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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
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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 T_1/2, 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 T_1/2. 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
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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 T_1/2, B(λ), δ, γ-branching ratio, quadrupole moment, g(k), g(R).

doi: 10.1016/0375-9474(81)90492-9
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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 T_1/2. 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
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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 T_1/2, 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 T_1/2. 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
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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
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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
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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, T_1/2, 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, T_1/2, 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 T_1/2.

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
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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
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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
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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 T_1/2. 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
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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
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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
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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
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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 ^{142,144,146,148,150}Nd(t, p), E=13 MeV; measured σ(Ep, θ), Q. ^{144,146,148,150,152}Nd deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(72)90986-4
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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 ^{83,84,85,86,87}Sr; 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, ^{142,143,144,145,146,148,150}Nd, ^{147,148,149,150,152,154}Sm, ^151,153Eu, ^{154,155,156,157,158,160}Gd; 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 ^{182,183,184,186}W, ^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 ^{161,162,163,164}Dy, ¹⁶⁵Ho, ^{166,167,168,170}Er, ¹⁶⁹Tm, ^{171,172,173,174,176}Yb, ¹⁷⁵Lu, ^{176,177,178,179,180}Hf; 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