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NSR database version of April 11, 2024.

Search: Author = D.F.Hebbard

Found 27 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0694.


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, β42, shape parameters. Asymmetric rotor model, coupled-channels analysis.

doi: 10.1016/0375-9474(83)90607-3
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1569.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1964EA04      Nucl.Phys. 53, 252 (1964)

L.G.Earwaker, D.F.Hebbard

States in N14 Near the Proton Threshold

NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(64)90603-0
Citations: PlumX Metrics


1963BA42      ANU-P/291 (1963)

G.M.Bailey, D.F.Hebbard

Non-Resonant Radiation from the N14(p, γ) Reaction

NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.


1963HE04      Nucl.Phys. 42, 563 (1963)

D.F.Hebbard, B.A.Robson

Tables of Whittaker Functions and their Logarithmic Derivatives

doi: 10.1016/0029-5582(63)90757-0
Citations: PlumX Metrics


1963HE11      Nucl.Phys. 49, 666 (1963)

D.F.Hebbard, G.M.Bailey

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0764.


1960HE02      Nuclear Phys. 15, 289 (1960)

D.F.Hebbard

Proton Capture by N15

NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(60)90308-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0646.


1960HE13      Nuclear Phys. 19, 511 (1960)

D.F.Hebbard

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
Citations: PlumX Metrics


1960HE14      Nuclear Phys. 21, 652 (1960)

D.F.Hebbard, J.L.Vogl

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0475.


1959HE47      Nuclear Phys. 13, 642 (1959)

D.F.Hebbard, B.Povh

Gamma Ray Cascades in O15

doi: 10.1016/0029-5582(59)90263-9
Citations: PlumX Metrics


1959PO79      Phys.Rev. 115, 608 (1959)

B.Povh, D.F.Hebbard

Angular Correlation Measurements in O15

doi: 10.1103/PhysRev.115.608
Citations: PlumX Metrics


1958HE48      Bull.Am.Phys.Soc. 3, No.5, 322, H3 (1958)

D.F.Hebbard, D.N.F.Dunbar

C14(p, p)C14 and C14(p, γ)N15 Reactions


1958HE52      Bull.Am.Phys.Soc. 3, No.8, 406, F6 (1958)

D.F.Hebbard

Gamma Rays from the 12.43-MeV Level in O16


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