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Search: Author = T.R.Ophel

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1996FI12      Nucl.Instrum.Methods Phys.Res. B117, 295 (1996)

L.K.Fifield, R.G.Cresswell, M.L.di Tada, T.R.Ophel, J.P.Day, A.P.Clacher, S.J.King, N.D.Priest

Accelerator Mass Spectrometry of Plutonium Isotopes

doi: 10.1016/0168-583X(96)00287-X
Citations: PlumX Metrics

1993CO03      Phys.Rev. C47, 1048 (1993)

P.D.Cottle, K.W.Kemper, M.A.Kennedy, L.F.Fifield, T.R.Ophel

5^- ' Octupole ' States in ^{146, 148}Nd and ¹⁴⁸Sm via Proton Scattering

NUCLEAR REACTIONS ^146,148Nd(p, p'), ¹⁴⁸Sm(p, p'), E=26 MeV; measured spectra, σ(θ). ^146,148Nd, ¹⁴⁸Sm deduced level configurations.

doi: 10.1103/PhysRevC.47.1048
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1596.

1993FI03      Nucl.Phys. A552, 125 (1993)

L.K.Fifield, W.N.Catford, N.A.Orr, T.R.Ophel, A.Etchegoyen, M.C.Etchegoyen

Charge-Exchange Reactions on ³⁶S

NUCLEAR REACTIONS ³⁶S(⁷Li, ⁷Be), E=54 MeV; ³⁶S(¹¹B, ¹¹C), E=81 MeV; ³⁶S(¹³C, ¹³N), E=94.5 MeV; ³⁶S(¹³C, ¹³C), E=98 MeV; ³⁶S(¹⁸O, ¹⁸F), E=124 MeV; ³⁶S(¹⁸O, ¹⁸O), E=112 MeV; measured σ(θ), spectra; deduced optical potentials, reaction mechanism.

doi: 10.1016/0375-9474(93)90335-U
Citations: PlumX Metrics

1989OR03      Nucl.Phys. A491, 443 (1989)

N.A.Orr, W.N.Catford, L.K.Fifield, M.A.C.Hotchkis, T.R.Ophel, D.C.Weisser, C.L.Woods

Observations of ²⁰N via the Heavy-Ion Transfer Reaction ⁴⁸Ca(¹⁸O, ²⁰N)⁴⁶Sc

NUCLEAR REACTIONS ⁴⁸Ca(¹⁸O, ²⁰N), E=108-119 MeV; measured Q, σ(E(²⁰N)). ²⁰N deduced mass excess.

doi: 10.1016/0375-9474(89)90578-2
Citations: PlumX Metrics

1988CA21      Nucl.Phys. A489, 347 (1988)

W.N.Catford, L.K.Fifield, T.R.Ophel, N.A.Orr, D.C.Weisser, C.L.Woods

Study of ⁵¹Ca via Three-Neutron Transfer

NUCLEAR REACTIONS ⁴⁸Ca(¹⁸O, ¹⁵O), E=108 MeV; measured σ(E(¹⁵O)). ⁵¹Ca deduced ground state mass excess, levels. Enriched target.

doi: 10.1016/0375-9474(88)90157-1
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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

1988OR01      Nucl.Phys. A477, 523 (1988); Erratum Nucl.Phys. A485, 734 (1988)

N.A.Orr, W.N.Catford, L.K.Fifield, T.R.Ophel, D.C.Weisser, C.L.Woods

Heavy-Ion Reaction Studies of ^35,36P

NUCLEAR REACTIONS ³⁷Cl(¹¹B, ¹³N), ³⁷Cl(¹³C, ¹⁴O), ³⁴S(¹⁸O, ¹⁷F), E=81-108 MeV; measured σ(E(¹³N)), σ(E(¹⁴O)), σ(E(¹⁷F)). ^35,36P deduced ground-state mass excess, levels. Enriched targets.

doi: 10.1016/0375-9474(88)90355-7
Citations: PlumX Metrics

1987EN04      Nucl.Phys. A470, 241 (1987)

J.B.A.England, T.R.Ophel, R.A.Bark, L.K.Fifield

A Study of States in ⁵⁷Co via the Reaction ⁵⁶Fe(⁷Li, ⁶He)⁵⁷Co at 38 MeV

NUCLEAR REACTIONS ⁵⁶Fe(⁷Li, ⁶He), E=38 MeV; measured σ(E(⁶He)), σ(θ). ⁵⁷Co deduced levels, J, π, spectroscopic factors. Full finite-range DWBA calculations.

doi: 10.1016/0375-9474(87)90131-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0861.

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

1985FI08      Nucl.Phys. A437, 141 (1985)

L.K.Fifield, P.V.Drumm, M.A.C.Hotchkis, T.R.Ophel, C.L.Woods

The ²⁶Mg(¹⁸O, ¹⁷F)²⁷Na and ²⁶Mg(¹⁸O, ¹⁵O)²⁹Mg Reactions and the Level Schemes of ²⁷Na and ²⁹Mg

NUCLEAR REACTIONS ²⁶Mg(¹⁸O, ¹⁷F), (¹⁸O, ¹⁵O), E=100-117 MeV; measured σ(E(¹⁷F)), σ(E(¹⁵O)). ²⁷Na, ²⁹Mg deduced levels, ground state mass excesses. Enriched targets.

doi: 10.1016/0375-9474(85)90230-1
Citations: PlumX Metrics

1984CO05      Nucl.Phys. A415, 114 (1984)

J.Cook, L.C.Dennis, K.W.Kemper, T.R.Ophel, A.F.Zeller, C.F.Maguire, Z.Kui

Large-Angle Enhancements in the ¹⁶O(⁶Li, α)¹⁸F Reaction at 48 MeV

NUCLEAR REACTIONS ¹⁶O(⁶Li, ⁶Li), (⁶Li, α), E=48 MeV; measured σ(θ); deduced optical model parameters. Finite-range DWBA analysis including exchange.

doi: 10.1016/0375-9474(84)90602-X
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1984CO20      Phys.Rev. C30, 1538 (1984)

J.Cook, K.W.Kemper, P.V.Drumm, L.K.Fifield, M.A.C.Hotchkis, T.R.Ophel, C.L.Woods

¹⁶O(⁷Li, ⁷Be)¹⁶N Reaction at 50 MeV

NUCLEAR REACTIONS ¹⁶O(⁷Li, ⁷Li), (⁷Li, ⁷Be), E=50 MeV; measured σ(θ), σ(E(¹⁶N)); deduced optical model parameters. ¹⁶N levels deduced spectroscopic amplitudes. Microscopic DWBA analysis.

doi: 10.1103/PhysRevC.30.1538
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1521.

1984EC01      Nucl.Phys. A425, 141 (1984)

J.S.Eck, K.W.Kemper, T.R.Ophel

The (⁷Li, ⁶Li) Reaction on ²⁸Si and ⁴⁰Ca at E(⁷Li) = 45 MeV

NUCLEAR REACTIONS ²⁸Si, ⁴⁰Ca(⁷Li, ⁶Li), E=45 MeV; measured σ(θ); deduced potential parameters. ⁴¹Ca, ²⁹Si levels deduced absolute C²S spectroscopic factors. DWBA analysis, Woods-Saxon, double folding potentials.

doi: 10.1016/0375-9474(84)90220-3
Citations: PlumX Metrics

1984FI02      Nucl.Phys. A417, 534 (1984)

L.K.Fifield, M.A.C.Hotchkis, P.V.Drumm, T.R.Ophel, G.D.Putt, D.C.Weisser

The Mass and Low-Lying Levels of ⁴⁰Cl

NUCLEAR REACTIONS ⁴⁰Ar(⁷Li, ⁷Be), E=52, 54 MeV; ⁴⁰Ar(¹¹B, ¹¹C), (¹¹B, ¹³N), E=81 MeV; measured σ(E(⁷Be)), σ(E(¹¹C)), σ(E(¹³N)). ⁴⁰Cl deduced mass excess, levels. ³⁸S deduced levels.

doi: 10.1016/0375-9474(84)90411-1
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1984OM02      Phys.Rev. C30, 896 (1984)

A.R.Omar, J.S.Eck, J.R.Leigh, T.R.Ophel

Elastic and Inelastic Scattering of ⁹Be + ⁹Be at E(⁹Be) = 35-50 MeV

NUCLEAR REACTIONS ⁹Be(⁹Be, ⁹Be), (⁹Be, ⁹Be'), E=35, 40, 45, 50 MeV; measured σ(E(⁹Be)), σ(θ); deduced potential parameters, β. Optical, coupled-channels model analysis.

doi: 10.1103/PhysRevC.30.896
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1527.

1984OM03      Phys.Rev. C30, 1516 (1984)

A.R.Omar, J.S.Eck, T.R.Ophel, J.R.Leigh

Total Fusion of ⁹Be + ⁹Be at E(⁹Be) = 35-55 MeV

NUCLEAR REACTIONS, ICPND ⁹Be(⁹Be, X), E=35, 40, 45, 50, 55 MeV; measured evaporation residue σ(θ), σ vs Z, fusion σ(E). ¹²C(¹³C, X), E(cm)=10-45 MeV; calculated total reaction σ. Optical model.

doi: 10.1103/PhysRevC.30.1516
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1528.

1983EC01      Phys.Rev. C27, 1807 (1983)

J.S.Eck, A.R.Omar, J.R.Leigh, T.R.Ophel

Fusion Cross Sections for ⁹Be + ⁴⁰Ca

NUCLEAR REACTIONS, ICPND ⁴⁰Ca(⁹Be, X), E=35, 40, 45, 50, 55, 60 MeV; measured σ(evaporation residue θ); deduced fusion σ. ⁴⁰Ca(⁹Be, ⁹Be), E=35-60 MeV; calculated σ(θ); deduced reaction σ. Optical model.

doi: 10.1103/PhysRevC.27.1807
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1529.

1983HO08      Nucl.Phys. A398, 130 (1983)

M.A.C.Hotchkis, L.K.Fifield, J.R.Leigh, T.R.Ophel, G.D.Putt, D.C.Weisser

New Measurements of the Masses of ¹⁵B and ¹⁹N

NUCLEAR REACTIONS ⁴⁸Ca(¹⁸O, ¹⁵B), (¹⁸O, ¹⁹N), E=108-119 MeV; measured σ(E(¹⁵B)), σ(E(¹⁹N)). ¹⁵B, ¹⁹N deduced mass excess. Enriched target.

doi: 10.1016/0375-9474(83)90652-8
Citations: PlumX Metrics

1983KE06      Nucl.Phys. A405, 348 (1983)

K.W.Kemper, G.G.Shute, C.H.Atwood, L.K.Fifield, T.R.Ophel

Spectroscopy of A = 16 from ¹³C(¹⁶Li, t)¹⁶O

NUCLEAR REACTIONS ¹³C(⁶Li, t), E=34 MeV; measured σ(θ). ¹⁶O levels deduced L, Γ, possible J, π. ¹⁶N, ¹⁶F deduced IAS. Hauser-Feshbach, finite range DWBA calculations.

doi: 10.1016/0375-9474(83)90576-6
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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
Citations: PlumX Metrics

1983PU01      Nucl.Phys. A399, 190 (1983)

G.D.Putt, L.K.Fifield, M.A.C.Hotchkis, T.R.Ophel, D.C.Weisser

The Mass of ¹⁸N

NUCLEAR REACTIONS ¹⁸O(⁷Li, ⁷Be), E=52 MeV; measured σ(E(⁷Be)). ¹⁸N deduced mass excess, levels. Enriched target.

doi: 10.1016/0375-9474(83)90602-4
Citations: PlumX Metrics

1982EC01      Phys.Rev. C25, 2391 (1982)

J.S.Eck, T.R.Ophel, P.D.Clark, J.Nurzynski, D.C.Weisser

Optical Model and Coupled-Channels Analysis of ⁷Li + ²⁸Si and ⁷Li + ⁴⁰Ca Scattering

NUCLEAR REACTIONS ²⁸Si, ⁴⁰Ca(⁷Li, ⁷Li), (⁷Li, ⁷Li'), E=45 MeV; measured σ(θ); deduced optical model parameters. ⁴⁰Ca deduced deformation length. Double folding model, coupled-channels calculations.

doi: 10.1103/PhysRevC.25.2391
Citations: PlumX Metrics

1982FI10      Nucl.Phys. A385, 505 (1982)

L.K.Fifield, J.L.Durell, M.A.C.Hotchkis, J.R.Leigh, T.R.Ophel, D.C.Weisser

The Mass of ¹⁸C from a Heavy Ion Double-Charge-Exchange Reaction

NUCLEAR REACTIONS ⁴⁸Ca(¹⁸O, ¹⁸C), ⁴⁸Ca(¹⁸O, ¹⁷C), E=112 MeV; measured σ(E(¹⁸C)), σ(E(¹⁷C)). ¹⁸C, ¹⁷C deduced mass excesses, levels. Enriched target.

doi: 10.1016/0375-9474(82)90100-2
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1982FU06      J.Phys.(London) G8, L141 (1982)

B.R.Fulton, J.B.A.England, S.D.Hoath, C.H.Atwood, T.R.Ophel

Intermediate Structure in the ²⁴Mg(¹⁶O, ¹²C)²⁸Si Reaction

NUCLEAR REACTIONS ²⁴Mg(¹⁶O, ¹²C), E(cm) ≈ 32-36 MeV; measured σ(θ=5°) vs E; deduced gross structure splitting, reaction mechanism.

doi: 10.1088/0305-4616/8/8/006
Citations: PlumX Metrics

1982KE12      Nucl.Phys. A391, 237 (1982)

K.W.Kemper, A.F.Zeller, T.R.Ophel, D.P.Stanley

⁷Li + ⁵⁴Fe Single-Nucleon Stripping Reactions at E = 48 MeV

NUCLEAR REACTIONS ⁵⁴Fe(⁷Li, ⁶Li), (⁷Li, ⁶He), E=48 MeV; measured σ(θ). ⁵⁵Co levels deduced J, C²S, single particle centroid energies. ⁵⁵Fe levels deduced C²S.

doi: 10.1016/0375-9474(82)90230-5
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1982LE14      Nucl.Phys. A382, 115 (1982)

J.Leigh, T.R.Ophel, D.C.Weisser, W.R.Phillips

The (⁷Li, ⁸Li) Reaction to the (h_9/2)^-1 State in ²⁰⁷Pb

NUCLEAR REACTIONS ²⁰⁸Pb(⁷Li, ⁸Li), E=52 MeV; measured σ(θ). ²⁰⁸Pb deduced 1h_9/2 neutron orbit rms radius, neutron excess distribution.

doi: 10.1016/0375-9474(82)90444-4
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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
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1981EC01      Phys.Rev. C23, 228 (1981)

J.S.Eck, T.R.Ophel, P.D.Clark, D.C.Weisser, G.R.Satchler

Elastic and Inelastic Scattering Measurements for the ²⁴Mg + ²⁰⁸Pb and ²⁸Si + ²⁰⁸Pb Systems

NUCLEAR REACTIONS ²⁰⁸Pb(²⁴Mg, ²⁴Mg), (²⁴Mg, ²⁴Mg'), E=145 MeV; ²⁰⁶Pb(²⁸Si, ²⁸Si), (²⁸Si, ²⁸Si'), E=162 MeV; measured σ(θ). ^208,206Pb level deduced deformation β₂. Optical model, coupled-channel analyses.

doi: 10.1103/PhysRevC.23.228
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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
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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

1980EC01      Nucl.Phys. A334, 519 (1980)

J.S.Eck, T.R.Ophel, P.D.Clark, D.C.Weisser

Classical and Potential Descriptions of ⁹Be + ²⁸Si and ⁹Be + ⁴⁰Ca Elastic Scattering Cross Sections at E(⁹Be) = 45 and 60 MeV

NUCLEAR REACTIONS ²⁸Si, ⁴⁰Ca(⁹Be, ⁹Be), E=45, 60 MeV; measured σ(θ). Wegner plots, optical-model, double-folding procedure analysis.

doi: 10.1016/0375-9474(80)90615-6
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1980EC03      Phys.Rev. C21, 2352 (1980)

J.S.Eck, J.R.Leigh, T.R.Ophel, P.D.Clark

Total Fusion Cross Section for the ⁹Be + ²⁸Si System

NUCLEAR REACTIONS ²⁸Si(⁹Be, X), E=30-60 MeV; measured evaporation residue σ(θ), total fusion σ.

doi: 10.1103/PhysRevC.21.2352
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1536.

1980EC04      Nucl.Phys. A341, 178 (1980)

J.S.Eck, T.R.Ophel, P.D.Clark, D.C.Weisser, G.R.Satchler

Inelastic Scattering of ⁹Be Projectiles to Low-Lying Collective States in ²⁸Si and ⁴⁰Ca at E(⁹Be) = 45 and 60 MeV

NUCLEAR REACTIONS ⁴⁰Ca, ²⁸Si(⁹Be, ⁹Be'), E=45, 60 MeV; measured σ(θ). DWBA, double-folding model potential.

doi: 10.1016/0375-9474(80)90369-3
Citations: PlumX Metrics

1980EC06      Aust.J.Phys. 33, 191 (1980)

J.S.Eck, T.R.Ophel, D.C.Weisser, P.D.Clark

Application of the Frahn Scaling Formula to the Analysis of the Excitation of 1^- States in ⁴⁰Ca by ⁹Be Scattering

NUCLEAR REACTIONS ⁴⁰Ca(⁹Be, ⁹Be), (⁹Be, ⁹Be'), E=45, 60 MeV; analyzed data; ⁴⁰Ca levels deduced β. Frahn scaling formula, heavy ion scattering.

1980EN02      J.Phys.(London) G6, 1553 (1980)

J.B.A.England, T.R.Ophel, A.Johnston, A.F.Zeller

The ⁵⁴Fe(d, t)⁵³Fe Reaction and the Neutron Configuration in ⁵⁴Fe

NUCLEAR REACTIONS ⁵⁴Fe(d, t), E=18 MeV; measured σ(Et, θt). ⁵³Fe deduced levels, S. DWBA analysis.

doi: 10.1088/0305-4616/6/12/010
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1980KE10      Aust.J.Phys. 33, 197 (1980)

K.W.Kemper, T.R.Ophel

The Non-Statistical Population of the 11.10 MeV (4^-) State in ¹⁶O by ¹²C(⁶Li, d)

NUCLEAR REACTIONS ¹²C(⁶Li, d), E=35.5 MeV; measured σ(θ, Ed). ¹⁶O level deduced nonstatistical population mechanism. Compound nucleus calculations.

doi: 10.1071/PH800197a
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1980KE12      Nucl.Phys. A348, 339 (1980)

K.W.Kemper, A.F.Zeller, T.R.Ophel

Final-State Spins of ⁴⁹Sc from the ⁴⁸Ca(⁷Li, ⁶He) Reaction

NUCLEAR REACTIONS ⁴⁸Ca(⁷Li, ⁶He), E=34 MeV; measured σ(θ). ⁴⁹Sc levels deduced J, S, single-particle centroids.

doi: 10.1016/0375-9474(80)90341-3
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1980ZE02      Nucl.Phys. A344, 307 (1980)

A.F.Zeller, K.W.Kemper, T.R.Ophel, A.Johnston

Selective Population of Three-Particle States at High Excitation Energies in ¹⁵N

NUCLEAR REACTIONS ¹²C(⁷Li, α), E=48 MeV; measured σ(Eα). ¹⁵N deduced levels, J, π, Γ, configuration.

doi: 10.1016/0375-9474(80)90680-6
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1979CL10      Aust.J.Phys. 32, 283 (1979)

P.D.Clark, A.Johnston, T.R.Ophel

Widths of the 14.32 and 14.40 MeV Levels in ¹⁶O

NUCLEAR REACTIONS ¹⁴N(α, d), E=30 MeV; measured σ(Ed). ¹⁶O levels deduced Γ.

doi: 10.1071/PH790283
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
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1979KO20      Phys.Rev. C20, 1305 (1979)

D.G.Kovar, D.F.Geesaman, T.H.Braid, Y.Eisen, W.Henning, T.R.Ophel, M.Paul, K.E.Rehm, S.J.Sanders, P.Sperr, J.P.Schiffer, S.L.Tabor, S.Vigdor, B.Zeidman, F.W.Prosser, Jr.

Systematics of Carbon- and Oxygen-Induced Fusion on Nuclei with 12 ≤ A ≤ 19

NUCLEAR REACTIONS ¹²C(¹²C, X), E(cm)=7.4-31.2 MeV; ¹²C(¹³C, X), E(cm)=7.6-24.9 MeV; ¹²C(¹⁴N, X), E(cm)=15.1-24.0 MeV; ¹²C(¹⁵N, X), E(cm)=8.9-26.7 MeV; ¹²C(¹⁶O, X), E(cm)=12.9-27.0 MeV; ¹²C(¹⁸O, X), E(cm)=11.9-28.0 MeV; ¹²C(¹⁹F, X), E(cm)=11.6-27.1 MeV; ¹⁶O(¹⁶O, X), E(cm)=16.9-36.0 MeV; measured fusion σ(E); deduced fusion barrier parameters.

doi: 10.1103/PhysRevC.20.1305
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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
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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
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1978FR04      Nucl.Phys. A294, 161 (1978)

A.D.Frawley, K.H.Bray, T.R.Ophel

Energy Levels of ¹⁶O Near 15 MeV Excitation from ¹⁵N + p Reactions

NUCLEAR REACTIONS ¹⁵N(p, p), (p, α), E=2.88-3.64 MeV; measured σ(E, θ). ¹⁶O deduced levels, J, π, Γ. Enriched target.

doi: 10.1016/0375-9474(78)90401-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0460.

1978KE05      J.Phys.(London) G4, L17 (1978)

K.W.Kemper, A.F.Zeller, T.R.Ophel

Location of the Major 2p₁/₂ Strength in ⁴⁹Sc by Forward-Angle Heavy-Ion j Dependence

NUCLEAR REACTIONS ⁴⁸Ca(⁷Li, ⁶He), E=34 MeV; measured σ(θ). ⁴⁹Sc level deduced configuration.

doi: 10.1088/0305-4616/4/2/002
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1978KO01      Phys.Rev. C17, 83 (1978)

D.G.Kovar, W.Henning, B.Zeidman, Y.Eisen, J.R.Erskine, H.T.Fortune, T.R.Ophel, P.Sperr, S.E.Vigdor

¹⁶O + ⁴⁸Ca Reaction at 56 Mev. I. Transitions to Resolved Levels

NUCLEAR REACTIONS ⁴⁸Ca(¹⁶O, ¹⁶O), (¹⁶O, ¹⁶O'), (¹⁶O, ¹⁷O), (¹⁶O, ¹⁸O), (¹⁶O, ¹⁴N), ⁴⁸Ca(¹⁶O, ¹⁵N), (¹⁶O, ¹⁶N), (¹⁶O, ¹³C), (¹⁶O, ¹⁴C), (¹⁶O, ¹⁵C), (¹⁶O, ¹⁹O), ⁴⁸Ca(¹⁶O, ¹⁷N), (¹⁶O, ¹²C), (¹⁶O, ¹¹B), (¹⁶O, ¹²B), (¹⁶O, ¹³B), E=56 MeV; measured σ(θ); deduced optical model parameters. ^51,50Ti, ¹⁸O, ⁵⁰Sc, ⁵¹V, ⁴⁸Sc, ⁴⁹Ti levels deduced reaction population.

doi: 10.1103/PhysRevC.17.83
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1978ME02      Phys.Rev. C17, 56 (1978)

L.Meyer-Schutzmeister, R.E.Segel, K.Raghunathan, P.T.Debevec, W.R.Wharton, L.L.Rutledge, T.R.Ophel

Giant Electric Resonances in ⁵⁸Ni Studied by Alpha Particle Capture

NUCLEAR REACTIONS ⁵⁴Fe(α, γ), E=7.6-12.8 MeV; measured σ(E, Eγ). ⁵⁸Ni giant resonances deduced E1, E2 strength.

doi: 10.1103/PhysRevC.17.56
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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
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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
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1978ZE06      J.Phys.(London) G4, 1607 (1978)

A.F.Zeller, T.R.Ophel, D.C.Weisser

Spin Assignments of Levels in ⁶⁵Ga by Forward-Angle j Dependence

NUCLEAR REACTIONS ⁶⁴Zn(⁷Li, ⁶He), E=36 MeV; measured σ(E(⁶He), θ). ⁶⁵Ga levels deduced J, π, configuration.

doi: 10.1088/0305-4616/4/10/010
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1977BR32      Nucl.Phys. A288, 334 (1977)

K.H.Bray, A.D.Frawley, T.R.Ophel, F.C.Barker

Levels of ¹⁶O Near 13 MeV Excitation from ¹⁵N + p Reactions

NUCLEAR REACTIONS ¹⁵N(p, α₀), ¹⁵N(p, αγ), E=0.9-1.25 MeV; measured σ(Ep, θ), Doppler profiles. ¹⁶O deduced levels, J, π, Γ. Enriched target.

doi: 10.1016/0375-9474(77)90139-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0710.

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
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1976BR34      Aust.J.Phys. 29, 139 (1976)

D.Branford, L.E.Carlson, F.C.P.Huang, N.Gardner, T.R.Ophel, I.F.Wright

A Search for an Excited Kπ = 0⁺ Rotational Band in ²⁴Mg

NUCLEAR REACTIONS ¹²C(¹⁶O, α), E=28.86, 34.81 MeV; measured DSA, αγ-, γγ-coin. ²³Na(p, γ); measured σ(E, Eγ, θ), γγ-coin. ²⁴Mg deduced levels, T_1/2, J, π, γ-branching.

doi: 10.1071/PH760139
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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
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1976OP02      Nucl.Phys. A273, 397 (1976)

T.R.Ophel, A.D.Frawley, P.B.Treacy, K.H.Bray

A Remeasurement of the ¹²C(α, γ₀) Excitation Function in the Vicinity of the 12.44 and 13.1 MeV Levels of ¹⁶O

NUCLEAR REACTIONS ¹²C(α, γ), E=6.5-8.5 MeV; measured σ(E, Eγ). ¹⁶O deduced resonance. Enriched target.

doi: 10.1016/0375-9474(76)90599-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0709.

1976SP03      Phys.Rev.Lett. 36, 405 (1976)

P.Sperr, S.Vigdor, Y.Eisen, W.Henning, D.G.Kovar, T.R.Ophel, B.Zeidman

Oscillations in the Excitation Function for Complete Fusion of ¹⁶O + ¹²C

NUCLEAR REACTIONS ¹²C(¹⁶O, X), E(cm)=13-27 MeV; measured total fusion σ(E).

doi: 10.1103/PhysRevLett.36.405
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1975BR21      Aust.J.Phys. 28, 235 (1975)

K.H.Bray, A.D.Frawley, T.R.Ophel, P.B.Treacy

⁶Li(d, d'): Direct Breakup Effects and Parameters of the First 2⁺ Level of ⁶Li

NUCLEAR REACTIONS ⁶Li(d, d'), E=20, 25 MeV; measured σ(Ed'). ⁶Li deduced level parameters.

doi: 10.1071/PH750235
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1973CA38      Part.Nucl. 6, 76 (1973)

L.E.Carlson, D.Branford, F.C.P.Huang, T.R.Ophel

The 1522 keV Transition in ²⁸Si

NUCLEAR REACTIONS ²⁷Al(p, γ), E=1025 keV; measured γγ(θ). ²⁸Si level deduced γ-mixing.

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
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1973MA03      Nucl.Phys. A202, 257 (1973)

P.Martin, T.R.Ophel

Excited States of ¹⁶O between 13.5 and 15.0 MeV

NUCLEAR REACTIONS ¹²C(α, α₀), ¹²C(α, α'), E=8.5-10.5 MeV; measured σ(Eα;θ). ¹⁶O deduced resonances, J, π, level-width. Natural target.

doi: 10.1016/0375-9474(73)90222-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0983.

1972MA53      Nucl.Phys. A194, 491 (1972)

P.Martin, T.R.Ophel

A Search for an 8⁺ Level in ¹⁶O with the ¹²C(α, ⁸Be)⁸Be Reaction

NUCLEAR REACTIONS ¹²C(α, ⁸Be), E=15.0-18.96 MeV; measured σ(Eα;θ). ¹⁶O deduced levels. Natural target.

doi: 10.1016/0375-9474(72)90997-9
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0857.

1971OP01      Nucl.Phys. A173, 609 (1971)

T.R.Ophel, Ph.Martin, S.D.Cloud, J.M.Morris

Energy Levels of ¹⁶O in the Region of Excitation between 13.5 and 15.0 MeV

NUCLEAR REACTIONS ¹²C(α, α₀), ¹²C(α, α'), ¹²C(α, α'γ), ¹²C(α, p), Eα=8.5-10.5 MeV; measured σ(Eα;θ), Doppler profiles. ¹⁶O deduced levels, J, π, level-width. Natural target.

doi: 10.1016/0375-9474(71)90975-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0983.

1970OP01      Phys.Lett. 32B, 101 (1970)

T.R.Ophel, S.D.Cloud, P.Martin, J.M.Morris

A 6⁺ Level in ¹⁶O

NUCLEAR REACTIONS ¹²C(α, α), (α, α'), E=8.5-10.5 MeV; measured σ(E;θ). ¹⁶O deduced resonance.

doi: 10.1016/0370-2693(70)90597-6
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1969CL07      Nucl.Phys. A136, 592 (1969)

S.D.Cloud, T.R.Ophel

The 1080 keV Resonance of the ¹⁵N(p, αγ) Reaction

NUCLEAR REACTIONS ¹⁵N(p, αγ), E = 898-1640 keV; measured σ(E;Eγ, θ(αγ)). ¹⁶O deduced resonances, J, π. Ge(Li) detector.

doi: 10.1016/0375-9474(69)90130-4
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1969HU15      Nucl.Phys. A135, 647 (1969)

F.C.P.Huang, T.R.Ophel

Resonances of the ²⁶Mg(p, γ) Reaction Between 660 and 1000 keV

NUCLEAR REACTIONS ²⁶Mg(p, γ), E = 0.66-1.0 MeV; measured σ(E;Eγ, θ). ²⁷Al deduced levels, J. Isotopic target. Ge(Li) detector.

doi: 10.1016/0375-9474(69)90010-4
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1969HU16      Nucl.Instr.Methods 68, 141 (1969)

F.C.P.Huang, C.H.Osman, T.R.Ophel

Line Shape Analysis of Spectra Obtained with Ge(Li) Detectors

NUCLEAR REACTIONS ¹⁹F(p, αγ), E not given; ²⁶Mg(p, γ), E not given; measured σ(E;Eγ); deduced Iγ. Ge(Li) detector; line shape analysis. ²⁷Al deduced γ-branching.

doi: 10.1016/0029-554X(69)90701-0
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1969MO32      Nucl.Instr.Methods 68, 344 (1969)

J.M.Morris, T.R.Ophel

A Method of Measuring (p, n) Thresholds for the Calibration of Beam Analyzing Systems

NUCLEAR REACTIONS ¹¹B, ¹³C(p, n), E not given; measured thresholds.

doi: 10.1016/0029-554X(69)90246-8
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1968EL05      Nucl.Phys. A115, 673(1968)

R.V.Elliott, T.R.Ophel, R.H.Spear

Branching Ratios of ²⁷Al Bound States

NUCLEAR REACTIONS ²⁴Mg(α, pγ), E = 9.0 MeV; ²⁷Al(p, p'γ), E = 5.8, 7.0 MeV; measured Eγ, Iγ. ²⁷Al levels deduced γ-branching. Enriched target.

doi: 10.1016/0375-9474(68)90758-6
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1968MO08      Nucl.Phys. A112, 97(1968)

J.M.Morris, G.W.Kerr, T.R.Ophel

Energy Levels of ¹⁶O in the Vicinity of 13 MeV

NUCLEAR REACTIONS ¹²C(α, α₀), E=6.6-8.5 MeV; measured σ(Eα, θ). ¹⁶O deduced levels, J, π, level-width. Natural target.

doi: 10.1016/0375-9474(68)90222-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1041.

1965MI05      Nucl.Phys. 66, 553(1965)

I.V.Mitchell, T.R.Ophel

Energy Levels of O¹⁶ in the Vicinity of 13 MeV (II)

NUCLEAR REACTIONS ¹²C(α, γ₀), (α, γγ), (α, p), (α, α'). E = 7.7-8.4 MeV; measured σ(α, γ₀), (α, γγ), (α, p)(E), σ(α, α')(E, θ). ¹⁶O deduced levels, J, π, level-width. Natural target.

doi: 10.1016/0029-5582(65)90784-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1051.

1965OP01      Proc.Phys.Soc.(London) 85, 1093 (1965)

T.R.Ophel, D.R.Osgood

The 992 keV Resonance of the ²⁷Al(p, γ) Reaction

NUCLEAR STRUCTURE ²⁸Si; measured not abstracted; deduced nuclear properties.

doi: 10.1088/0370-1328/85/6/306
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1964MI12      Nucl.Phys. 58, 529(1964)

I.V.Mitchell, T.R.Ophel

Energy Levels of O¹⁶ in the Vicinity of 13 MeV

NUCLEAR REACTIONS ¹²C(α, γ), (α, α'γ), Eα=6.9-8.2 MeV; measured Eγ, α, γ(θ, E). ¹²C, ¹⁶O deduced levels, J, π. Enriched target.

doi: 10.1016/0029-5582(64)90565-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF1051.

1964OP01      Nucl.Phys. 52, 417 (1964)

T.R.Ophel, B.T.Lawergren

The Low-Lying Levels of Al²⁷ (I)

NUCLEAR STRUCTURE ²⁷Al; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(64)90704-7
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1963OP01      Phys.Letters 6, 230 (1963)

T.R.Ophel, B.D.Lawergren

The Decay of Mg²⁷

NUCLEAR STRUCTURE ²⁷Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(63)90555-9
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1962LA04      Proc.Phys.Soc.(London) 79, 881 (1962)

B.T.Lawergren, T.R.Ophel

NUCLEAR STRUCTURE ²⁷Al; measured not abstracted; deduced nuclear properties.

1962LA17      Phys.Letters 2, 265 (1962)

B.T.Lawergren, T.R.Ophel

The 2.21 MeV Level of Al²⁷

NUCLEAR STRUCTURE ²⁷Al; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(62)90029-X
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1962OP02      Nuclear Phys. 30, 215 (1962)

T.R.Ophel, B.T.Lawergren

The 721, 809, 839 and 954 keV Resonances of the Mg²⁶(p, γ) Reaction

NUCLEAR STRUCTURE ²⁷Al; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90045-7
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1962OP03      Nuclear Phys. 33, 198 (1962)

T.R.Ophel, R.N.Glover, E.W.Titterton

Gamma Ray Yields from the Proton Bombardment of B¹⁰

NUCLEAR STRUCTURE ¹⁰B; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90518-7
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1962OP04      Phys.Letters 2, 167 (1962)

T.R.Ophel, B.T.Lawergren

The 661 keV Resonance of the Mg²⁶(p, γ) Reaction

NUCLEAR STRUCTURE ²⁷Al; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(62)90071-9
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1961BA37      Australian J.Phys. 14, 335 (1961)

S.Bashkin, T.R.Ophel

NUCLEAR STRUCTURE ²⁸Mg, ²⁸Si; measured not abstracted; deduced nuclear properties.

1960HW01      Phys.Rev. 119, 352 (1960)

C.F.Hwang, T.R.Ophel, E.H.Thorndike, R.Wilson

Depolarization and Time Reversal in p-p Scattering at 142 MeV

doi: 10.1103/PhysRev.119.3520
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1960TH03      Phys.Rev. 119, 362 (1960)

E.H.Thorndike, T.R.Ophel

Proton-Proton Depolarization at 98 MeV

doi: 10.1103/PhysRev.119.362
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1958OP02      Proc.Phys.Soc.(London) 71, 389 (1958)

T.R.Ophel, I.F.Wright

Photodisintegration of Sodium by ⁷Li(p, γ) Radiation

doi: 10.1088/0370-1328/71/3/312
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1958OP29      Proc.Phys.Soc.(London) 72, 321 (1958)

T.R.Ophel