NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = D.C.Kean Found 30 matches. 1980SP05 Nucl.Phys. A345, 252 (1980) R.H.Spear, M.T.Esat, M.P.Fewell, D.C.Kean, T.H.Zabel, A.M.Baxter, S.Hinds Static Quadrupole Moments of the First Excited States of 200Hg and 202Hg NUCLEAR REACTIONS 200,202Hg(α, α'), E=13.5-16.5 MeV; 200,202Hg(12C, 12C'), E=40-60 MeV; 202,200Hg(16O, 16O'), E=59-65 MeV; measured Coulomb excitation probabilities. 200,202Hg level deduced B(E2), quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(80)90423-6
1979FE05 Nucl.Phys. A319, 214 (1979) M.P.Fewell, S.Hinds, D.C.Kean, T.H.Zabel Static Quadrupole Moment of the First Excited State of 24Mg NUCLEAR REACTIONS 208Pb(24Mg, 24Mg'), E=80-110 MeV, θ(lab)=90°, 172°; measured Coulomb excitation probability of 24Mg first 2+ state; deduced quadrupole moment, B(E2;0+→2+). Enriched target.
doi: 10.1016/0375-9474(79)90182-9
1979FE06 Nucl.Phys. A321, 457 (1979) M.P.Fewell, A.M.Baxter, D.C.Kean, R.H.Spear, T.H.Zabel Electric Moments of the First Excited State of 18O NUCLEAR REACTIONS 208Pb(18O, 18O'), E=57-86 MeV; measured Coulomb excitation. 18O level deduced quadrupole moment, B(E2). Enriched target.
doi: 10.1016/0375-9474(79)90138-6
1979FE08 Phys.Rev.Lett. 43, 1463 (1979) M.P.Fewell, D.C.Kean, R.H.Spear, T.H.Zabel, A.M.Baxter, S.Hinds Static Quadrupole Moment of the First Excited State of 30Si NUCLEAR REACTIONS 208Pb(30Si, 30Si'), E=106-136 MeV; measured reorientation effect in Coulomb excitation. 30Si level deduced static quadrupole moment.
doi: 10.1103/PhysRevLett.43.1463
1978JO04 Phys.Lett. 72B, 307 (1978) A.M.R.Joye, A.M.Baxter, S.Hinds, D.C.Kean, R.H.Spear Quadrupole Moments of the First Excited States of 204,206Pb NUCLEAR REACTIONS 204,206Pb(α, α'), E=13.8-18.5 MeV; 204,206Pb(12C, 12C'), E=44-60 MeV; 204,206Pb(16O, 16O'), E=59-85 MeV; measured Coulomb excitation. 204,206Pb deduced quadrupole moment, B(E2).
doi: 10.1016/0370-2693(78)90125-9
1978SP08 Aust.J.Phys. 31, 377 (1978) R.H.Spear, T.H.Zabel, A.M.Baxter, M.P.Fewell, S.Hinds, A.M.R.Joye, D.C.Kean Determination of Maximum Safe Bombarding Energies and B(E3) Values in Reorientation Experiments with 204Pb, 206Pb and 208Pb NUCLEAR REACTIONS 204,206Pb(α, α), (α, α'), E=13.8 MeV; 204,206Pb(12C, 12C), (12C, 12C'), E=52 MeV; 204,206,208Pb(16O, 16O), (16O, 16O'), E=60 MeV; measured σ(elastic), σ(inelastic); deduced optimum E-projectile for onset of Coulomb, nuclear interference. 204,206Pb deduced B(E3).
doi: 10.1071/PH780377
1977ES02 Phys.Lett. 72B, 49 (1977) M.T.Esat, D.C.Kean, R.H.Spear, M.P.Fewell, A.M.Baxter The Static Quadrupole Moment of the First Excited State of 198Hg NUCLEAR REACTIONS 198Hg(α, α'γ), E=14.1-18 MeV; 198Hg(12C, 12C'γ), E=43-54 MeV; 198Hg(16O, 16O'γ), E=60-80 MeV; measured Coulomb excitation reorientation effect. 198Hg level deduced quadrupole moment, B(E2).
doi: 10.1016/0370-2693(77)90060-0
1977FE04 J.Phys.(London) G3, L27 (1977) M.P.Fewell, D.C.Kean, R.H.Spear, A.M.Baxter The Quadrupole Moment of the First Excited State of 18O NUCLEAR REACTIONS 208Pb(18O, 18O'), E=57-72 MeV; measured Coulomb excitation reorientation effect. 18O level deduced quadrupole moment.
doi: 10.1088/0305-4616/3/2/003
1977JO04 Phys.Rev.Lett. 38, 807 (1977) A.M.R.Joye, A.M.Baxter, M.P.Fewell, D.C.Kean, R.H.Spear Quadrupole Moment of the First 3- State in 208Pb NUCLEAR REACTIONS 208Pb(16O, 16O'), E=59-64 MeV; 208Pb(α, α'), E=15.3 MeV; measured Coulomb excitation. 208Pb level deduced quadrupole moment, B(E3).
doi: 10.1103/PhysRevLett.38.807
1977SP05 Aust.J.Phys. 30, 133 (1977) R.H.Spear, J.P.Warner, A.M.Baxter, M.T.Esat, M.P.Fewell, S.Hinds, A.M.R.Joye, D.C.Kean Vibrational Excitations in the Even-Mass Cadmium Isotopes NUCLEAR REACTIONS 106,108,110,112,114,116Cd(α, α), (α, α'), E=17.5 MeV; measured σ(Eα'). 106,108,110,112,114,116Cd deduced levels.
doi: 10.1071/PH770133
1976ES01 Phys.Lett. 61B, 242 (1976) M.T.Esat, D.C.Kean, R.H.Spear, R.A.I.Bell Quadrupole Moments in the Cadmium Isotopes NUCLEAR REACTIONS 106,110,112,114,116Cd(α, α'γ), E=8.5 MeV; 106,110,112,114,116Cd(16O, 16O'γ), E=44 MeV; measured Coulomb excitation. 106,110,112,114,116Cd levels deduced B(E2).
doi: 10.1016/0370-2693(76)90139-8
1976ES02 Nucl.Phys. A274, 237 (1976) M.T.Esat, D.C.Kean, R.H.Spear, A.M.Baxter Mass Dependence of the Static Quadrupole Moments of the First 2+ States in the Cadmium Isotopes NUCLEAR REACTIONS 106,108,110,112,114,116Cd(α, α'), E=8-17 MeV; 106,108,110,112,114,116Cd(16O, 16O'), E=40-44 MeV; measured Coulomb excitation probabilities of first 2+ states. 106,108,110,112,114,116Cd deduced B(E2), quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(76)90239-6
1975OL02 Can.J.Phys. 53, 123 (1975) R.W.Ollerhead, D.C.Kean, S.G.T.Leong, C.Doekes, T.M.R.Meadley Branching Ratios and Lifetimes of 25Mg Levels between 5.2 and 6.1 MeV NUCLEAR REACTIONS 25Mg(p, p'γ); measured Ep', γγ-coin, DSA. 25Mg deduced levels, T1/2, γ-branching ratios, J, π.
doi: 10.1139/p75-018
1975SP02 Phys.Rev. C11, 742 (1975) R.H.Spear, R.A.I.Bell, M.T.Esat, P.R.Gardner, D.C.Kean, A.M.Baxter Electromagnetic Transitions in 22Na NUCLEAR REACTIONS 23Na(3He, αγ), E=8.46 MeV; measured αγ-coin. 19F(α, nγ), E=4.7-6.1, 11.2 MeV; measured σ(E, Eγ, θ), nγ(θ). 22Na levels deduced J, π, γ-mixing, Q0, g K-gR.
doi: 10.1103/PhysRevC.11.742
1974KE02 Can.J.Phys. 52, 265 (1974) The Mixing Ratio of the (p3/2)-1 → (p1/2)-1 Transition in 15O NUCLEAR REACTIONS 14N(p, γ); measured γγ(θ). 15O deduced γ-mixing.
doi: 10.1139/p74-037
1974OL07 Can.J.Phys. 52, 2329 (1974) R.W.Ollerhead, D.C.Kean, R.M.Gorman, M.B.Thomson Branching Ratios and Lifetimes of 25Mg Levels below 5.2 MeV NUCLEAR REACTIONS 25Mg(p, p'γ), E=9 MeV; measured σ(Ep'), p'γ-coin, DSA. 25Mg deduced levels, T1/2, γ-branching ratios, E2, M1 strengths, quadrupole moment.
doi: 10.1139/p74-304
1973GA30 Aust.J.Phys. 26, 747 (1973) P.R.Gardner, D.C.Kean, R.H.Spear, A.M.Baxter, R.A.I.Bell, L.E.Carlson Spin-Parity Combinations in 32S NUCLEAR REACTIONS 32S(α, α'), (p, p'), (p, p'γ), Eα=16.8-18.2 MeV, Ep=11.2, 9.16 MeV; measured σ(E, Eα', θ), σ(Ep', θ), p'γ-coin. 32S deduced levels, J, π.
doi: 10.1071/PH730747
1973GA31 Aust.J.Phys. 26, 739 (1973) P.R.Gardner, A.M.Baxter, R.A.I.Bell, L.E.Carlson, D.C.Kean, T.R.Ophel, R.H.Spear Polarization Studies of Ground-State Radiation from the 2.21 and 2.73 MeV Levels of 27Al NUCLEAR REACTIONS 27Al(p, p'γ), E=4.41 MeV; measured Eγ, Iγ, γ(θ), γγcoin, P(γ). 27Al levels deduced γ-mixing.
doi: 10.1071/PH730739
1972KE13 Can.J.Phys. 50, 1539 (1972) A Study of Levels in 25Mg via the 22Ne(α, nγ)25Mg Reaction NUCLEAR REACTIONS 22Ne(α, nγ), E=4.8-7.0 MeV; measured σ(E;Eγ, θ(γ)), γ-linear polarization. 25Mg deduced levels, J, π, γ-mixing, γ-branching.
doi: 10.1139/p72-208
1971BA27 Aust.J.Phys. 24, 1 (1971) F.C.Barker, K.W.Carter, D.C.Kean, C.J.Piluso, R.H.Spear A Study of the Energy Levels of 27Si NUCLEAR REACTIONS 28Si(3He, α), E=11 MeV; measured σ(Eα). 27Si deduced levels.
1971CA38 Aust.J.Phys. 24, 471 (1971) K.W.Carter, D.C.Kean, C.J.Piluso, R.H.Spear A Search for High-Spin State in 27Al NUCLEAR REACTIONS 12C(16O, pγ), 24Mg(α, pγ), E(16O) < 30 MeV, Eα=11-16 MeV; measured σ(Ep, Eγ, θ(γ), θ(pγ)). 27Al deduced levels, J, π, γ-branching.
1971DO04 Can.J.Phys. 49, 483 (1971) C.Doekes, D.C.Kean, R.V.Elliott, R.H.Spear High Resolution Study of the Energy Levels of 27Al NUCLEAR REACTIONS 27Al(p, p'), E=15 MeV; measured σ(Ep', θ). 27Al deduced levels.
doi: 10.1139/p71-062
1971KE18 Can.J.Phys. 49, 2793 (1971) Spin of the 4.057 MeV Level in 25Mg NUCLEAR REACTIONS 22Ne(α, nγ), E=6.2, 6.8 MeV; measured Iγ(θ), γ-linear polarization. 25Mg level deduced J, π. Ge(Li) detector.
doi: 10.1139/p71-338
1971PI06 Aust.J.Phys. 24, 459 (1971) C.J.Piluso, R.H.Spear, K.W.Carter, D.C.Kean, F.C.Barker Magnetic Analysis of the Reactions 7Li(3He, d)8Be and 7Li(3He, t)7Be NUCLEAR REACTIONS 7Li(3He, d), (3He, t), E=15 MeV; measured σ(Ed, θ), σ(Et, θ). 7,8Be deduced levels, level-width.
1969CA04 Nucl.Phys. A126, 49(1969) K.W.Carter, R.V.Elliott, D.C.Kean, R.H.Spear Angular-Correlation Studies of the Reaction 24Mg(α, pγ)27Al NUCLEAR REACTIONS 24Mg(α, pγ), E=9.1, 13.0 MeV; measured σ(Ep, Eγ, θ(pγ)). 27Al levels deduced γ-branching, J, π, delta. Enriched target.
doi: 10.1016/0375-9474(69)90399-6
1969CA12 Nucl.Phys. A134, 505(1969) K.W.Carter, D.C.Kean, C.J.Piluso, R.H.Spear The 4.41 and 4.51 MeV Levels of 27Al NUCLEAR REACTIONS 24Mg(α, pγ), E = 10.51 MeV; measured α, pγ(θ), Eγ, Iγ. 27Al levels deduced γ-branching, J, delta. Enriched target.
doi: 10.1016/0375-9474(69)90017-7
1969KE01 Nucl.Phys. A123, 430(1969) D.C.Kean, K.W.Carter, R.H.Spear Gamma-Ray Branching Ratios of the Low-Lying Levels of 29Al NUCLEAR REACTIONS 26Mg(α, pγ), E=10.4-10.9 MeV; measured σ(Eγ, Ep). 29Al levels deduced γ-branchings. Enriched target.
doi: 10.1016/0375-9474(69)90511-9
1969KE08 Nucl.Phys. A132, 241 (1969) D.C.Kean, K.W.Carter, C.J.Piluso, R.H.Spear Angular Correlation Studies of the Low-Lying Levels of 29Al NUCLEAR REACTIONS 26Mg(α, pγ), E=10.6, 11.3 MeV; measured σ(Ep, Eγ, θ), Eγ, Iγ. 29Al levels deduced γ-branching, J, delta. Enriched target.
doi: 10.1016/0375-9474(69)90481-3
1968KE07 Australian J. Phys. 21, 405 (1968) D.C.Kean, R.V.Elliott, R.H.Spear A Study of the 3.00 MeV Level of 27Al via 24Mg(α, pγ)27Al NUCLEAR STRUCTURE 27Al; measured not abstracted; deduced nuclear properties.
doi: 10.1071/PH680405
1967HA17 Nucl.Phys. A98, 330(1967) Energy Levels of 23Na and 23Mg NUCLEAR REACTIONS 24Mg(3He, α), 25Mg(d, α), E = 8, 10 MeV; measured σ(Eα). 23Na, 23Mg deduced levels. Enriched targets.
doi: 10.1016/0375-9474(67)90143-1
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