07      Phys.Rev. C35, 1119 (1987)

S.A.Page, H.C.Evans, G.T.Ewan, S.-P.Kwan, J.R.Leslie, J.D.MacArthur, W.McLatchie, P.Skensved, S.-S.Wang, H.-B.Mak, A.B.McDonald, C.A.Barnes, T.K.Alexander, E.T.H.Clifford

Weak Pion-Nucleon Coupling Strength: New constraint from parity mixing in 18F

NUCLEAR REACTIONS 16O(3He, p), E=4.05 MeV; measured γ CP; deduced weak pion-nucleon coupling strength. 19F levels deduced parity mixing.

doi: 10.1103/PhysRevC.35.1119
Citations: PlumX Metrics

1985EV03      Phys.Rev.Lett. 55, 791 (1985)

H.C.Evans, G.T.Ewan, S.-P.Kwan, J.R.Leslie, J.D.MacArthur, H.-B.Mak, W.McLatchie, S.A.Page, P.Skensved, S.-S.Wang, A.B.McDonald, C.A.Barnes, T.K.Alexander, E.T.H.Clifford

Parity Mixing of 0+ and 0- Levels in 18F

NUCLEAR REACTIONS 16O(3He, p), E=4.05 MeV; measured Eγ, Iγ, γ CP; deduced weak pion-nucleon coupling constant. 18F transition deduced parity nonconserving matrix element.

doi: 10.1103/PhysRevLett.55.791
Citations: PlumX Metrics

1985MA32      Phys.Rev. C32, 314 (1985)

J.D.MacArthur, S.-P.Kwan, H.-B.Mak, W.McLatchie, S.A.Page, S.-S.Wang, T.K.Alexander

Experimental Evidence Against the Proposed Band Based on a Shape Isomer in 32S

NUCLEAR REACTIONS 28Si(α, γ), E=1.76-3.82 MeV; σ(Eγ, E), γ yield, γ(θ). 32S level deduced J, π, B(λ).

doi: 10.1103/PhysRevC.32.314
Citations: PlumX Metrics

1982EV01      Nucl.Instrum.Methods 192, 143 (1982)

H.C.Evans, G.T.Ewan, J.R.Leslie, J.D.MacArthur, H.-B.Mak, W.McLatchie, R.C.Turnock, M.B.Woods

A Cryopumped Transmission Gas Target for Nuclear Structure Studies

NUCLEAR REACTIONS 14N(α, α)(α, γ), E ≈ 1517.5-1535 keV; measured σ(θ, E), σ(Eγ). 16O(α, γ), E=3.020, 3.036 MeV; measured Eγ, Iγ. 20Ne deduced E2 transition strength. Differentially pumped transmission gas target.

doi: 10.1016/0029-554X(82)90816-3
Citations: PlumX Metrics

1980MA26      Nucl.Phys. A343, 79 (1980)

H.-B.Mak, G.T.Ewan, H.C.Evans, J.D.MacArthur, W.McLatchie, R.E.Azuma

The Alpha Widths of the 5603, 5605 and 5668 keV States in 18F

NUCLEAR REACTIONS 14N(α, α), E=1.5, 1.6 MeV; measured σ(θ, Eα). 18F resonances deduced Γα. R-matrix formalism. Differentially pumped natural nitrogen gas target.

doi: 10.1016/0375-9474(80)90641-7
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1279.

1980MA27      Phys.Rev. C22, 356 (1980)

J.D.MacArthur, H.C.Evans, J.R.Leslie, H.-B.Mak

First Two Members of the K=0- Band in 20Ne

NUCLEAR REACTIONS 16O(α, α), E=1305-1330 keV, 2950-3075 keV; measured σ(E, θ); 16O(α, γ), E=1.37, 2.6, 2.9, 3.036 MeV; measured σ(E), Eγ. 20Ne resonances deduced Γα, B(λ), Γγ.

NUCLEAR STRUCTURE 16O, 40,48Ca, 60Ni, 90Zr, 116Sn, 140Ce, 208Pb, 238U; calculated binding energies. Energy density formalism, generalized Thomas-Fermi form, variational procedure.

doi: 10.1103/PhysRevC.22.356
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0693.

1978MA30      Nucl.Phys. A304, 210 (1978)

H.-B.Mak, H.C.Evans, G.T.Ewan, J.D.Macarthur

The 18O(p, α)15N Cross Section at Low Energies

NUCLEAR REACTIONS 18O(p, α), E=240-700 keV; measured σ(E, θ); deduced S.

doi: 10.1016/0375-9474(78)90104-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1917.

1976MA23      Can.J.Phys. 54, 1134 (1976)

J.D.MacArthur, A.J.Brown, P.A.Butler, L.L.Green, C.J.Lister, A.N.James, P.J.Nolan, J.F.Sharpey-Schafer

Properties of the Levels in 22Na Deduced from the 19F(α, nγ)22Na Reaction

NUCLEAR REACTIONS 19F(α, nγ), E=9.1 MeV; measured σ(Eγ, θ), linear polarization, DSA. 22Na deduced levels, K, J, π, T1/2, γ-branching, quadrupole moment.

doi: 10.1139/p76-137
Citations: PlumX Metrics

1976NO03      J.Phys.(London) G2, 249 (1976)

P.J.Nolan, A.J.Brown, P.A.Butler, L.L.Green, A.N.James, C.J.Lister, J.D.MacArthur, J.F.Sharpey-Schafer

Gamma Ray Spectroscopy Studies in the Nuclei 36Ar and 36Cl

NUCLEAR REACTIONS 33S(α, nγ), (α, pγ), E=6.0-14.0 MeV; measured σ(E, Eγ, θ), γγ-coin, recoil distance, linear polarization. 36Ar, 36Cl deduced levels, J, π, T1/2, δ, γ-branching. Ge(Li) detectors, enriched targets.

doi: 10.1088/0305-4616/2/4/010
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2110.

1976NO05      J.Phys.(London) G2, 569 (1976)

P.J.Nolan, A.J.Brown, P.A.Butler, L.L.Green, A.N.James, J.R.Leslie, C.J.Lister, J.D.MacArthur, J.F.Sharpey-Schafer

Levels in 37Cl between 4 and 9 MeV in Excitation

NUCLEAR REACTIONS 34S(α, pγ), E=14, 17 MeV; measured pγ-coin, angular distributions, DSAM. 37Cl deduced levels, J, π, δ, T1/2, γ-branching. Enriched targets, Ge(Li), NaI(Tl), Si detectors.

doi: 10.1088/0305-4616/2/8/008
Citations: PlumX Metrics

1975BU14      J.Phys. (London) G1, 665 (1975)

P.A.Butler, A.J.Brown, L.L.Green, A.N.James, C.J.Lister, J.D.MacArthur, P.J.Nolan, J.F.Sharpey-Schafer

Electromagnetic and Angular Momentum Properties of States in 25Mg below 6.05 MeV in Excitation

NUCLEAR REACTIONS 22Na(α, nγ), E=8.00, 9.15 MeV; measured σ(Eγ, θ), linear polarization. 25Mg levels deduced J, π, δ, γ-branching, quadrupole moment, g.

doi: 10.1088/0305-4616/1/6/014
Citations: PlumX Metrics

1975BU15      J.Phys. (London) G1, 543 (1975)

P.A.Butler, A.J.Brown, P.E.Carr, L.L.Green, A.N.James, C.J.Lister, J.D.MacArthur, P.J.Nolan, J.F.Sharpey-Schafer

Electromagnetic and Angular Momentum Properties of States in 33S below 5.0 MeV in Excitation

NUCLEAR REACTIONS 30Si(α, nγ), E=6.7, 8.0, 9.8 MeV; measured σ(Eγ, θ), polarization. 33S deduced levels, J, π, δ, γ-branching.

doi: 10.1088/0305-4616/1/5/007
Citations: PlumX Metrics

1975NO01      J.Phys.(London) G1, 35 (1975)

P.J.Nolan, L.L.Gadeken, A.J.Brown, P.A.Butler, L.L.Green, C.J.Lister, A.N.James, J.D.MacArthur, J.F.Sharpey-Schafer, D.A.Viggars

Properties of 37Ar II. Levels Above 3.8 MeV Excitation Energy

NUCLEAR REACTIONS 34S(α, nγ), E=10.5-16.0 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, DSA, pγ. 37Ar deduced levels, J, π, γ-mixing, T1/2, γ-branching ratios, transition strengths.

doi: 10.1088/0305-4616/1/1/006
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1373.

1970HE14      Can.J.Phys. 48, 1040 (1970)

A.W.Herman, E.A.Heighway, J.D.MacArthur

Beta Decay of 187W

RADIOACTIVITY 187W; measured βγ-, γγ-, ceγ-coin, Eβ, Iβ; deduced Q, log ft. 187Re deduced levels, ICC, γ-multipolarity, J, π. Ge(Li), Si(Au), NaI(Tl) detectors.

doi: 10.1139/p70-135
Citations: PlumX Metrics

1965MA10      Nucl.Phys. 61, 394 (1965)

J.D.MacArthur, M.W.Johns

The Decay of Ir194

RADIOACTIVITY 194Ir[from 193Ir(n, γ)]; measured βγ-, βce-, γγ-, γ ce-coin, γγ(θ); deduced Iβ, Iγ. 194Pt deduced levels, J.

doi: 10.1016/0029-5582(65)90101-X
Citations: PlumX Metrics

1964KA22      Phys.Canada 20, No.2, 35, Abstr.7.3 (1964)

M.Kawamura, J.D.MacArthur

Coincidence Measurements in the Decay of Ir192

NUCLEAR STRUCTURE 192Ir; measured not abstracted; deduced nuclear properties.

1964MA39      Phys.Canada 20, No.2, 35, Abstr.7.4 (1964)

J.D.MacArthur, M.W.Johns

The Decay of Ir194

NUCLEAR STRUCTURE 194Ir; measured not abstracted; deduced nuclear properties.

1959JO35      Can.J.Phys. 37, 1205 (1959)

M.W.Johns, J.D.MacArthur

Zero Spin of the 1265-keV State in Pt194

doi: 10.1139/p59-139
Citations: PlumX Metrics

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