NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = T.P.Morrison Found 25 matches. 1988JA05 Nucl.Instrum.Methods Phys.Res. A267, 144 (1988) A.N.James, T.P.Morrison, K.L.Ying, K.A.Connell, H.G.Price, J.Simpson Microsecond Mass Separation of Heavy Compound Nucleus Residues using the Daresbury Recoil Separator NUCLEAR REACTIONS 58Ni(76Se, X), E=300 MeV; measured γ(recoil nucleus)-coin; deduced evidence for 130Ce, 130Pr, 130Nd.
doi: 10.1016/0168-9002(88)90638-9
1986EL05 J.Phys.(London) G12, 1059 (1986) A.M.Y.El-Lawindy, J.D.Burrows, P.A.Butler, A.N.James, G.D.Jones, T.P.Morrison, J.Simpson, K.A.Connell, R.Wadsworth, D.L.Watson Gamma-Ray Spectroscopy up to Spin 20 in 232U NUCLEAR REACTIONS 232Th(α, 4n), E=42 MeV; measured γγ-coin, total Eγ, γ-multiplicity. 232U deduced levels, J, π, γ-branching. Ge, bismuth germanate detectors. Cranked shell model.
doi: 10.1088/0305-4616/12/10/014
1986YI01 J.Phys.(London) G12, L211 (1986) K.L.Ying, P.J.Bishop, A.N.James, A.J.Kirwan, D.J.G.Love, T.P.Morrison, P.J.Nolan, D.C.B.Watson, K.A.Connell, A.H.Nelson, J.Simpson Experimental Investigation of the Structure of 124Ce NUCLEAR STRUCTURE 124,126,128,130,138Ce; calculated deformation, potential energy surfaces. NUCLEAR REACTIONS 54Fe(74Se, 2n2p), E=300 MeV; measured Eγ, Iγ, γγ-, γ(residue)-coin. 124Ce deduced transitions, possible level J, π, deformation.
doi: 10.1088/0305-4616/12/9/004
1985BU22 Nucl.Instrum.Methods 239, 221 (1985) P.A.Butler, K.A.Connell, J.D.Burrows, A.M.Y.El-Lawindy, M.W.Guidry, A.N.James, G.D.Jones, C.Lauterbach, T.P.Morrison, J.Simpson The Application of a Multiple Gas Counter Spectrometer to the Study of Heavy Ion Reactions NUCLEAR REACTIONS 163Dy(58Ni, 58Ni'), (58Ni, 59Ni), E=280-304 MeV; measured (particle)γ-coin, s(θ). Multiple gas counter spectrometer.
doi: 10.1016/0168-9002(85)90719-3
1984BU21 ATOMKI Kozlem. 26, 58 (1984) P.A.Butler, D.Burrows, K.Connell, A.El-Lawindy, A.N.James, G.D.Jones, T.P.Morrison, J.Simpson, R.Wadsworth Gamma-Ray Spectroscopy in the Region of Octupole Deformation near Z = 90 NUCLEAR REACTIONS 208Pb(18O, 2nα), (18O, 3n), E=83 MeV; measured γγ-coin. 220Ra, 223Th deduced levels, J, π, band structure, E1 transition characteristics.
1984BU29 J.Phys.(London) G10, 1449 (1984) J.D.Burrows, P.A.Butler, K.A.Connell, A.N.James, G.D.Jones, A.M.Y.El-Lawindy, T.P.Morrison, J.Simpson, R.Wadsworth A Level Scheme for 220Ra NUCLEAR REACTIONS 208Pb(18O, xnyp), E=83 MeV; measured γγ(evaporation residue)-coin. 220Ra deduced levels, γ-branching, J, π, B(λ) ratios. Ge, heavy ion recoil detectors, enriched targets.
doi: 10.1088/0305-4616/10/10/014
1984BU38 Nucl.Instrum.Methods 227, 259 (1984) J.D.Burrows, P.A.Butler, K.A.Connell, G.D.Jones, A.N.James, A.M.Y.El-Lawindy, T.P.Morrison, J.Simpson, R.Wadsworth Application of a Compound Nucleus Residue Detector NUCLEAR REACTIONS 208Pb(18O, 3n), E=83, 85 MeV; 208Pb(18O, 4n), E=95 MeV; measured Eγ, Iγ, γ(evaporation residue)-coin. Gas filled avalanche detector.
doi: 10.1016/0168-9002(84)90131-1
1983DA12 J.Phys.(London) G9, 947 (1983) R.Daniel, J.D.Burrows, P.A.Butler, J.R.Cresswell, A.D.Irving, D.J.G.Love, T.P.Morrison, P.J.Nolan, J.F.Sharpey-Schafer The Measurement of Entry States in Light Nuclei NUCLEAR REACTIONS 28Si(16O, 2p), (16O, αp), 32S(16O, 2p), (16O, 3p), (16O, n2p), (16O, pα), (16O, 2pα), E=40 MeV; 58Ni(16O, 2p), (16O, 3p), (16O, pα), (16O, 2pα), E=55 MeV; measured (particle)γ-, γγ(particle)-coin, γ-multipilicity, total Ep; deduced relative σ. 46Ti, 72Se deduced moments of inertia.
doi: 10.1088/0305-4616/9/8/017
1981EK01 J.Phys.(London) G7, 85 (1981) L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, A.Nilsson, V.Paar, P.J.Twin, R.Wadsworth, E.Wallander, N.J.Ward Gamma-Ray Spectroscopy on 87Sr and the Energy-B(E2) Rule NUCLEAR REACTIONS 84Kr(α, nγ), E=11-17 MeV; measured γ(θ), γγ-coin, linear polarizations, DSA, σ(Eγ). 87Sr deduced levels, J, π, δ, T1/2, B(λ). Enriched target, Ge(Li) detectors. Generalized vibrator model.
doi: 10.1088/0305-4616/7/1/013
1981WA09 J.Phys.(London) G7, 815 (1981) N.J.Ward, L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, O.M.Mustaffa, D.N.Simister, P.J.Twin, R.Wadsworth Gamma-ray Studies of 62Zn NUCLEAR REACTIONS 58Ni(6Li, np), E=15-24 MeV; measured Eγ, Iγ, γγ-coin, γ(θ), linear polarization, DSA, recoil. 62Zn deduced levels, J, π, δ, T1/2, γ-branching. Enriched target, Ge(Li) detectors. Shell model, interacting boson approximation model.
doi: 10.1088/0305-4616/7/6/014
1981WA10 Nucl.Phys. A361, 387 (1981) E.Wallander, A.Nilsson, L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, H.G.Price, P.J.Twin, R.Wadsworth, N.J.Ward States in 89Sr Excited by the 86Kr(α, n)89Sr Reaction NUCLEAR REACTIONS 86Kr(α, nγ), E=12-16 MeV; measured Eγ, Iγ(E), Iγ(θγ), γγ-coin, linear polarization, DSA. 89Sr deduced levels, J, π, δ, T1/2, B(λ). Enriched solid 86Kr targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(81)90641-2
1980BU13 J.Phys.(London) G6, 1165 (1980) P.A.Butler, R.Daniel, A.D.Irving, T.P.Morrison, P.J.Nolan, V.Metag Experimental Upper Limit for a γ Branch from the 236U Shape Isomer NUCLEAR REACTIONS 235U(d, p), E=11 MeV; measured σ(Eγ), γp(t). 236U level deduced limit on Γγ/ΓF.
doi: 10.1088/0305-4616/6/9/012
1980EK03 J.Phys.(London) G6, 1415 (1980) L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, A.Nilsson, P.J.Twin, R.Wadsworth, E.Wallander, N.J.Ward Lifetime and Linear Polarization Measurements with the 80Kr(α, nγ)83Sr and 82Kr(α, nγ)85Sr Reactions NUCLEAR REACTIONS 80Kr(α, nγ), 82Kr(α, 2nγ), 82Kr(α, nγ), E=14, 18 MeV; measured γ(θ), linear polarizations, DSA. 83,84,85Sr levels deduced J, π, δ, T1/2, transitions rates. Enriched solid 80,82Kr targets, Ge(Li)detectors.
doi: 10.1088/0305-4616/6/11/013
1980JO11 Nucl.Instrum.Methods 178, 581 (1980) G.D.Jones, L.P.Ekstrom, F.Kearns, T.P.Morrison, P.J.Twin, R.Wadsworth, N.J.Ward, B.Collinge, C.L.Wilkinson An On-Line Computer Controlled Time Digitizer for Half-Life Measurements NUCLEAR REACTIONS 74Ge(d, n), E=7 MeV; measured γγ-coin. 75As level deduced T1/2. On-line computerized digitizer. RADIOACTIVITY 38K(IT) [from 24Mg(16O, np), E=38 MeV]; 24Na(IT) [from 23Na(d, p), E=4 MeV]; 77Se(IT) [from 74Ge(α, n), E=16 MeV]; 71Ge(EC) [from 70Ge(d, p), E=6 MeV]; 73As(EC), 77As(β-) [from 72,76Ge(d, n), E=6, 7 MeV]; measured T1/2. On-line computerized digitizer.
doi: 10.1016/0029-554X(80)90841-1
1980KE06 J.Phys.(London) G6, 1131 (1980) F.Kearns, L.P.Ekstrom, G.D.Jones, T.P.Morrison, O.M.Mustaffa, H.G.Price, D.N.Simister, P.J.Twin, R.Wadsworth, N.J.Ward Heavy-Ion Gamma-Ray Spectroscopy of 60Ni NUCLEAR REACTIONS 56Fe(7Li, 2npγ), E=14-24 MeV; measured nγ-, γγ-coin, γ(θ), linear polarization, DSA, recoil. 60Ni deduced levels J, π, δ, T1/2, transition rates. Enriched target, Ge(Li), neutron scintillation detectors.
doi: 10.1088/0305-4616/6/9/010
1980SI02 J.Phys.(London) G6, 81 (1980) D.N.Simister, L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, O.M.Mustaffa, H.G.Price, P.J.Twin, R.Wadsworth, N.J.Ward Gamma-Ray Studies in 64Zn: Levels Above 3.1 MeV NUCLEAR REACTIONS 61Ni(α, nγ), E=8.6, 9.35 MeV; 56Fe(11B, 2npγ), E=30 MeV; measured γγ-, nγ-coin, Eγ, Iγ(θ), DSA, linear polarization. 64Zn deduced levels, J, π, δ, T1/2, γ-branching. Shell model, cluster vibration, interacting boson models. Ge(Li) detectors, enriched targets.
doi: 10.1088/0305-4616/6/1/015
1980WA19 J.Phys.(London) G6, 1403 (1980) R.Wadsworth, L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, P.J.Twin, N.J.Ward Gamma-Ray Studies on the Neutron-Deficient Isotope 70Se NUCLEAR REACTIONS 58Ni(14N, pnγ), E=36 MeV; 60Ni(12C, 2nγ), E=34 MeV; measured nγ-, γγ-coin, γ(θ), linear polarizations. 70Se levels deduced J, π, δ, γ-branchings. Enriched targets, Ge(Li)detectors.
doi: 10.1088/0305-4616/6/11/012
1979EK03 J.Phys.(London) G5, 803 (1979) L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, O.M.Mustaffa, D.N.Simister, H.G.Price, P.J.Twin, R.Wadsworth, N.J.Ward Gamma-Ray Spectroscopy on 48Cr NUCLEAR REACTIONS 36Ar(14N, npγ), E=28-36 MeV; 40Ca(10B, npγ), E=24 MeV; measured γγ-coin, γ(θ), linear polarizations, DSA, RDM. 48Cr deduced levels, J, π, δ, T1/2, transition rates. Enriched 36Ar target. Shell model intepretation.
doi: 10.1088/0305-4616/5/6/008
1979MO22 J.Phys.(London) G5, 1751 (1979) T.P.Morrison, G.D.Jones, L.P.Ekstrom, F.Kearns, A.Kogan, P.R.G.Lornie, O.Mustaffa, H.G.Price, D.N.Simister, P.J.Twin, R.Wadsworth Coulomb-Nuclear Interference in the (7Li, 7Li) Reactions NUCLEAR REACTIONS 46,48Ti(7Li, 7Li'), E=17 MeV; 58Ni(7Li, 7Li'), E=19 MeV; measured σ(θ); deduced optical potentials. DWBA analyses.
doi: 10.1088/0305-4616/5/12/014
1979MU08 J.Phys.(London) G5, 1283 (1979); see 79Mu09 O.M.Mustaffa, L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, H.G.Price, D.N.Simister, P.J.Twin, R.Wadsworth, N.J.Ward Gamma-Ray Spectroscopy in 63Zn and 63Cu
doi: 10.1088/0305-4616/5/9/012
1979MU09 J.Phys.(London) G5, 1283 (1979) O.M.Mustaffa, L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, H.G.Price, D.N.Simister, P.J.Twin, R.Wadsworth, N.J.Ward Gamma-Ray Spectroscopy in 63Zn and 63Cu NUCLEAR REACTIONS 60Ni(α, nγ), (α, pγ), E=9.5-19.0 MeV; 54Fe(11B, npγ), (11B, 2pγ), E=30 MeV; 58Ni(7Li, npγ), E=20 MeV; measured γγ-coin, Iγ(θ), linear polarizations, RDM, DSA. 63Zn, 63Cu levels deduced J, π, δ, T1/2, γ-branching ratios. Enriched targets, Ge(Li) detectors. Shell-model calculations.
doi: 10.1088/0305-4616/5/9/012
1979WA23 J.Phys.(London) G5, 1761 (1979) R.Wadsworth, L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, O.M.Mustaffa, H.G.Price, P.J.Twin, N.J.Ward A Study of the Neutron-Deficient Isotope 66Ge NUCLEAR REACTIONS 58Ni(10B, np), E=28.5, 29, 30 MeV; measured nγ-, γγ-coin, Iγ(θ), linear polarizations, RDM. 66Ge levels deduced J, π, δ, T1/2, γ-branchings. Enriched targets.
doi: 10.1088/0305-4616/5/12/015
1978MU02 J.Phys.(London) G4, 99 (1978) O.M.Mustaffa, A.Kogan, G.D.Jones, P.R.G.Lornie, T.P.Morrison, H.G.Price, D.N.Simister, P.J.Twin, R.Wadsworth Nuclear Spectroscopy in 63Zn: States below 1.5 MeV NUCLEAR REACTIONS 60Ni(α, nγ), E=8-16 MeV; measured Eγ, Iγ(E, θ), γγ-coin, linear polarization, DSA. 63Zn levels deduced T1/2, J, π, λ, δ, γ-branching. Enriched target, Ge(Li) detectors.
doi: 10.1088/0305-4616/4/1/011
1978SI02 J.Phys.(London) G4, 111 (1978) D.N.Simister, G.D.Jones, A.Kogan, P.R.G.Lornie, T.P.Morrison, O.M.Mustaffa, H.G.Price, P.J.Twin, R.Wadsworth Gamma Ray Spectroscopy in 64Zn-Levels below 3.1 MeV in Excitation NUCLEAR REACTIONS 61Ni(α, nγ), E=7.8 MeV; measured Eγ, Iγ(θ), linear polarization, DSA. 64Zn deduced levels, J, π, T1/2, λ, δ. Enriched targets, Ge(Li) detectors.
doi: 10.1088/0305-4616/4/1/012
1978SI10 J.Phys.(London) G4, 1127 (1978) D.N.Simister, G.D.Jones, F.Kearns, A.Kogan, P.R.G.Lornie, T.P.Morrison, O.M.Mustaffa, H.G.Price, P.J.Twin, R.Wadsworth Quasi-Band Structure in 64Zn NUCLEAR REACTIONS 61Ni(α, nγ), E=9.35 MeV; 56Fe(11B, 2npγ), E=30 MeV; measured γ(θ), DSA, linear polarization, σ(Eγ). 64Zn deduced levels, J, π, T1/2, γ-branching, B(λ). Enriched targets, Ge(Li) detectors. Shell model.
doi: 10.1088/0305-4616/4/7/017
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