NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = G.C.Morrison Found 78 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
1967MO07 Priv.Comm. (June 1967) 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
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
1966MO20 Bull.Am.Phys.Soc. 11, No.3, 366, GA8 (1966) 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) 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) 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
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
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
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
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
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) 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
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) 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) 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
1959LI55 Phys.Rev. 116, 1526 (1959) Coulomb Excitation of Nuclei by Li6 and Li7 Projectiles
doi: 10.1103/PhysRev.116.1526
1959MO04 Phys.Rev.Letters 3, 585 (1959) Excited States of B13
doi: 10.1103/PhysRevLett.3.585
1959MO12 Phys.Rev. 116, 1583 (1959) Excited States of B13
doi: 10.1103/PhysRev.116.1583
1959MO97 Bull.Am.Phys.Soc. 4, No.4, 286, X2 (1959) Nuclear Reaction Products from the Lithium Bombardment of Li7 and Li6 Targets
1958FE09 Nuclear Phys. 5, 41 (1958) The Spectrum of Neutrons from the Reaction p + d Yields p + p + n
doi: 10.1016/0029-5582(58)90007-5
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
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