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Search: Author = W.McLatchie

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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.


1990RA23      Phys.Rev. C42, R2275 (1990)

T.J.Radcliffe, T.K.Alexander, G.C.Ball, H.C.Evans, J.R.Leslie, H.-B.Mak, W.McLatchie, P.Skensved, A.T.Stewart

Search for Resonances in the Electron-Positron Annihilation-in-Flight Cross Section between 1 and 4 MeV

NUCLEAR REACTIONS 19F(p, α), E=1.27 MeV; measured e+-spectra in Ge following 16O-decay; deduced e+e- annihilation-in-flight σ.

doi: 10.1103/PhysRevC.42.R2275
Citations: PlumX Metrics


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


1984AD06      Phys.Rev. C30, 1153 (1984)

E.Adamides, W.McLatchie, P.Skensved, J.R.Leslie

Lifetimes of States in 97Tc

NUCLEAR REACTIONS 97Mo(p, nγ), E=3.5 MeV; measured Eγ, Iγ(θ), DSA. 97Tc deduced T1/2, B(E2), B(M1), δ, B(E1) values. Ge(Li) detector, Ge(Li)-NaI(Tl) anti-Compton spectrometer, enriched targets.

doi: 10.1103/PhysRevC.30.1153
Citations: PlumX Metrics


1984EV01      Can.J.Phys. 62, 1139 (1984)

H.C.Evans, I.P.Johnstone, J.R.Leslie, W.McLatchie, H.-B.Mak, P.Skensved, T.K.Alexander

The Branching Ratio in the Decay of 7Be

RADIOACTIVITY 7Be(EC) [from 10B(p, α), E=2 MeV]; measured Eγ, Iγ; deduced vector coupling constant G(A). 7Li level deduced EC-branching ratio.

NUCLEAR REACTIONS 10B(p, α), E=2 MeV; measured Eγ, Iγ, recoil σ(E(7Be)), σ(Eα). 7Li level deduced EC-decay branching ratio.

doi: 10.1139/p84-158
Citations: PlumX Metrics


1983KO18      Nucl.Phys. A403, 155 (1983)

R.L.Kozub, D.J.Fields, C.B.Chitwood, Jr., T.K.Alexander, G.C.Ball, J.S.Forster, H.-B.Mak, W.McLatchie

Lifetimes of Levels in 25Na and 26,27Mg Excited via the 26Mg Bombardment of 3H

NUCLEAR REACTIONS 3H(26Mg, α), (26Mg, t), (26Mg, d), E=40 MeV; measured Doppler broadened lineshapes, (particle)γ-coin. 25Na, 26,27Mg levels deduced T1/2. Compared to shell model calculations.

doi: 10.1016/0375-9474(83)90194-X
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


1981CH04      Can.J.Phys. 59, 238 (1981)

C.-W.Cheng, S.K.Saha, J.Keinonen, H.-B.Mak, W.McLatchie

Hydrogen Burning of 39K in Explosive Oxygen Burning

NUCLEAR REACTIONS 39K(p, γ), E=0.7-2.9 MeV; measured Iγ(θ), branching ratios; deduced astrophysical reaction rates of 39K hydrogen burning. 40Ca resonance deduced relative, absolute γ transition strengths.

doi: 10.1139/p81-030
Citations: PlumX Metrics


1981SK01      Nucl.Phys. A366, 125 (1981)

P.Skensved, R.Chapman, R.L.Kozub, J.R.Leslie, W.McLatchie, D.Ward, H.R.Andrews, O.Hausser

The Ground-State Rotational Band in 175Lu

NUCLEAR REACTIONS 175Lu(40Ca, 40Ca'), E=168 MeV; γ40Ca(θ), recoil, Eγ, Iγ, γ(θ), DSA, Coulomb excitation. 175Lu levels deduced T1/2, B(λ), δ, γ-branching ratio, quadrupole moment, g(k), g(R).

doi: 10.1016/0375-9474(81)90492-9
Citations: PlumX Metrics


1980BA40      Nucl.Phys. A349, 271 (1980)

G.C.Ball, O.Hausser, T.K.Alexander, W.G.Davies, J.S.Foster, I.V.Mitchell, J.R.Beene, D.Horn, W.McLatchie

Electric Quadrupole Moments of the First Excited States of 28Si, 32S and 34S

NUCLEAR REACTIONS 4He(32S, α), (34S, α), E=70 MeV; measured Doppler-broadened line shapes, αγ(t). 32,34S levels deduced T1/2. 208Pb(28Si, 28Si'), E=105 MeV; 208Pb(32S, 32S'), (34S, 34S'), E=122 MeV; measured σ(θ, E(28Si)), σ(θ, E(32S)), σ(θ, E(34S)), Coulomb excitation. 32,34S, 28Si level deduced static quadrupole moment, B(E2). Enriched targets.

doi: 10.1016/0375-9474(80)90454-6
Citations: PlumX Metrics


1980CO02      Can.J.Phys. 58, 359 (1980)

B.E.Cooke, J.R.Leslie, W.McLatchie, P.Skensved

An Examination of Doppler Shift Attenuation Factors and Lifetimes for Excited Nuclear States in 59Cu and 63Cu

NUCLEAR REACTIONS 58,62Ni(p, γ), E=resonance; measured DSA, capture γ. 59,63Cu resonances deduced T1/2, γ transition strength.

doi: 10.1139/p80-051
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1980KE05      Phys.Rev. C22, 351 (1980)

J.Keinonen, H.-B.Mak, P.Skensved, J.R.Leslie, W.M.McLatchie

Lifetime of the 1.04 MeV State in 18F

NUCLEAR REACTIONS 18O(p, n), E=3.75 MeV; measured DSA. 18F level deduced T1/2. Implanted target.

doi: 10.1103/PhysRevC.22.351
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.


1979BA31      Nucl.Phys. A325, 305 (1979)

G.C.Ball, W.G.Davies, J.S.Forster, H.R.Andrews, D.Horn, W.McLatchie

The Use of Exotic Heavy Ion Transfer Reactions to Study Light Neutron Rich Nuclei

NUCLEAR REACTIONS 207,208Pb(18O, 21O), (18O, 22O), (18O, 19N), (18O, 17O), E=93 MeV; measured position spectra; deduced Q. 21,22O, 19N, 17C deduced mass excess. Enriched targets, QD3 spectrometer analysis.

doi: 10.1016/0375-9474(79)90165-9
Citations: PlumX Metrics


1979KI12      Nucl.Phys. A327, 172 (1979)

W.E.Kieser, R.E.Azuma, I.Berka, K.P.Jackson, A.B.McDonald, H.B.Mak, W.McLatchie

The Jπ = 3- Doublet at E = 6241 keV in 18F: Isospin Mixing

NUCLEAR REACTIONS 4He(14N, α), E=8.19-8.32 MeV; measured Iα(E, θ). 14N(α, γ), E=2.35, 2.53 MeV; measured Eγ, Iγ(θ), absolute strength of γ-transition. 17O(p, γ), E=0.67 MeV; measured Eγ, Iγ(θ), absolute strength of γ-transition. 17O(p, α), E=0.67 MeV; measured Iα, absolute strength of γ-transition. 18F levels deduced J, π, Eα, T, Γp, Γα, Γγ. Natural, enriched targets.

doi: 10.1016/0375-9474(79)90323-3
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1978MC07      Nucl.Phys. A305, 151 (1978)

A.B.McDonald, E.D.Earle, W.McLatchie, H.B.Mak, D.J.Martin, P.G.Ikossi

Isospin-Forbidden Particle Decays in Light Nuclei (IV). Total Width of the Lowest T = 2 Level of 24Mg

NUCLEAR REACTIONS 23Na(p, γ), (p, p), (p, α), E ≈ 3.9 MeV; measured σ(E). 24Mg deduced lowest T=2, J, π=0+ level, total Γ.

doi: 10.1016/0375-9474(78)90169-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0409.


1977CO03      J.Phys.(London) G3, 391 (1977)

B.E.Cooke, J.R.Leslie, W.McLatchie, B.C.Robertson

A Comparison of Two Independent Measurements of the Lifetime of a State in 59Cu

NUCLEAR REACTIONS 58Ni(p, γ), E=1833, 3547 keV; measured σ(E, Eγ, θ), DSA. 59Cu deduced levels, resonances, J, T1/2, Γ.

doi: 10.1088/0305-4616/3/3/014
Citations: PlumX Metrics


1977TA10      Nucl.Phys. A289, 165 (1977)

P.Taras, D.Ward, H.R.Andrews, J.S.Geiger, R.L.Graham, W.McLatchie

Electromagnetic Properties of the Ground State Rotational Band in 169Tm

NUCLEAR REACTIONS 169Tm(32S, 32S'γ), E=130, 140 MeV; measured recoil distance, DSA, 32S'γ(θ), Eγ, Iγ. 169Tm levels deduced transitions, δ, T1/2, B(λ), γ-branching.

doi: 10.1016/0375-9474(77)90527-9
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1976CO11      J.Phys.(London) G2, 131 (1976)

B.E.Cooke, R.L.Kozub, W.McLatchie, T.K.Alexander, J.S.Forster, C.Broude, J.R.Beene

Lifetimes of Levels in 36,37Cl and 34S Excited by the 35Cl Bombardment Of 3H

NUCLEAR REACTIONS 3H(35Cl, pγ), (35Cl, dγ), (35Cl, αγ), E=55 MeV; measured recoil distance, particle γ-coin. 37,36Cl, 34S levels deduced T1/2.

doi: 10.1088/0305-4616/2/2/009
Citations: PlumX Metrics


1976DA18      Nucl.Phys. A269, 477 (1976)

W.G.Davies, R.M.DeVries, G.C.Ball, J.S.Forster, W.McLatchie, D.Shapira, J.Toke, R.E.Warner

A Comparison of α-Transfer and α-Decay in the Lead Region

NUCLEAR REACTIONS 204,207,208Pb, 209Bi(16O, 12C), E=93 MeV; measured σ(θ). 208,211,212Po, 213At levels deduced S, Γα. DWBA analysis, resolution 200 keV, θ=60-104°.

doi: 10.1016/0375-9474(76)90694-1
Citations: PlumX Metrics


1976MA08      Nucl.Phys. A258, 131 (1976)

D.J.Martin, W.McLatchie, B.C.Robertson, J.Szucs

The 1g9/2 Analogue State in 55Co

NUCLEAR REACTIONS 54Fe(p, γ), E=3.47 MeV; measured σ(E, Eγ, θ), Q, resonance strength. 55Co deduced M1, E1 rates, 9/2+ analog, antianalog states. Enriched target.

doi: 10.1016/0375-9474(76)90534-0
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1976MI01      Phys.Rev. C13, 879 (1976)

G.F.Millington, R.M.Hutcheon, J.R.Leslie, W.McLatchie

Energy of the Lowest T=2 State in 20F

NUCLEAR REACTIONS 18O(3He, pγ), E=5 MeV; measured Ep, Eγ. 20F deduced resonance. 20Na, 20Mg; calculated mass excess.

doi: 10.1103/PhysRevC.13.879
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1975CO21      Can.J.Phys. 53, 2506 (1975)

B.E.Cooke, J.R.Leslie, B.C.Robertson, W.McLatchie

A Detailed Study of the g9/2 Analogue Resonance in 59Cu by the 58Ni(p, γ)59Cu Reaction

NUCLEAR REACTIONS 58Ni(p, γ), E=3.5-3.6 MeV; measured σ(E, Eγ, θ). 59Cu deduced level, resonance, J, π, Γ.

doi: 10.1139/p75-304
Citations: PlumX Metrics


1975DE22      Phys.Rev.Lett. 35, 835 (1975)

R.M.DeVries, D.Shapira, W.G.Davies, G.C.Ball, J.S.Forster, W.McLatchie

Inverse α Decay via the Reaction 208Pb(16O, 12C)212Po

NUCLEAR REACTIONS 208Pb(16O, 12C), E=93 MeV; measured σ(E(12C), θ). 212Po levels deduced S.

doi: 10.1103/PhysRevLett.35.835
Citations: PlumX Metrics


1975FR22      Nucl.Phys. A255, 351 (1975)

G.G.Frank, B.C.Robertson, W.McLatchie

The Lifetime of the 8543 and 8945 keV Levels in 28Si

NUCLEAR REACTIONS 27Al(p, γ), E=2.677, 3.096 MeV; measured Eγ, Doppler shift attenuation. 28Si levels deduced T1/2. Ge(Li) detector.

doi: 10.1016/0375-9474(75)90685-5
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1975TR05      Nucl.Phys. A246, 457 (1975)

J.P.Trentelman, B.E.Cooke, J.R.Leslie, W.McLatchie, B.C.Robertson

A Study of the 58Ni(p, γ)59Cu Reaction

NUCLEAR REACTIONS 58Ni(p, γ), E=0.9-2.3 MeV; measured σ(E, Eγ, θ). 59Cu deduced levels, analog resonances, J, t, γ-mixing, γ-branching ratios.

doi: 10.1016/0375-9474(75)90659-4
Citations: PlumX Metrics


1974ES01      Nucl.Phys. A232, 139 (1974)

M.T.Esat, J.R.Leslie, W.McLatchie

Resonances in the Reaction 56Fe(p, γ)57Co

NUCLEAR REACTIONS 56Fe(p, γ), E=1.2-1.5 MeV; measured σ(E;Eγ, θ). 57Co deduced levels, analog resonances, J, T, γ-mixing, resonance strengths. Natural target.

doi: 10.1016/0375-9474(74)90649-6
Citations: PlumX Metrics


1974MI13      Nucl.Phys. A228, 382 (1974)

G.F.Millington, J.R.Leslie, W.McLatchie, G.C.Ball, W.G.Davies, J.S.Forster

Hole States of 20F and 20Ne

NUCLEAR REACTIONS 21Ne(d, 3He), E=26 MeV; measured σ(E(3He), θ). 20F deduced levels, L(p), J, π, S. 21Ne(d, t), E=26 MeV; measured σ(Et, θ). 20Ne deduced levelsln, J, π, S. Enriched 21Ne target.

doi: 10.1016/0375-9474(74)90609-5
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1974TR03      Z.Phys. 266, 69 (1974)

J.P.Trentelman, J.R.Leslie, W.McLatchie

The Gamma Decay of Analogue States in 61Cu

NUCLEAR REACTIONS 60Ni(p, γ), E=1840-1880, 2220-2300 keV; measured σ(Eγ, θ). 61Cu deduced resonances, γ-branching, level-width, γ-mixing.

doi: 10.1007/BF01668667
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1973MO11      Z.Phys. 261, 155 (1973)

D.G.Montague, K.Ramavataram, N.S.Chant, W.G.Davies, J.E.Kitching, W.McLatchie, J.M.Morton

States in 86Sr, 84Sr and 87Y Populated in the (p, t) Reaction

NUCLEAR REACTIONS 86,88Sr, 89Y(p, t), E=49.5 MeV; measured σ(Et, θ). 84,86Sr, 87Y deduced levels, J, π, L.

doi: 10.1007/BF01394557
Citations: PlumX Metrics


1973TR06      Nucl.Phys. A206, 393 (1973)

J.P.Trentelman, J.R.Leslie, W.McLatchie

Analogue States in 61Cu

NUCLEAR REACTIONS 60Ni(p, γ), E=1.5-1.9 MeV; measured σ(E;Eγ, θ). 61Cu deduced levels, analog resonances, J, T, γ-mixing, resonance strenths, Coulomb energy differences.

doi: 10.1016/0375-9474(73)90542-3
Citations: PlumX Metrics


1972CH11      Nucl.Phys. A186, 603 (1972)

R.Chapman, W.McLatchie, J.E.Kitching

The (t, p) Reaction on the Even Isotopes of Neodymium

NUCLEAR REACTIONS 142,144,146,148,150Nd(t, p), E=13 MeV; measured σ(Ep, θ), Q. 144,146,148,150,152Nd deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(72)90986-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1753.


1972CH40      Nucl.Phys. A196, 347 (1972)

R.Chapman, J.E.Kitching, W.McLatchie

Proton Pick-up from 92Mo

NUCLEAR REACTIONS 92Mo(t, α), Et=12 MeV; measured σ(Eα, θ). 91Nb deduced levels, L(p), S. Enriched 92Mo target.

doi: 10.1016/0375-9474(72)90969-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1763.


1972MA26      Nucl.Phys. A187, 337 (1972)

D.J.Martin, J.R.Leslie, W.McLatchie, C.F.Monahan, L.E.Carlson

The γ-Ray Decay Properties of Analogue States of 55Fe Excited in the Reaction 54Fe(p, γ)55Co

NUCLEAR REACTIONS 54Fe(p, γ), E=1.80-1.87 MeV; measured σ(E, Eγ, θ), Q, polarization. 55Co deduced levels, isobaric analog resonances, J, π, γ-mixing, resonance strengths. Enriched target.

doi: 10.1016/0375-9474(72)90581-7
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1971KI16      Nucl.Phys. A177, 433 (1971)

J.E.Kitching, W.G.Davies, W.J.Darcey, W.McLatchie, J.Morton

Effective Interaction among 1g9/2 and 2p1/2 Neutrons in the Strontium Isotopes

NUCLEAR STRUCTURE 83,84,85,86,87Sr; calculated levels, one-nucleon S, wave functions. Effective interaction shell model.

doi: 10.1016/0375-9474(71)90302-2
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1971LE21      Nucl.Phys. A170, 115 (1971)

J.R.Leslie, W.McLatchie, C.F.Monahan, J.K.Thrasher

Analogue States Excited in the Reaction 56Fe(p, γ)57Co

NUCLEAR REACTIONS 56Fe(p, γ), E=1.2-1.7 MeV; measured σ(E;Eγ, θ), Q. 57Co deduced levels, analog resonances, J, T, γ-mixing, resonance strengths. Natural target. 27Al(p, γ), E=992, 1262, 1381, 1389 keV; measured σ(E;Eγ). 28Si deduced resonance strengths.

doi: 10.1016/0375-9474(71)90686-5
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1971LE25      Phys.Lett. 36B, 76 (1971)

J.R.Leslie, D.J.Martin, W.McLatchie

Transitions between Analogue States of 55Fe

NUCLEAR REACTIONS 54Fe(p, γ), E=1803, 1887 keV; measured σ(Eγ, θ(γ)). 55Co deduced resonances, level-width, isobaric analogs, γ-branching, γ-mixing.

doi: 10.1016/0370-2693(71)90112-2
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1971MO02      Nucl.Phys. A161, 228 (1971)

J.M.Morton, W.G.Davies, W.McLatchie, W.Darcey, J.E.Kitching

The Level Structures of 85,87Sr from (d, p) Reactions

NUCLEAR REACTIONS 84,86Sr(d, p), Ed=12.0 MeV; measured σ(Ep, θ) absolute; deduced Q. 85,87Sr deduced levels, J, L, π, S. Enriched targets.

doi: 10.1016/0375-9474(71)90330-7
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1970CH03      Phys.Lett. 31B, 292 (1970)

R.Chapman, W.McLatchie, J.E.Kitching

(t, p)-Reaction Studies of the Transitional Nuclei-150Nd and 152Nd

NUCLEAR REACTIONS 148,150Nd(t, p), E=13 MeV; measured σ(θ), Q. 150,152Nd levels deduced L, deformation.

doi: 10.1016/0370-2693(70)90174-7
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1970KI10      Phys.Lett. 32B, 343 (1970)

J.E.Kitching, W.Darcey, W.G.Davies, W.McLatchie, J.M.Morton

The Conservation of Seniority in the 1g9/2 Neutron Shell

NUCLEAR REACTIONS 87Sr(p, d), E=20 MeV; measured σ(θ). 86Sr levels deduced L, seniority conservation in 1g9/2 shell.

doi: 10.1016/0370-2693(70)90490-9
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1970MA05      Nucl.Phys. A145, 223 (1970)

J.D.Macdougall, W.McLatchie, S.Whineray, H.E.Duckworth

Precise Atomic Mass Differences and Mass Systematics in the Region of 90 Neutrons

ATOMIC MASSES 141Pr, 142,143,144,145,146,148,150Nd, 147,148,149,150,152,154Sm, 151,153Eu, 154,155,156,157,158,160Gd; measured mass differences; deduced nucleon pairing, separation energies.

doi: 10.1016/0375-9474(70)90316-7
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1970MC03      Nucl.Phys. A145, 244 (1970)

W.McLatchie, S.Whineray, J.D.Macdougall, H.E.Duckworth

New Atomic Mass Differences and Mass Systematics in the Region 100 < N < 126

ATOMIC MASSES 182,183,184,186W, 185,187Re, 188,189,190Os; measured mass differences; deduced neutron pairing, separation energies.

doi: 10.1016/0375-9474(70)90317-9
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1970MC26      Nucl.Phys. A159, 615 (1970)

W.McLatchie, W.Darcey, J.E.Kitching

The Reactions 152Sm(p, t)150Sm and 154Sm(p, t)152Sm

NUCLEAR REACTIONS 152,154Sm(p, t), E=20.6 MeV; measured σ(Et, θ). 150,152Sm deduced levels, L, J, π. Enriched targets.

doi: 10.1016/0375-9474(70)90861-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1774.


1970WH01      Nucl.Phys. A151, 377 (1970)

S.Whineray, J.D.Macdougall, W.McLatchie, H.E.Duckworth

Separation and Pairing Energies Involving Isotopes of Tb, Dy, Ho, Er, Tm, Yb, Lu and Hf

ATOMIC MASSES 161,162,163,164Dy, 165Ho, 166,167,168,170Er, 169Tm, 171,172,173,174,176Yb, 175Lu, 176,177,178,179,180Hf; measured mass differences; deduced nucleon separation, pairing energies.

doi: 10.1016/0375-9474(70)90288-5
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1969DU04      Phys.Rev.Letters 23, 592 (1969)

H.E.Duckworth, R.C.Barber, P.Van Rookhuyzen, J.D.Macdougall, W.McLatchie, S.Whineray, R.L.Bishop, J.O.Meredith, P.Williams, F.C.G.Southon, W.Wong, B.G.Hogg, M.E.Kettner

Neutron Separation and Pairing Energies in the Region 82 < N < 126

doi: 10.1103/PhysRevLett.23.592
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1969MC16      Phys.Letters 30B, 529 (1969)

W.McLatchie, J.E.Kitching, W.Darcey

The Reaction 154Sm(p, t)152Sm and Further Evidence for Shape Coexistence in 152Sm

NUCLEAR REACTIONS 154Sm(p, t), E = 21 MeV; measured σ(θ). 152Sm deduced shape coexistence, no 0+ spherical state.

doi: 10.1016/0370-2693(69)90446-8
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1968DA08      Phys.Letters 27B, 363 (1968)

W.G.Davies, J.E.Kitching, W.McLatchie, D.G.Montague, K.Ramavataram, N.S.Chant

Levels Excited in the Reaction 58Ni(p, t)56Ni

NUCLEAR REACTIONS 58Ni(p, t), E=50 MeV; measured σ(θ). 56Ni deduced levels, J, π.

doi: 10.1016/0370-2693(68)90183-4
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1967MC18      Proc.Intern.Conf.Atomic Masses, 3rd, Winnipeg, Canada, R.C.Barber, Ed., Univ.Manitoba Press, p.702 (1967)

W.McLatchie, J.D.Macdougall, S.Whineray, H.E.Duckworth, R.C.Barber, B.G.Hogg, P.Van Rookhuyzen

Atomic Mass Determinations at McMaster University and the University of Manitoba Part I: Nuclear Binding Energies in the Region 82 < N < 126

NUCLEAR STRUCTURE 146Nd, 145Nd, 143Nd, 148Nd, 142Nd, 144Nd, 168Er, 165Dy, 184W, 180Hf, 152Sm, 150Sm, 150Nd, 149Sm, 179Hf, 178Hf, 175Yb, 174Yb, 173Yb, 176Yb; measured not abstracted; deduced nuclear properties.


1966MA05      Z.Naturforsch. 21a, 63 (1966)

J.D.Macdougall, W.McLatchie, S.Whineray, H.E.Duckworth

Precise Atomic Mass Differences Involving Isotopes of Nd, Sm, Cd, and Pb

NUCLEAR STRUCTURE 152Sm, 150Nd, 150Sm, 154Sm, 149Sm, 208Pb, 206Pb, 112Cd, 114Cd, 116Cd, 142Nd, 144Nd, 148Nd, 148Sm, 146Nd, 145Nd, 143Nd, 147Sm; measured not abstracted; deduced nuclear properties.


1966MA06      Bull.Am.Phys.Soc. 11, No.1, 121, HB8 (1966)

J.D.MacDougall, W.McLatchie, S.Whineray, H.E.Duckworth

Precise Atomic Mass Differences Involving Isotopes of Pr, Nd, Sm, Eu, and Gd

NUCLEAR STRUCTURE 145Nd, 146Nd, 148Nd, 144Nd, 149Sm, 154Sm, 150Nd, 150Sm, 152Sm, 153Eu; measured not abstracted; deduced nuclear properties.


1964BA03      Can. J. Phys. 42, 391 (1964)

R.C.Barber, W.McLatchie, R.L.Bishop, J.D.Macdougall, P.Van Rookhuyzen, H.E.Duckworth

Some New Mass Comparisons Involving Isotopes of Ti, V, Zn, Ge, and Se

NUCLEAR STRUCTURE 66Zn, 49Ti, 47Ti, 48Ti, 51V, 46Ti, 78Se, 80Se, 76Ge, 68Zn, 74Ge, 72Ge, 70Zn; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p64-037
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1964BA15      Phys. Rev. Letters 12, 597 (1964)

R.C.Barber, H.E.Duckworth, B.G.Hogg, J.D.Macdougall, W.McLatchie, P.Van Rookhuyzen

Mass Effect Corresponding to the Onset of Nuclear Deformation in the Region N Approx. 90

NUCLEAR STRUCTURE 162Dy, 154Gd, 156Gd, 158Gd, 160Gd, 164Dy, 152Dy, 154Sm, 152Sm, 149Sm, 150Sm, 150Nd, 144Nd, 146Sm, 148Nd, 148Sm, 146Nd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.12.597
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1964MC01      Bull.Am.Phys.Soc.9, No.1, 20, BC7 (1964)

W.McLatchie, R.C.Barber, R.L.Bishop, H.E.Duckworth, B.G.Hogg, P.Van Rookhuyzen

Change in the Slope of Neutron-Separation-Energy Curves at N = 124

NUCLEAR STRUCTURE 209Bi, 208Pb, 207Pb, 204Pb, 206Pb, 205Tl, 200Hg, 199Hg, 198Hg, 204Hg, 203Tl, 201Hg, 202Hg; measured not abstracted; deduced nuclear properties.


1964MC07      Can.J.Phys. 42, 926 (1964)

W.McLatchie, R.C.Barber, R.L.Bishop, H.E.Duckworth, B.G.Hogg, J.D.Macdougall, P.Van Rookhuyzen

Some New Neutron Separation Energies for Isotopes of Hg, Tl, Pb, and Bi

NUCLEAR STRUCTURE 202Hg, 201Hg, 203Tl, 204Hg, 198Hg, 200Hg, 199Hg, 205Tl, 206Pb, 204Pb, 207Pb, 208Pb, 209Bi; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p64-086
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1964MC11      Phys.Letters 10, 330 (1964)

W.McLatchie, R.C.Barber, H.E.Duckworth, P.Van Rookhuyzen

Direct Determinations of the Sm144-Nd144 and Nd150-Sm150 Energy Differences

NUCLEAR STRUCTURE 144Sm, 144Nd, 150Sm, 150Nd; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90527-X
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1963BA16      Bull.Am.Phys.Soc. 8, No.4, 376, U11 (1963)

R.C.Barber, W.McLatchie, R.L.Bishop, P.Van Rookhuyzen, H.E.Duckworth

Neutron-Separation Energies for Tellurium and the Te123-Sb123, I128-Te128, and I130-Te130 Decay Energies

NUCLEAR STRUCTURE 124Sn, 124Te, 123Te, 126Te, 125Te, 130I, 132Te, 128Te, 128I; measured not abstracted; deduced nuclear properties.


1963BA20      Can.J.Phys. 41, 696 (1963)

R.C.Barber, R.L.Bishop, W.McLatchie, P.Van Rookhuyzen, H.E.Duckworth

Neutron Separation Energies for Zirconium and the Zr96-Nb96 and Nb94-Zr94 Decay Energies

NUCLEAR STRUCTURE 92Zr, 96Zr, 94Zr; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p63-070
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1963BA47      Can.J.Phys. 41, 1482 (1963)

R.C.Barber, W.McLatchie, R.L.Bishop, P.Van Rookhuyzen, H.E.Duckworth

Neutron Separation Energies for Tellurium and the I130, Te130 and Te123, Sb123 Decay Energies

NUCLEAR STRUCTURE 128Te, 130I, 129Te, 130Te, 125Te, 127Te, 126Te, 123Te, 124Te; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p63-147
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1963BI11      Phys.Canada 19, No.3, 53, Abstr. 11.2 (1963)

R.L.Bishop, R.C.Barber, W.McLatchie, P.van Rookhuyzen, H.E.Duckworth

Some Neutron Separation Energies for Cadmium

NUCLEAR STRUCTURE 114Cd, 116Cd, 113Cd, 112Cd; measured not abstracted; deduced nuclear properties.


1963BI12      Can.J.Phys. 41, 1532 (1963)

R.L.Bishop, R.C.Barber, W.McLatchie, J.D.MacDougall, P.Van Rookhuyzen, H.E.Duckworth

Systematics Governing Double Neutron Separation Energies Between the 50 and 82 Neutron Shells

NUCLEAR STRUCTURE 112Cd, 110Cd, 94Mo, 97Mo, 96Mo, 98Mo, 100Mo, 113Cd, 116Cd, 114Cd; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p63-154
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1962BA24      Can.J.Phys. 40, 1496 (1962)

R.C.Barber, R.L.Bishop, L.A.Cambey, W.McLatchie, H.E.Duckworth

Some Atomic Masses and Neutron Separation Energies for Isotopes of Tin and Antimony

NUCLEAR STRUCTURE 120Sn, 124Sn, 121Sb, 121Sn, 122Sn, 122Sb, 123Sb, 123Sn, 119Sn, 118Sn, 116Sn, 117Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1139/p62-158
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Note: The following list of authors and aliases matches the search parameter W.McLatchie: , W.L.MCLATCHIE, W.M.MCLATCHIE, W.T.MCLATCHIE