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NSR database version of April 11, 2024.

Search: Author = G.C.Morrison

Found 78 matches.

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1990ZY01      Nucl.Phys. A510, 441 (1990)

L.Zybert, J.B.A.England, G.M.Field, O.Karban, R.Zybert, M.Becha, C.N.Pinder, G.C.Morrison, M.Bentley, P.Fallon, R.Moktah, J.W.Roberts, J.F.Sharpey-Schafer

Deep Proton-Hole States in 147Pr, 151Pm and 155Eu

NUCLEAR REACTIONS 148Nd(t, α), E=35.32, 37.32 MeV; 152Sm(t, α), 156Gd(t, α), E=35.32 MeV; measured σ(θ). 147Pr, 151Pm, 155Eu deduced relative nuclear structure factors, g7/2-g9/2 hole strength distributions. Enriched targets. Calculated deformed Woods-Saxon proton single particle levels.

doi: 10.1016/0375-9474(90)90061-P
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0088.


1988BA45      Nucl.Phys. A485, 161 (1988)

D.Barker, J.M.Nelson, D.W.Banes, B.R.Fulton, S.D.Hoath, M.C.Mannion, G.C.Morrison, C.A.Ogilvie, L.Zybert, R.Zybert

A Study of Proton Pairing Vibrations in the fp-Shell using 14C-Induced Two-Proton Pickup Reactions

NUCLEAR REACTIONS 50Ti, 52Cr, 54Fe(14C, 16O), E=113 MeV; 52Cr(14C, 16O), E=130 MeV; measured σ(E(16O), θ). 48Ca, 50Ti, 52Cr deduced spectroscopic strength. Enriched targets. DWBA calculations.

doi: 10.1016/0375-9474(88)90527-1
Citations: PlumX Metrics


1988SO07      Phys.Rev. C38, 654 (1988)

D.I.Sober, L.W.Fagg, B.Zeidman, R.D.Lawson, D.F.Geesaman, G.C.Morrison, O.Karban, X.K.Maruyama, H.de Vries, E.A.J.M.Offermann, C.W.de Jager, R.A.Lindgren, J.F.A.van Hienen

Electroexcitation of 8- States in 52Cr

NUCLEAR REACTIONS 52Cr(e, e'), E=170-260 MeV; measured σ(E(e')), θ=115°, 154°. 52Cr deduced B(M8), total T=2, T=3 strengths, sums for M8 transitions. Shell model.

doi: 10.1103/PhysRevC.38.654
Citations: PlumX Metrics


1988ZE01      Phys.Rev. C38, 2251 (1988)

B.Zeidman, D.F.Geesaman, P.Zupranski, R.E.Segel, G.C.Morrison, C.Olmer, G.R.Burleson, S.J.Greene, R.L.Boudrie, C.L.Morris, L.W.Swenson, G.S.Blanpied, B.G.Ritchie, C.L.H.Johnstone

Inelastic Scattering of Pions by 10B

NUCLEAR REACTIONS 10B(π+, π+), (π+, π+'), E=162 MeV; measured σ(θ). 10B deduced levels, J, π, stretched configurations, B(λ).

doi: 10.1103/PhysRevC.38.2251
Citations: PlumX Metrics


1987EN06      Nucl.Phys. A475, 422 (1987)

J.B.A.England, L.Zybert, G.T.A.Squier, O.Karban, R.Zybert, J.M.Nelson, D.Barker, B.R.Fulton, M.C.Mannion, C.A.Ogilvie, L.Potvin, C.Pinder, C.O.Blyth, G.C.Morrison, G.J.Pyle, S.Roman, N.M.Clarke, K.I.Pearce, P.J.Simmonds, R.J.Griffiths, D.L.Watson, M.D.Cohler, R.Wadsworth, J.O'Donnell, M.Smithson

Elastic Scattering of 33 MeV Tritons and Isospin Dependence of Mass-3 Optical Potential

NUCLEAR REACTIONS 12C, 16O, 19F, 24Mg, 40,48Ca, 51V, 58Ni, 89Y, 208Pb, 232Th(t, t), E=33 MeV; measured σ(θ); deduced optical-model parameters, isospin dependence.

doi: 10.1016/0375-9474(87)90072-8
Citations: PlumX Metrics

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1986DR03      Nucl.Phys. A448, 93 (1986)

P.V.Drumm, O.Karban, A.K.Basak, P.M.Lewis, S.Roman, G.C.Morrison

Study of 14N by One-Nucleon Transfer Reactions Induced with Polarised 3He

NUCLEAR REACTIONS 13C, 15N(polarized 3He, 3He), 13C(polarized 3He, d), 15N(polarized 3He, α), E=33 MeV; measured σ(θ), A(θ); deduced optical-model parameters. 14N levels deduced j-transfer values, S(lj).

doi: 10.1016/0375-9474(86)90182-X
Citations: PlumX Metrics

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1985HO10      Phys.Lett. 154B, 33 (1985)

S.D.Hoath, G.C.Morrison, J.M.Nelson, P.Videbaek, P.D.Bond, O.Hansen, M.J.Levine, C.E.Thorn, W.Trautmann

Spectroscopy of the Heavy Ion Transfer Reaction 48Ca(28Si, 27Al)49Sc

NUCLEAR REACTIONS 48Ca(28Si, 27Al), E=180 MeV; measured σ(θ), σ(E(27Al)); deduced optical model parameters. 27Al, 49Sc deduced levels, S. Finite-range DWBA, recoil.

doi: 10.1016/0370-2693(85)91562-X
Citations: PlumX Metrics


1984DE33      Nucl.Phys. A426, 399 (1984)

P.Dessagne, M.Bernas, M.Langevin, G.C.Morrison, J.Payet, F.Pougheon, P.Roussel

The Complex Transfer Reaction (14C, 15O) on Ni, Zn and Ge Targets: Existence and mass of 69Ni

NUCLEAR REACTIONS 58,60,62,64Ni, 68,70Zn, 74,76Ge(14C, 15O), E=72 MeV; measured σ(E(15O)), σ(θ), reaction σ. 61Fe, 67,69Ni, 73,75Zn deduced mass excess.

doi: 10.1016/0375-9474(84)90114-3
Citations: PlumX Metrics


1984GE06      Phys.Rev. C30, 952 (1984)

D.F.Geesaman, R.D.Lawson, B.Zeidman, G.C.Morrison, A.D.Bacher, C.Olmer, G.R.Burleson, W.B.Cottingame, S.J.Greene, R.L.Boudrie, C.L.Morris, R.A.Lindgren, W.H.Kelly, R.E.Segel, L.W.Swenson

Quenching of Isoscalar Spin-Flip Strength in 54Fe

NUCLEAR REACTIONS 54Fe(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ), σ(E(π)). 54Fe levels deduced isoscalar, isovector strengths.

doi: 10.1103/PhysRevC.30.952
Citations: PlumX Metrics


1983GE03      Phys.Rev. C27, 1134 (1983)

D.F.Geesaman, D.Kurath, G.C.Morrison, C.Olmer, B.Zeidman, R.E.Anderson, R.L.Boudrie, H.A.Thiessen, G.S.Blanpied, G.R.Burleson, R.E.Segal, L.W.Swenson

Inelastic Scattering of 162-MeV Pions by 14N

NUCLEAR REACTIONS 14N(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=162 MeV; measured σ(θ), σ(E(π)). 14N levels deduced B(λ). DWIA analysis, shell model wave functions.

doi: 10.1103/PhysRevC.27.1134
Citations: PlumX Metrics


1981BA37      Nucl.Phys. A368, 74 (1981)

A.K.Basak, O.Karban, S.Roman, G.C.Morrison, C.O.Blyth, J.M.Nelson

Scattering and Charge-Exchange Reactions with Polarized 3He on Lithium Isotopes

NUCLEAR REACTIONS 6,7Li(polarized 3He, 3He), (polarized 3He, 3He'), (polarized 3He, t), E=33.3 MeV; measured σ(θ), A(θ); deduced optical-model parameters, reaction mechanism. Enriched 6Li target.

doi: 10.1016/0375-9474(81)90731-4
Citations: PlumX Metrics


1981BA38      Nucl.Phys. A368, 93 (1981)

A.K.Basak, O.Karban, S.Roman, G.C.Morrison, C.O.Blyth, J.M.Nelson

Polarization Effects in 3He Induced Transfer Reactions on Lithium Isotopes

NUCLEAR REACTIONS 6,7Li(polarized 3He, d), (polarized 3He, α), E=33.3 MeV; measured σ(θ), A(θ). 7,8Be, 5,6Li levels deduced S. Enriched 6Li target. DWBA, coupled-channels analyses.

doi: 10.1016/0375-9474(81)90732-6
Citations: PlumX Metrics


1981BH02      Nucl.Phys. A363, 516 (1981)

R.K.Bhowmik, E.C.Pollacco, J.B.A.England, G.C.Morrison, N.E.Sanderson

Emission of α-Particles in Deep Inelastic Reactions Induced by 148 MeV 14N

NUCLEAR REACTIONS 12C, 27Al, 58Ni(14N, X), E=148 MeV; measured σ(fragment E, θ), fragment mass = 2-8; 12C, 27Al, 58Ni(14N, αX), E=148 MeV; measured absolute σ(E(X), θ(X), Eα, θα), αX-coin; deduced reaction mechanisms. Enriched 58Ni target.

doi: 10.1016/0375-9474(81)90271-2
Citations: PlumX Metrics


1980MO28      J.Phys.(Paris), Colloq.C-10, 243 (1980)

G.C.Morrison, R.K.Bhowmik, E.C.Pollacco, J.B.A.England, N.E.Sanderson

Alpha Emission with 10 MeV/A 14N Projectiles

NUCLEAR REACTIONS 58Ni, 27Al, 12C(14N, αX), E=148 MeV; measured σ(fragment E, θ), σ(θα, Eα), σ(Eα, θα, fragment E, θ), αX-coin, αX(θ); deduced direct mechanism for α-decay followed by deep inelastic collision.


1979BH06      Phys.Rev.Lett. 43, 619 (1979)

R.K.Bhowmik, E.C.Pollacco, N.E.Sanderson, J.B.A.England, G.C.Morrison

Pre-Emission of α Particles in Deep-Inelastic Reactions

NUCLEAR REACTIONS 58Ni(14N, 2α), (14N, αX), E=148 MeV; measured σ(Eα, E(HI), θ) for X=Li, Be, B, C, N; deduced reaction mechanism. Thick target.

doi: 10.1103/PhysRevLett.43.619
Citations: PlumX Metrics


1979FU01      Nucl.Phys. A315, 477 (1979)

B.R.Fulton, N.E.Sanderson, R.Ost, B.A.England, G.C.Morrison

Transfer Reactions and Scattering Induced by 13C on 52Cr

NUCLEAR REACTIONS 52Cr(13C, 13C'), (13C, 12B), (13C, 14C), (13C, 14N), E=105 MeV; measured σ(θ). 51V, 51Cr, 53Mn levels deduced S. Optical model, DWBA analyses. Enriched target.

doi: 10.1016/0375-9474(79)90624-9
Citations: PlumX Metrics


1978BH03      Phys.Lett. 80B, 41 (1978)

R.K.Bhowmik, E.C.Pollacco, N.E.Sanderson, J.B.A.England, G.C.Morrison

A Study of Heavy-Ion-Alpha Correlations with 11B Projectiles

NUCLEAR REACTIONS 12C(11B, αX), 58Ni(11B, αX), E=116 MeV; measured X-α(θ), differential α-multiplicities.

doi: 10.1016/0370-2693(78)90301-5
Citations: PlumX Metrics


1977FU03      Nucl.Phys. A284, 329 (1977)

H.W.Fulbright, C.L.Bennett, R.A.Lindgren, R.G.Markham, S.C.McGuire, G.C.Morrison, U.Strohbusch, J.Toke

Four-Nucleon Transfer via the (6Li, d) Reaction

NUCLEAR REACTIONS 40,42,44,48Ca, 50Ti, 50,52,54Cr, 54,56Fe, 58,60,62Ni, 90Zr(6Li, d), E=28-38 MeV; measured σ(Ed, θ). 44Ti, 54,58,56Fe, 58,60Ni, 62,64,66Zn deduced levels, Sα, L, J, π. DWBA analysis.

doi: 10.1016/0375-9474(77)90127-0
Citations: PlumX Metrics


1977RO12      Nucl.Phys. A284, 365 (1977)

S.Roman, A.K.Basak, J.B.A.England, O.Karban, G.C.Morrison, J.M.Nelson

Polarization Effects in the Elastic Scattering of 3He and (3He, d) Reaction on 58Ni

NUCLEAR REACTIONS 58Ni(polarized 3He, 3He), 58Ni(polarized 3He, d), E=33.3 MeV; measured A(θ). Enriched target.

doi: 10.1016/0375-9474(77)90390-6
Citations: PlumX Metrics


1976KA23      Nucl.Phys. A269, 312 (1976)

O.Karban, A.K.Basak, J.B.A.England, G.C.Morrison, J.M.Nelson, S.Roman, G.G.Shute

The j-Dependence of (3He, d) and (3He, α) Reaction Analysing Powers in the 1p Shell

NUCLEAR REACTIONS 9Be, 12C(polarized 3He, d), (polarized 3He, α), E=33.3 MeV; measured σ(θ), A(θ); deduced J-dependence. 10B, 8Be, 13N, 11C levels deduced S.

doi: 10.1016/0375-9474(76)90683-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetR0022.


1976OS04      Nucl.Phys. A265, 142 (1976)

R.Ost, N.E.Sanderson, S.Mordechai, J.B.A.England, B.R.Fulton, J.M.Nelson, G.C.Morrison

Do Many-Particle Reactions Contribute to 'Deep-Inelastic' Peaks (Question)

NUCLEAR REACTIONS 60Ni(13C, X), E=105 MeV; measured σ(E(Z), θ), Z=3-8. 58,64Ni(13C, X), E=105 MeV; measured σ(E(Z), θ), Z=3-8, light particle coin for Li, B, Be, α, p; deduced reaction mechanism. Enriched targets.

doi: 10.1016/0375-9474(76)90120-2
Citations: PlumX Metrics


1975FU02      Phys.Lett. 53B, 449 (1975)

H.W.Fulbright, U.Strohbusch, R.G.Markham, R.A.Lindgren, G.C.Morrison, S.C.McGuire, C.L.Bennett

(6Li, d) Spectroscopy in the f-p Shell

NUCLEAR REACTIONS 40,42,44,48Ca, 50Ti, 52Cr, 54,56Fe, 58,60,62Ni, 90Zr(6Li, d), E=28, 32 MeV; measured σ(Ed, θ). 58Ni levels deduced J.

doi: 10.1016/0370-2693(75)90215-4
Citations: PlumX Metrics


1974CO37      Phys.Rev. C10, 2399 (1974)

J.R.Comfort, H.T.Fortune, G.C.Morrison, J.V.Maher

92,98Mo(d, α)90,96Nb Reactions and Particle-Hole Multiplets

NUCLEAR REACTIONS 92,98Mo(d, α), E=17 MeV; measured σ(Eα, θ). 90,96Nb deduced levels, J, π, L.

doi: 10.1103/PhysRevC.10.2399
Citations: PlumX Metrics


1974ZE01      Phys.Rev. C9, 409 (1974)

B.Zeidman, R.H.Siemssen, G.C.Morrison, L.L.Lee, Jr.

Zn(3He, d) Reactions at 18 MeV

NUCLEAR REACTIONS 64,66,68,70Zn(3He, d), E=18 MeV; measured σ(Ed, θ). 65,67,69,71Ga deduced levels, L, S.

doi: 10.1103/PhysRevC.9.409
Citations: PlumX Metrics


1973KO01      Phys.Rev. C7, 107 (1973)

H.J.Korner, G.C.Morrison, L.R.Greenwood, R.H.Siemssen

16O-Induced Transfer Reactions on fp-Shell Target Nuclei. I. The (16O, 15N) One-Proton Transfer Reaction

NUCLEAR REACTIONS 40,42,44,46,48Ca, 46,50Ti, 52,54Cr, 54,56,58Fe, 62,64Ni, 68,70Zn(16O, 15N), E=42, 48, 56 MeV; measured σ(θ); deduced J-dependence.

doi: 10.1103/PhysRevC.7.107
Citations: PlumX Metrics


1972BR25      Phys.Rev.Lett. 29, 295 (1972)

G.Bruge, A.Chameaux, R.Devries, G.C.Morrison

58Ni(α, α')58Ni and the Nature of High-Lying States in 58Ni

NUCLEAR REACTIONS 58Ni(α, α'), E=30 MeV; measured σ(Eα', θ). 58Ni deduced level, J, π, β(L).

doi: 10.1103/PhysRevLett.29.295
Citations: PlumX Metrics


1972FO11      Phys.Rev. C6, 21 (1972)

H.T.Fortune, G.C.Morrison, R.C.Bearse, J.L.Yntema, B.H.Wildenthal

19F(d, p)20F and the Nuclear Structure of 20F

NUCLEAR REACTIONS 19F(d, p), E=16 MeV; measured σ(Ep, θ). 20F deduced levels, J, π, S.

doi: 10.1103/PhysRevC.6.21
Citations: PlumX Metrics


1972MA13      Phys.Rev. C5, 1313 (1972)

J.V.Maher, H.T.Fortune, G.C.Morrison, B.Zeidman

Reaction 27Al(d, p)28Al at E = 23 MeV

NUCLEAR REACTIONS 27Al(d, p), E=23 MeV; measured σ(Ep, θ). 28Al deduced levels, J, π, S.

doi: 10.1103/PhysRevC.5.1313
Citations: PlumX Metrics


1972MO14      Phys.Rev.Lett. 28, 1662 (1972)

G.C.Morrison, H.J.Korner, L.R.Greenwood, R.H.Siemssen

(16O, 15N) Reactions on fp-Shell Target Nuclei

NUCLEAR REACTIONS 48Ca, 58Fe, 64Ni(16O, 15N), E=42, 48, 56 MeV; Ca(16O, 15N)41Sc/43Sc/45Sc/47Sc/49Sc/49Sc, E=48 MeV; measured σ(θ).

doi: 10.1103/PhysRevLett.28.1662
Citations: PlumX Metrics


1972ST19      Phys.Rev.Lett. 28, 47 (1972)

U.Strohbusch, H.J.Korner, G.C.Morrison, J.P.Schiffer

Reactions to Unbound Final States

NUCLEAR REACTIONS 116Sn(3He, d); measured σ(Ed, θ). 117Sb deduced analog state transition.

doi: 10.1103/PhysRevLett.28.47
Citations: PlumX Metrics


1972ZE03      Priv.Comm. (1972)

B.Zeidman, R.H.Siemssen, L.L.Lee, G.C.Morrison


1971FO01      Phys.Rev. C3, 337 (1971)

H.T.Fortune, G.C.Morrison, J.A.Nolen, Jr., P.Kienle

Ru103,105 States Observed in the Reactions Ru102,104(d, p)

NUCLEAR REACTIONS 102,104Ru(d, p), E=14 MeV; measured σ(Ep, θ). 103,105Ru deduced levels, J, π, L(n), S.

doi: 10.1103/PhysRevC.3.337
Citations: PlumX Metrics


1971FO08      Phys.Rev. C3, 2133 (1971)

H.T.Fortune, G.C.Morrison, R.H.Siemssen

6Li + 6Li Scattering at E(c.m.) = 5-17 MeV

NUCLEAR REACTIONS 6Li(6Li, 6Li), E=5-17 MeV; measured σ(E;θ).

doi: 10.1103/PhysRevC.3.2133
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1971MA11      Phys.Rev. C3, 1162 (1971)

J.V.Maher, J.R.Comfort, G.C.Morrison

87Y States Populated by Single-Proton Stripping

NUCLEAR REACTIONS 86Sr(3He, d), E=20 MeV; measured σ(Ed, θ), Q 87Y deduced levels, L(p), S .

doi: 10.1103/PhysRevC.3.1162
Citations: PlumX Metrics


1971TH02      Phys.Rev. C3, 536 (1971)

M.J.Throop, D.H.Youngblood, G.C.Morrison

Lifetime of the 981-keV State in Li8

NUCLEAR REACTIONS 2H(7Li, pγ), E=7.4 MeV; measured Doppler shift attenuation. 8Li level deduced T1/2.

doi: 10.1103/PhysRevC.3.536
Citations: PlumX Metrics


1970BE12      Phys.Rev. C1, 608 (1970)

R.C.Bearse, J.C.Legg, G.C.Morrison, R.E.Segel

Study of the Low-Lying T = 3/2 States in Na21

NUCLEAR REACTIONS 20Ne(p, γ), E=6.85-7.22 MeV; measured σ(E;Eγ). 21Na deduced resonances, J, π, level-width, K, branching ratios.

doi: 10.1103/PhysRevC.1.608
Citations: PlumX Metrics


1970CO19      Phys.Rev.Lett. 25, 383 (1970)

J.R.Comfort, J.V.Maher, G.C.Morrison, J.P.Schiffer

g9/2-d5/2 Interactions in Nb96 and Nb92

NUCLEAR REACTIONS 96Zr(3He, t), E=21 MeV; measured σ(Et, θ). 96Nb deduced levels, J, π.

doi: 10.1103/PhysRevLett.25.383
Citations: PlumX Metrics


1970CO26      Phys.Lett. 32B, 685 (1970)

J.R.Comfort, G.C.Morrison, B.Zeidman, H.T.Fortune

Evidence for a Jπ = 8+ State in 16O

NUCLEAR REACTIONS 12C(6Li, d), E=29 MeV; 12C(7Li, t), E=31.5 MeV; measured σ(Ed, θ), σ(Et, θ). 16O deduced high-spin 4p-4h state.

doi: 10.1016/0370-2693(70)90445-4
Citations: PlumX Metrics


1970VO04      Phys.Rev. C1, 2066 (1970)

D.von Ehrenstein, G.C.Morrison, J.A.Nolen, Jr., N.Williams

Study of the (d, p) Reaction on the Even-A Barium Isotopes 130-138

NUCLEAR REACTIONS 130,132,134,136,138Ba(d, p), E=12 MeV; measured σ(Ep, θ), Q. 131,133,135,137,139Ba deduced levels, L(n), J, π, S.

doi: 10.1103/PhysRevC.1.2066
Citations: PlumX Metrics


1970WI18      Phys.Rev. C2, 1539 (1970)

N.Williams, G.C.Morrison, J.A.Nolen, Jr., Z.Vager, D.von Ehrenstein

Isobaric Analog Resonances from Proton Scattering on the Barium Isotope

NUCLEAR REACTIONS 130,132,134,136,138Ba(p, p), E=7-12 MeV; measured σ(E;θ). 131,133,135,137,139La deduced isobaric analog resonances, level-width, S, Coulomb displacement energies.

doi: 10.1103/PhysRevC.2.1539
Citations: PlumX Metrics


1969JO20      Australian J.Phys. 22, 541 (1969)

G.A.Jones, G.C.Morrison, R.B.Taylor

Analogues of Excited States in 91Zr

NUCLEAR REACTIONS 90Zr(p, p'), E = 6-8 MeV; measured σ(E;Eγ). 91Nb deduced resonances, isobaric analogs, J, π.

doi: 10.1071/PH690541
Citations: PlumX Metrics


1969VO05      Phys.Rev. To Be Published (1969)

D.Von Ehrenstein, J.A.Nolen, Jr., G.C.Morrison, N.Williams


1968LA01      Nucl.Phys. A106, 455 (1968)

B.Lawergren, G.C.Morrison, A.T.G.Ferguson

Excitation of Isobaric Analogue States in the 27Al(d, n)28Si Reaction

NUCLEAR REACTIONS 27Al(d, n), E = 2.980 MeV; measured σ(En, θ). 28Si deduced levels, J, π, T, S for s1/2 transfer.

doi: 10.1016/0375-9474(67)90890-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1198.


1968LA03      Nucl.Phys. A108, 325(1968)

B.T.Lawergren, A.T.G.Ferguson, G.C.Morrison

States with T = 1 in 20Ne, 24Mg and 28Si

NUCLEAR REACTIONS 19F, 23Na(d, n), E = 2.980 MeV; measured σ(En, θ). 20Ne, 24Mg deduced levels, J, π, T, S.

doi: 10.1016/0375-9474(68)90095-X
Citations: PlumX Metrics


1968MO17      Phys.Rev. 174, 1366 (1968)

G.C.Morrison, D.H.Youngblood, R.C.Bearse, R.E.Segel

Gamma Decay of T = 3/2 States in Al25 and P39

NUCLEAR STRUCTURE 29P, 25Al; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.174.1366
Citations: PlumX Metrics


1968NO02      Bull.Am.Phys.Soc. 13, No.4, 584, BF15 (1968)

J.A.Nolen, Jr., H.T.Fortune, P.Kienle, G.C.Morrison

Energy Levels of 103Ru and 105Ru from the 102,104Ru(d, p) Reaction

NUCLEAR STRUCTURE 103Ru, 105Ru; measured not abstracted; deduced nuclear properties.


1968WE04      Nucl.Phys. A108, 547 (1968); Erratum Nucl.Phys. A119, 694 (1968)

A.Weidinger, R.H.Siemssen, G.C.Morrison, B.Zeidman

The Reaction 25Mg(3He, d)26Al at 12 MeV

NUCLEAR REACTIONS 25Mg(3He, d), E = 12 MeV; measured σ(Ed, θ). 26Al deduced L, S. Enriched target.

doi: 10.1016/0375-9474(68)90323-0
Citations: PlumX Metrics


1967BL07      Nucl.Phys. A92, 365(1967)

J.L.Black, M.M.Islam, G.A.Jones, G.C.Morrison, R.B.Taylor

Isobaric Analogues of States in 90Y

NUCLEAR REACTIONS 89Y(p, γ), E = 5-8.5 MeV; 89Y(p, n), 89Y(p, p'), E = 5-6.5 MeV; measured excitation functions. 90Zr deduced isobaric analog states. Natural target.

doi: 10.1016/0375-9474(67)90224-2
Citations: PlumX Metrics


1967BL18      Phys.Rev. 158, 893 (1967)

A.E.Blaugrund, D.H.Youngblood, G.C.Morrison, R.E.Segel

Lifetime of the 1.042-MeV State in 18F

NUCLEAR STRUCTURE 18O, 18F; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.158.893
Citations: PlumX Metrics


1967MO07      Priv.Comm. (June 1967)

G.C.Morrison

NUCLEAR STRUCTURE 59Cu, 65Cu, 62Cu, 61Ni, 63Cu; measured not abstracted; deduced nuclear properties.


1967MO15      Phys.Rev.Letters 19, 592 (1967)

G.C.Morrison, N.Williams, J.A.Nolen, Jr., D.Von Ehrenstein

Structure of Particle-Hole States in Ba138

NUCLEAR STRUCTURE 138Ba; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.19.592
Citations: PlumX Metrics


1967SC29      Phys.Rev. 164, 1274 (1967)

J.P.Schiffer, G.C.Morrison, R.H.Siemssen, B.Zeidman

Study of the (d, p) Reaction in the 1p shell

NUCLEAR STRUCTURE 12B, 12C, 10Be, 9Be, 10B, 8Li, 7Li, 11B, 14C, 13C, 14N, 15N, 6Li; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.164.1274
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1450.


1966MO20      Bull.Am.Phys.Soc. 11, No.3, 366, GA8 (1966)

G.C.Morrison, J.P.Schiffer

Excited States in Cu62 from the Ni61(He3, D) Reaction

NUCLEAR STRUCTURE 62Cu; measured not abstracted; deduced nuclear properties.


1966MO21      Bull.Am.Phys.Soc. 11, No.4, 629, S19 (1966)

G.C.Morrison, J.P.Schiffer

Excitation of Isobaric-Analog States by the (He3, d) Reaction on Ni Isotopic Targets

NUCLEAR STRUCTURE 65Cu, 63Cu, 61Cu, 59Cu; measured not abstracted; deduced nuclear properties.


1966MO22      Proc.Conf.Isobaric Spin in Nucl.Phys., Tallahassee, Florida, J.D.Fox, D.Robson, Eds., Academic Press, New York, p.748 (1966)

G.C.Morrison, J.P.Schiffer

A Study of Isobaric Spin Purity of Analogue States in Cu59

NUCLEAR STRUCTURE 59Cu; measured not abstracted; deduced nuclear properties.


1966SI02      Phys.Rev.Letters 16, 1050 (1966)

R.H.Siemssen, G.C.Morrison, B.Zeidman, H.Fuchs

Discrepancies in Proton-Transfer Reactions to States with Different Isobaric Spin

NUCLEAR STRUCTURE 13C, 14N, 10B, 9Be, 26Al; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.16.1050
Citations: PlumX Metrics


1966YO01      Phys.Letters 22, 625 (1966)

D.H.Youngblood, G.C.Morrison, R.E.Segel

Lowest T = 3/2 State in 29P

NUCLEAR STRUCTURE 29P; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90682-2
Citations: PlumX Metrics


1965AL12      Phys.Letters 17, 56 (1965)

D.L.Allan, G.A.Jones, G.C.Morrison, R.B.Taylor, R.B.Weinberg

Analogues of Excited States in 119Sn

NUCLEAR STRUCTURE 118Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90647-5
Citations: PlumX Metrics


1964JO13      Phys.Lett.11, 329 (1964)

G.A.Jones, A.M.Lane, G.C.Morrison

Cross Sections for Reactions with Analogue State Resonances

NUCLEAR STRUCTURE 90Zr, 89Y; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90350-6
Citations: PlumX Metrics


1963BE20      Proc.Third Conf.on Reactions between Complex Nuclei, Asilomar, Cal., A.Ghiorso, R.M.Diamond, H.E.Conzett, Ed., Univ.of California, p.417 (1963)

R.D.Bent, J.E.Evans, G.C.Morrison, I.J.Van Heerden

Lifetimes of Levels in Ne21

NUCLEAR STRUCTURE 21Ne; measured not abstracted; deduced nuclear properties.


1963BE41      Conf.Low Medium Energy Nucl.Phys., Univ.Manchester, p. 9 (1963)

R.D.Bent, J.E.Evans, G.C.Morrison, I.J.Van Heerden

Lifetimes of Levels in Ne21

NUCLEAR STRUCTURE 21Ne; measured not abstracted; deduced nuclear properties.


1963FE01      Bull.Am.Phys.Soc. 8, No.1, 47, NA2 (1963)

A.T.G.Ferguson, G.C.Morrison, N.Gale, R.E.White

Investigation of Some (d, n) Reactions in Light Nuclei

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


1963HU02      Phys.Rev. 129, 791 (1963)

M.N.Huberman, M.Kamegai, G.C.Morrison

Absolute Cross Sections and Angular Distributions for Charged Particles from Lithium-Lithium Nuclear Reactions

NUCLEAR STRUCTURE 7Li, 6Li; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.129.791
Citations: PlumX Metrics


1963MI02      Bull.Am.Phys.Soc. 8, No.4, 292, A16 (1963)

P.D.Miller, G.C.Morrison, N.Gale, G.Dearnaley

α Particles from the Bombardment of B10 and B11 by Li6 and Li7

NUCLEAR STRUCTURE 11B, 10B, 6Li; measured not abstracted; deduced nuclear properties.


1962FE07      Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 13, 5.4 (September 1962)

A.T.G.Ferguson, N.Gale, P.D.Miller, G.C.Morrison, R.E.White

NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.


1962GA08      R.E.White - Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 14, 5.7 (September 1962)

N.Gale, A.T.G.Ferguson, P.D.Miller, G.C.Morrison

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


1962MO12      Conf.Low Energy Nuclear Phys.Harwell, Aere-R 4131, 13, 5.5 (September 1962)

G.C.Morrison, R.E.White, A.T.G.Ferguson

NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.


1962MO13      Conf.Low Energy Nuclear Phys.Harwell, AERE-R-4131, 14, 5.6 (September 1962)

G.C.Morrison, A.T.G.Ferguson, N.Gale, P.D.Miller, H.Naylor, R.E.White

NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.


1961MO02      Phys.Rev. 121, 182 (1961)

G.C.Morrison

Possibility of a Stripping Mechanism in Transformations Induced by Lithium Ions

NUCLEAR STRUCTURE 10B, 11B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.121.182
Citations: PlumX Metrics


1961MO15      Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.575 (1961)

G.C.Morrison, A.T.G.Ferguson, J.E.Evans

Angular Distributions of the Be9(d, n)B10 Neutrons

NUCLEAR STRUCTURE 9B; measured not abstracted; deduced nuclear properties.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0096.


1960MO15      Proc.Second Conf.On Reactions between Complex Nuclei, Gatlinburg, A.Zucker, E.C.Halbert, F.T.Howard, Eds., John Wiley and Sons, Inc., New York, p.246 (1960)

G.C.Morrison, M.N.Huberman

Nuclear Reaction Products from the Lithium Bombardment of Li7 and Li6 Targets

NUCLEAR STRUCTURE 12B, 9Be, 10B, 11B; measured not abstracted; deduced nuclear properties.


1960MO17      Phys.Rev.Letters 5, 565 (1960)

G.C.Morrison

Cluster Model Interpretation of the Isotopic Spin Selection Rule in Certain Nuclear Reactions

NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.5.565
Citations: PlumX Metrics


1959LI55      Phys.Rev. 116, 1526 (1959)

C.S.Littlejohn, G.C.Morrison

Coulomb Excitation of Nuclei by Li6 and Li7 Projectiles

doi: 10.1103/PhysRev.116.1526
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1959MO04      Phys.Rev.Letters 3, 585 (1959)

G.C.Morrison, J.A.Galey

Excited States of B13

doi: 10.1103/PhysRevLett.3.585
Citations: PlumX Metrics


1959MO12      Phys.Rev. 116, 1583 (1959)

G.C.Morrison, J.A.Galey

Excited States of B13

doi: 10.1103/PhysRev.116.1583
Citations: PlumX Metrics


1959MO97      Bull.Am.Phys.Soc. 4, No.4, 286, X2 (1959)

G.C.Morrison, J.A.Galey

Nuclear Reaction Products from the Lithium Bombardment of Li7 and Li6 Targets


1958FE09      Nuclear Phys. 5, 41 (1958)

A.T.G.Ferguson, G.C.Morrison

The Spectrum of Neutrons from the Reaction p + d Yields p + p + n

doi: 10.1016/0029-5582(58)90007-5
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1957BR27      Phil.Mag. 2, 785 (1957)

G.Brown, G.C.Morrison, H.Muirhead, W.T.Morton

A Study of Protons Emitted from Aluminium, Iron and Rhodium on Bombardment with Neutrons of 13.2 MeV

doi: 10.1080/14786435708241029
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21375.


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