NSR Query Results
Output year order : Descending NSR database version of May 8, 2024. Search: Author = D.F.Hebbard Found 27 matches. 1988HE06 Nucl.Phys. A481, 161 (1988) D.F.Hebbard, J.Nurzynski, T.R.Ophel, P.V.Drumm, Y.Kondo, B.A.Robson, R.Smith The 20Ne(16O, 16O)20Ne Excitation Function at θ(cm) = 90° and Parity-Dependent Interactions NUCLEAR REACTIONS 20Ne(16O, 16O), (16O, 16O'), E(cm)=21.5-31.2 MeV; measured σ(E); deduced optical model parameters. 36Ar resonances deduced parity. Extended optical model analysis.
doi: 10.1016/0375-9474(88)90478-2
1986DR11 Aust.J.Phys. 39, 369 (1986) P.V.Drumm, D.F.Hebbard, T.R.Ophel, J.Nurzynski, Y.Kondo, B.A.Robson, R.Smith Excitation Function for 16O + 24Mg Elastic Scattering at θ(c.m.) = 90° NUCLEAR REACTIONS 24Mg(16O, 16O), (16O, 16O'), E=53-75.5 MeV; measured σ(E(16O)), σ(θ) vs E. Enge split-pole magnetic spectrometer. Optical model analysis.
doi: 10.1071/PH860369
1986NU01 J.Phys.(London) G12, 383 (1986) J.Nurzynski, D.F.Hebbard, T.R.Ophel, Y.Kondo, B.A.Robson, R.Smith Excitation Functions for 24Mg(16O, 16O')24Mg(*) (0 ≤ E(x) ≤ 8.4 MeV) Scattering at Forward Angles NUCLEAR REACTIONS 24Mg(16O, 16O'), E(cm)=33.6-49.2 MeV; measured σ(E(16O)), σ(θ) vs E. 16O, 24Mg levels deduced possible excitation. Enriched target, magnetic spectrometer. Coupled channels calculations.
doi: 10.1088/0305-4616/12/5/005
1983NU01 Nucl.Phys. A399, 259 (1983) J.Nurzynski, C.H.Atwood, T.R.Ophel, D.F.Hebbard, B.A.Robson, R.Smith The 24Mg(16O, 16O') Reaction and Triaxial Structures in 24Mg NUCLEAR REACTIONS 24Mg(16O, 16O'), E=43.5 MeV; measured σ(θ); deduced optical model parameters. 24Mg levels deduced B(E2), quadrupole moment, β4/β2, shape parameters. Asymmetric rotor model, coupled-channels analysis.
doi: 10.1016/0375-9474(83)90607-3
1981CL01 Nucl.Phys. A352, 267 (1981) P.D.Clark, T.R.Ophel, J.Nurzynski, C.H.Atwood, D.F.Hebbard Spin Assignments from the 142Nd(7Li, 6He)143Pm and 144Sm(7Li, 6He)145Eu Reactions at 52 MeV NUCLEAR REACTIONS 142Nd, 144Sm(7Li, 7Li), (7Li, 6He), E=52 MeV; 142Nd(6Li, 6Li), E=46 MeV; 144Sm(6Li, 6Li), E=45 MeV; measured σ(θ); deduced optical-model parameters. 143Pm, 145Eu levels deduced S, J, π. Enriched targets, finite-range DWBA analysis.
doi: 10.1016/0375-9474(81)90380-8
1981EC02 Phys.Rev. C23, 2068 (1981) J.S.Eck, J.Nurzynski, T.R.Ophel, P.D.Clark, D.F.Hebbard, D.C.Weisser Possible Triaxial Structures in 24Mg from 16O + 24Mg Elastic and Inelastic Scattering NUCLEAR REACTIONS 24Mg(16O, 16O), (16O, 16O'), E=67 MeV; measured σ(θ). Triaxial rotor model, coupled-channels analysis.
doi: 10.1103/PhysRevC.23.2068
1981NU02 Nucl.Phys. A363, 253 (1981) J.Nurzynski, T.R.Ophel, P.D.Clark, J.S.Eck, D.F.Hebbard, D.C.Weisser, B.A.Robson, R.Smith Energy Dependence of the 24Mg(16O, 12C)28Si Reaction NUCLEAR REACTIONS 24Mg(16O, 12C), E=32.4-48.6 MeV; measured σ(E, θ); 24Mg(16O, 16O), E=37.5, 40.2 MeV; measured σ(θ); deduced optical model parameters. 40Ca resonances deduced J. DWBA analysis, band crossing model.
doi: 10.1016/0375-9474(81)90465-6
1980CL08 Nucl.Phys. A349, 258 (1980) P.D.Clark, T.R.Ophel, J.S.Eck, A.F.Zeller, J.Nurzynski, D.C.Weisser, D.F.Hebbard Spin Assignments from the 138Ba(7Li, 6He)139La and 140Ce(7Li, 6He)141Pr Reactions at 52 MeV NUCLEAR REACTIONS 138Ba, 140Ce(7Li, 7Li), (7Li, 6He), E=52 MeV; 139La(6Li, 6Li), E=48 MeV; 141Pr(6Li, 6Li), E=47 MeV; measured σ(θ); deduced optical model parameters. 139La, 141Pr levels deduced S, J, π. Enriched targets. Finite-range DWBA analysis.
doi: 10.1016/0375-9474(80)90453-4
1979KE05 Nucl.Phys. A320, 413 (1979) K.W.Kemper, A.F.Zeller, T.R.Ophel, D.F.Hebbard, A.Johnston, D.C.Weisser Elastic and Inelastic Scattering of 6Li and 7Li and 54Fe at E = 36-50 MeV NUCLEAR REACTIONS 54Fe(6Li, 6Li), (6Li, 6Li'), E=38, 44, 50 MeV; 54Fe(7Li, 7Li), (7Li, 7Li'), E=36, 42, 48 MeV; measured σ(θ). 54Fe levels deduced optical-model parameters, deformation lengths.
doi: 10.1016/0375-9474(79)90198-2
1979ZE01 Nucl.Phys. A323, 477 (1979) A.F.Zeller, K.W.Kemper, D.C.Weisser, T.R.Ophel, D.F.Hebbard, A.Johnston Lithium-Induced Reactions on Carbon at 48 MeV NUCLEAR REACTIONS 12C(7Li, 7Li), (7Li, 7Li'), (7Li, 6He), (7Li, 6Li), E=48; 13C(6Li, 6Li), (6Li, 6He), E=40 MeV; measured σ(θ); deduced optical-model parameters. 13N, 13C deduced S. Enriched targets, finite range DWBA analysis.
doi: 10.1016/0375-9474(79)90121-0
1979ZE03 Nucl.Phys. A332, 515 (1979) A.F.Zeller, D.C.Weisser, T.R.Ophel, D.F.Hebbard The 208Pb(7Li, 6He)209Bi Reaction at 52 MeV NUCLEAR REACTIONS 208Pb(7Li, 7Li), (7Li, 6He), E=52 MeV; 209Bi(6Li, 6Li), E=44 MeV; measured σ(θ); deduced optical model parameters. 209Bi levels deduced S. Enriched target, finite range DWBA analysis.
doi: 10.1016/0375-9474(79)90016-2
1978WE14 Nucl.Phys. A308, 222 (1978) D.C.Weisser, A.F.Zeller, T.R.Ophel, D.F.Hebbard Mass of 48K NUCLEAR REACTIONS 48Ca(7Li, 7Be), E=52 MeV; measured σ(23.75°), σ(27.75°). 48K deduced mass excess, level. Enriched target.
doi: 10.1016/0375-9474(78)90451-7
1978ZE02 Nucl.Phys. A301, 130 (1978) A.F.Zeller, G.T.Hickey, D.C.Weisser, D.F.Hebbard, B.A.Robson The 26Mg(14N, 10B)30Si and 26Mg(14N, 11B)29Si Reactions NUCLEAR REACTIONS 26Mg(14N, 14N), (14N, 10B), (14N, 11B), E=60-95 MeV; measured σ(E, θ); deduced optical model parameters, reaction mechanism. 30Si levels deduced S. DWBA, Hauser-Feshbach analysis. Enriched targets.
doi: 10.1016/0375-9474(78)90133-1
1978ZE05 Nucl.Phys. A309, 255 (1978) A.F.Zeller, K.W.Kemper, T.R.Ophel, D.C.Weisser, D.F.Hebbard, A.Johnston, G.T.Hickey The 118Sn(7Li, 6He)119Sb Reaction at 48 MeV NUCLEAR REACTIONS 118Sn(6Li, 6Li), E=42 MeV; 118Sn(7Li, 7Li), 118Sn(7Li, 6He), E=48 MeV; measured σ(θ). 119Sb levels deduced S. Finite-range DWBA analysis; deduced optical model parameters. Enriched targets.
doi: 10.1016/0375-9474(78)90546-8
1977HI03 J.Phys.(London) G3, L81 (1977) G.T.Hickey, A.F.Zeller, D.C.Weisser, D.F.Hebbard, T.R.Ophel A Search for 15B NUCLEAR REACTIONS 11B(18O, 14O), E=96, 103 MeV; measured upper limit σ.
doi: 10.1088/0305-4616/3/1/010
1976HI10 Phys.Rev.Lett. 37, 130 (1976) G.T.Hickey, D.C.Weisser, J.Cerny, G.M.Crawley, A.F.Zeller, T.R.Ophel, D.F.Hebbard Use of the Four-Neutron Transfer Reaction 18O(18O, 14O)22O to Determine The Mass of 22O NUCLEAR REACTIONS 18O(18O, 14O), E=100 MeV; measured σ; deduced Q. 22O deduced mass excess.
doi: 10.1103/PhysRevLett.37.130
1964EA04 Nucl.Phys. 53, 252 (1964) States in N14 Near the Proton Threshold NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90603-0
1963BA42 ANU-P/291 (1963) Non-Resonant Radiation from the N14(p, γ) Reaction NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1963HE04 Nucl.Phys. 42, 563 (1963) Tables of Whittaker Functions and their Logarithmic Derivatives
doi: 10.1016/0029-5582(63)90757-0
1963HE11 Nucl.Phys. 49, 666 (1963) Non-Resonant Radiation from the N14(p, γ) Reaction (II) NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90130-5
1960HE02 Nuclear Phys. 15, 289 (1960) Proton Capture by N15 NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90308-4
1960HE13 Nuclear Phys. 19, 511 (1960) Gamma Rays from the 351-keV C14(p, γ) Resonance NUCLEAR STRUCTURE 15N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90261-3
1960HE14 Nuclear Phys. 21, 652 (1960) Elastic Scattering and Radiative Capture of Protons by C13 NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90084-5
1959HE47 Nuclear Phys. 13, 642 (1959) Gamma Ray Cascades in O15
doi: 10.1016/0029-5582(59)90263-9
1959PO79 Phys.Rev. 115, 608 (1959) Angular Correlation Measurements in O15
doi: 10.1103/PhysRev.115.608
1958HE48 Bull.Am.Phys.Soc. 3, No.5, 322, H3 (1958) C14(p, p)C14 and C14(p, γ)N15 Reactions
1958HE52 Bull.Am.Phys.Soc. 3, No.8, 406, F6 (1958) Gamma Rays from the 12.43-MeV Level in O16
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