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NSR database version of April 11, 2024.

Search: Author = C.L.Woods

Found 25 matches.

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1989BA60      Aust.J.Phys. 42, 233 (1989)

F.C.Barker, C.L.Woods

Investigation of E1 Strength in Coulomb Excitation of Light Nuclei

NUCLEAR STRUCTURE 6,7Li, 10,11B, 12C, 17O; calculated E1 strength contribution to Coulomb excitation. Shell model.


1989CA25      Nucl.Phys. A503, 263 (1989)

W.N.Catford, L.K.Fifield, N.A.Orr, C.L.Woods

Study of 19N and 21O by Multinucleon Transfer

NUCLEAR REACTIONS 18O(18O, 17F), (18O, 15O), E=117 MeV; measured σ(E(17F)), σ(E(15O)). 19N, 21O deduced levels. Enriched targets. Shell model comparison.

NUCLEAR STRUCTURE 17,19N, 19,21O; calculated levels. Shell model.

doi: 10.1016/0375-9474(89)90264-9
Citations: PlumX Metrics


1989DR03      Nucl.Phys. A496, 530 (1989)

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

The 40Ar(13C, 14O)39S Reaction and the Ground-State Mass of 39S

NUCLEAR REACTIONS 40Ar(13C, 14O), (13C, 15O), (13C, 12C), E=96 MeV; measured σ(E(14O)), σ(E(15O)), σ(E(12C)); deduced reaction mechanism, Q. 39S deduced mass excess, excited state. DWBA calculations. Gas target.

doi: 10.1016/0375-9474(89)90075-4
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


1989OR04      Nucl.Phys. A491, 457 (1989)

N.A.Orr, L.K.Fifield, W.N.Catford, C.L.Woods

Reaction Studies of the Neutron-Rich Nuclei 22,23F

NUCLEAR REACTIONS 22Ne(7Li, 7Be), (18O, 17F), E=54-108 MeV. 22,23F deduced ground state mass excess, levels. Enriched targets.

doi: 10.1016/0375-9474(89)90579-4
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
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


1988WO02      Nucl.Phys. A476, 392 (1988)

C.L.Woods, W.N.Catford, L.K.Fifield, N.A.Orr, R.J.Sadleir

Studies of the T(z) = (5/2) Nuclei 31Al and 29Mg

NUCLEAR REACTIONS 30Si(18O, 17F), E=100 MeV; 30Si(13C, 14O), E=93 MeV; measured σ(E(17F)), σ(E(14O)). 31Al deduced ground state mass excess. 31Al, 29Mg deduced levels, L. Enriched targets.

doi: 10.1016/0375-9474(88)90490-3
Citations: PlumX Metrics


1988WO07      Nucl.Phys. A484, 145 (1988)

C.L.Woods, W.N.Catford, L.K.Fifield, N.A.Orr

A Measurement of the Mass of 39Sc

NUCLEAR REACTIONS 40Ca(14N, 15C), E=102.5 MeV; measured σ(E(15C)). 39Sc deduced level, J, π, analog character, mass excess, levels. Enriched target.

doi: 10.1016/0375-9474(88)90146-7
Citations: PlumX Metrics


1988WO10      Aust.J.Phys. 41, 525 (1988)

C.L.Woods, F.C.Barker, W.N.Catford, L.K.Fifield, N.A.Orr

Experimental Investigation and R-Matrix Analysis of Low-Lying Levels in 5He and 5Li

NUCLEAR REACTIONS 4He(7Li, 6Li), (7Li, 6He), E=50 MeV; 6Li(12C, 13N), (13C, 14C), E=90 MeV; measured σ(θ). 5He, 5Li levels deduced reduced widths, spectroscopic factors. R-matrix analysis.

doi: 10.1071/PH880525
Citations: PlumX Metrics


1986FI06      Nucl.Phys. A453, 497 (1986)

L.K.Fifield, C.L.Woods, W.N.Catford, R.A.Bark, P.V.Drumm, K.T.Keoghan

The Mass of 35Si

NUCLEAR REACTIONS 34,36S(13C, 14O), E=91 MeV; measured σ(E(14O)). 35Si deduced mass excess. 33Si deduced energy levels. Enriched targets.

doi: 10.1016/0375-9474(86)90449-5
Citations: PlumX Metrics


1986WO02      Nucl.Phys. A451, 413 (1986)

C.L.Woods

Shell-Model Calculations for Neutron-Rich Nuclei with A = 35-41

NUCLEAR STRUCTURE 36,37S, 35P, 38Ar; calculated levels, single nucleon transfer spectroscopic factors. 39Ar; calculated levels, single nucleon spectroscopic factors, δ. 41,40Ar, 38,37Cl; calculated levels, single nucleon spectroscopic factors, average T1/2. 40,41Cl, 38,39S, 36,37P, 35,36Si; calculated levels. Shell model.

doi: 10.1016/0375-9474(86)90068-0
Citations: PlumX Metrics


1985BA68      Aust.J.Phys. 38, 563 (1985)

F.C.Barker, C.L.Woods

States of 5He and 5Li

NUCLEAR STRUCTURE 5He, 5Li; calculated levels, spectroscopic factors, Γ. Shell model.

doi: 10.1071/PH850563
Citations: PlumX Metrics


1985DR06      Nucl.Phys. A441, 95 (1985)

P.V.Drumm, L.K.Fifield, R.A.Bark, M.A.C.Hotchkis, C.L.Woods, P.Maier-Komor

Ground-State Mass Excesses and Low-Lying Levels of the Neutron-Rich Nuclei 36P, 35P and 34P

NUCLEAR REACTIONS 36,34S(7Li, 7Be), 36S(6Li, 7Be), E=52 MeV; 36,34S(11B, 11C), E=83 MeV; measured σ(E(7Be)), σ(E(11C)). 36,35,34P deduced mass excess, levels. Enriched targets.

doi: 10.1016/0375-9474(85)90169-1
Citations: PlumX Metrics


1985FI03      Nucl.Phys. A440, 531 (1985)

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

Masses and Level Schemes of 33Si and 34Si

NUCLEAR REACTIONS 36S(11B, 13N), (11B, 14N), E=83 MeV; measured σ(E(13N)), σ(E(14N)). 33,34Si deduced ground-state mass excesses, levels. Enriched targets.

doi: 10.1016/0375-9474(85)90244-1
Citations: PlumX Metrics


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


1985LE17      Nucl.Phys. A443, 210 (1985)

P.M.Lewis, A.R.Poletti, M.J.Savage, C.L.Woods

The Mean Life of the Second 0+ State in 42Ca

NUCLEAR REACTIONS 42Ca(p, p'γ), E=5 MeV; measured pγ-coin. 42Ca level deduced T1/2, B(E2). Enriched target, direct electronic timing.

doi: 10.1016/0375-9474(85)90260-X
Citations: PlumX Metrics


1985VE02      Phys.Rev.Lett. 54, 1129 (1985)

M.C.Vetterli, J.A.Kuehner, A.J.Trudel, C.L.Woods, R.Dymarz, A.A.Pilt, H.R.Weller

Measurement of T20 for the Reaction 1H(d(pol), γ)3He and D-State Effects in 3He

NUCLEAR REACTIONS 1H(polarized d, γ), E=19.8 MeV; measured tensor analyzing power T20(θ). 3He deduced D-state effects.

doi: 10.1103/PhysRevLett.54.1129
Citations: PlumX Metrics


1985WI18      Nucl.Phys. A437, 65 (1985)

J.S.Winfield, N.A.Jelley, W.D.M.Rae, C.L.Woods

Spectroscopic-Factor Discrepancies in (9Be, 10B) For Different Ejectile Excitations

NUCLEAR REACTIONS 63Cu, 54Fe, 26,24Mg, 16O(9Be, 10B), 26Mg, 16O(9Be, 9Be), E=43 MeV; 40Ca(9Be, 10B), (9Be, 9Be), E=30, 45 MeV; measured σ(θ). 62Ni, 53Mn, 25,23Na, 15N, 39K levels deduced spectroscopic factors. Magnetic spectrometer, ΔE counter telescope.

doi: 10.1016/0375-9474(85)90227-1
Citations: PlumX Metrics


1985WO04      Nucl.Phys. A437, 454 (1985)

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

A Study of 25Ne via the 26Mg(13C, 14O)25Ne Reactions

NUCLEAR REACTIONS 24,26Mg(13C, 14O), E=96 MeV; measured σ(E(14O)). 25Ne deduced mass excess, levels. Enriched target.

doi: 10.1016/0375-9474(85)90101-0
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1521.


1984WO09      Nucl.Phys. A427, 73 (1984)

C.L.Woods, F.C.Barker

Narrow Highly Excited States of 9Be

NUCLEAR REACTIONS 9Be(e, e'), E not given; calculated transverse form factors. 9Be levels deduced B(λ), Γγ, Γ, spectroscopic factors. Shell model, special p-shell interactions.

doi: 10.1016/0375-9474(84)90139-8
Citations: PlumX Metrics


1983WO06      Nucl.Phys. A402, 31 (1983)

C.L.Woods, J.A.Kuehner, A.A.Pilt, A.J.Trudel, M.C.Vetterli

Spin-Parity Assignments for 66Cu Levels via the 68Zn(d(pol), α)66Cu Reaction

NUCLEAR REACTIONS 68Zn(polarized d, α), E=9, 9.5, 10, 10.5 MeV; measured T20(θ=4°). 66Cu levels deduced J, π. Enriched target.

doi: 10.1016/0375-9474(83)90560-2
Citations: PlumX Metrics


1982WO09      J.Phys.(London) G8, 1699 (1982)

C.L.Woods, B.A.Brown, N.A.Jelley

A Comparison of Woods-Saxon and Doubled-Folding Potentials for Lithium Scattering from Light Target Nuclei

NUCLEAR REACTIONS 12C, 16O, 26Mg(6Li, 6Li), E=36 MeV; 15N(7Li, 7Li), E=28.8 MeV; 25Mg(7Li, 7Li), E=27 MeV; 12C(6Li, 6Li'), E=36 MeV; calculated σ(θ); deduced potential dependence. Woods-Saxon, double folding potentials, optical model, DWBA analyses.

doi: 10.1088/0305-4616/8/12/012
Citations: PlumX Metrics


1980WO05      J.Phys.(London) G6, L187 (1980)

C.L.Woods, N.A.Jelley, A.A.Pilt, J.S.Winfield

Is the (6Li, 7Be)Reaction a Useful Spectroscopic Tool (Question)

NUCLEAR REACTIONS 26Mg(6Li, 7Be), (6Li, 6Li), (6Li, 6Li'), E=36 MeV; measured σ(θ). 26Mg level deduced β2. 25Na level deduced C2S; DWBA.

doi: 10.1088/0305-4616/6/11/002
Citations: PlumX Metrics


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