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Search: Author = C.L.Woods

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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 T_1/2. ^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 T_1/2, 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
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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
Citations: PlumX Metrics

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