NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = W.G.Davies Found 59 matches. 1996HO19 Phys.Rev.Lett. 77, 2408 (1996) D.Horn, G.C.Ball, D.R.Bowman, W.G.Davies, D.Fox, A.Galindo-Uribarri, A.C.Hayes, G.Savard, L.Beaulieu, Y.Larochelle, C.St-Pierre Pionic Fusion of Heavy Ions NUCLEAR REACTIONS 12C(12C, X), E(cm)=137 MeV; measured pionic fusion associated σ.
doi: 10.1103/PhysRevLett.77.2408
1987KO34 Nucl.Phys. A472, 419 (1987) V.T.Koslowsky, J.C.Hardy, E.Hagberg, R.E.Azuma, G.C.Ball, E.T.H.Clifford, W.G.Davies, H.Schmeing, U.J.Schrewe, K.S.Sharma The Precise Determination of Q(EC)-Value Differences between Four Pairs of Superallowed β-Emitters: 14O and 26mAl, 26mAl and 42Sc, 42Sc and 54Co, 50Mn and 54Co NUCLEAR REACTIONS 14N, 26Mg(3He, t), E=25 MeV; 50Cr, 54Fe(3He, t), E=29 MeV; 26Mg, 42Ca(3He, t), E=18.86 MeV; 42Ca, 54Fe(3He, t), E=18.89 MeV; measured triton energy differences; deduced Q-value differences. 14O, 26mAl, 42Sc, 54Co, 50Mn deduced Q(EC) differences. Q3D spectrometer, enriched composite targets, high voltage target assembly.
doi: 10.1016/0375-9474(87)90041-8
1987WA21 Nucl.Phys. A470, 339 (1987) R.E.Warner, B.A.Vaughan, J.A.Ditusa, J.W.Rovine, R.S.Wakeland, C.P.Browne, S.E.Darden, S.Sen, A.Nadasen, A.Basak, T.R.Donoghue, T.Rinckel, K.Sale, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster The Mechanism of the 7Li(d, 2α)n Reaction from E(d) = 3 to 15 MeV NUCLEAR REACTIONS, MECPD 7Li(d, 2α), E=3-15 MeV; measured σ(θ1, θ2) vs energy difference; deduced reaction mechanism. 8Be deduced levels. Enriched 7LiF targets.
doi: 10.1016/0375-9474(87)90006-6
1984RO04 Phys.Rev. C29, 755 (1984) R.G.H.Robertson, P.Dyer, R.C.Melin, T.J.Bowles, A.B.McDonald, G.C.Ball, W.G.Davies, E.D.Earle Upper Limit on the Isovector Parity-Violating Decay Width of the 0+ T = 1 State of 6Li NUCLEAR REACTIONS, ICPND 2H(α, γ), E=6.24 MeV; measured capture σ. 6Li level deduced isovector parity violating decay Γ upper limit.
doi: 10.1103/PhysRevC.29.755
1982AL15 Phys.Lett. 113B, 132 (1982) T.K.Alexander, G.C.Ball, W.G.Davies, J.S.Forster, I.V.Mitchell, H.-B.Mak Lifetime Measurements of Levels in 26Si and the Ratio of Neutron to Proton Transition Amplitudes for Mirror Nuclei NUCLEAR REACTIONS 3He(24Mg, n), E=50 MeV; measured γγ-coin, DSA. 26Si levels deduced T1/2, B(E2), neutron to proton transition matrix elements. 18O, 26Mg transitions deduced isocalar transition strengths, neutron to proton transition matrix elements. Electromagnetic transition, pion scattering data input.
doi: 10.1016/0370-2693(82)90409-9
1982AL22 Phys.Rev.Lett. 49, 438 (1982) T.K.Alexander, G.C.Ball, J.S.Forster, W.G.Davies, I.V.Mitchell, H.-B.Mak Lifetimes of Levels of 30S and the Variation of E2 Transition Strengths with T(z) and A NUCLEAR REACTIONS 3He(28Si, n), E=60 MeV; measured DSA. 30S levels deduced T1/2. 30Si, 30P, 30S deduced E2 transition strength vs T(z), mass.
doi: 10.1103/PhysRevLett.49.438
1982BA06 Nucl.Phys. A377, 268 (1982) G.C.Ball, T.K.Alexander, W.G.Davies, J.S.Forster, I.V.Mitchell A DBLA Measurement of the Lifetime of the First Excited Level in 18O and a Critical Comparison of Lifetime Results by Different Methods NUCLEAR REACTIONS 4He(18O, α), E=34 MeV; 1H(18O, p), E=47 MeV; measured DSA, (particle)γ-coin. 18O level deduced T1/2, B(E2).
doi: 10.1016/0375-9474(82)90333-5
1982BA40 Nucl.Phys. A386, 333 (1982) G.C.Ball, T.K.Alexander, W.G.Davies, J.S.Forster, I.V.Mitchell, J.Keinonen, H.B.Mak Lifetimes of Low-Lying Levels in 18F NUCLEAR REACTIONS 3He(16O, p), E=19.4 MeV; measured DSA, pγ-coin. 18F levels deduced T1/2.
doi: 10.1016/0375-9474(82)90116-6
1982KO28 Phys.Lett. 119B, 57 (1982) V.T.Koslowsky, J.C.Hardy, R.E.Azuma, G.C.Ball, E.T.H.Clifford, W.G.Davies, E.Hagberg, H.Schmeing, U.J.Schrewe, K.S.Sharma Fermi Beta-Decay: Precision Q-value doublet measurements by a new technique NUCLEAR REACTIONS 14N, 26Mg(3He, t), E not given; measured σ(Et, θ=0°), Q-value difference. 26mAl, 14O deduced superallowed β-decay Q(EC) difference, ft. Doublet technique.
doi: 10.1016/0370-2693(82)90242-8
1981HA08 Nucl.Phys. A357, 356 (1981) J.C.Hardy, G.C.Ball, W.G.Davies, J.S.Forster, H.Schmeing, E.T.H.Clifford A Precise P(K)/P(β+) Measurement at Z = 55 (I). The mass of 130Cs NUCLEAR REACTIONS 129,136Xe(3He, d), E=27 MeV; measured Q. 130Cs deduced levels, J, π, Q(EC), mass excess. 137Cs deduced mass excess. Natural enriched target.
doi: 10.1016/0375-9474(81)90226-8
1981KE04 Phys.Rev. C23, 2073 (1981) J.Keinonen, H.-B.Mak, T.K.Alexander, G.C.Ball, W.G.Davies, J.S.Forster, I.V.Mitchell Lifetime of the 1.04 MeV State in 18F, Measured through the Inverse Reaction 3He(16O, p)18F NUCLEAR REACTIONS 3He(16O, p), E=15.9 MeV; measured DSA, pγ-coin. 18F level deduced T1/2. He-ion implanted in thin Al, Nb, Zr foils, Ge(Li) detectors.
doi: 10.1103/PhysRevC.23.2073
1981RO12 Phys.Rev.Lett. 47, 1867 (1981); Erratum Phys.Rev.Lett. 75, 4334 (1995) R.G.H.Robertson, P.Dyer, R.A.Warner, R.C.Melin, T.J.Bowles, A.B.McDonald, G.C.Ball, W.G.Davies, E.D.Earle Observation of the Capture Reaction 2H(α, γ)6Li and Its Role in Production of 6Li in the Big Bang NUCLEAR REACTIONS 2H(α, γ), E(cm)=1, 1.33, 1.63, 2.08, 2.33, 3.01 MeV; measured σ(capture) vs E; deduced 6Li production role in big bang. Recoil 6Li ion detection, magnetic analysis.
doi: 10.1103/PhysRevLett.47.1867
1981TA24 Phys.Lett. 107B, 35 (1981) P.Taras, G.C.Ball, W.G.Davies, H.R.Andrews, B.Haas Evidence for Alpha-Cluster Structure at 12.9 MeV CM in the 12C + 16O System NUCLEAR REACTIONS 12C(16O, 12C), E(cm)=12.2-13.5 MeV; measured σ(θ) vs E, σ(E(12C)). 28Si resonance deduced J, π, Γ, α-cluster structure.
doi: 10.1016/0370-2693(81)91141-2
1981WA15 Nucl.Phys. A365, 142 (1981) R.E.Warner, G.C.Ball, W.G.Davies, J.S.Forster Double Spectator Poles Observed in a Double Coincidence Study of the 6Li + 6Li → 2α + 2d Reaction NUCLEAR REACTIONS 6Li(6Li, 2α), (6Li, 2d), E=36-47 MeV; measured σ(θ1, θ2, E1, E2); deduced reaction mechanisms. Isotopic target.
doi: 10.1016/0375-9474(81)90392-4
1980BA40 Nucl.Phys. A349, 271 (1980) G.C.Ball, O.Hausser, T.K.Alexander, W.G.Davies, J.S.Foster, I.V.Mitchell, J.R.Beene, D.Horn, W.McLatchie Electric Quadrupole Moments of the First Excited States of 28Si, 32S and 34S NUCLEAR REACTIONS 4He(32S, α), (34S, α), E=70 MeV; measured Doppler-broadened line shapes, αγ(t). 32,34S levels deduced T1/2. 208Pb(28Si, 28Si'), E=105 MeV; 208Pb(32S, 32S'), (34S, 34S'), E=122 MeV; measured σ(θ, E(28Si)), σ(θ, E(32S)), σ(θ, E(34S)), Coulomb excitation. 32,34S, 28Si level deduced static quadrupole moment, B(E2). Enriched targets.
doi: 10.1016/0375-9474(80)90454-6
1980WA10 Nucl.Phys. A341, 483 (1980) R.E.Warner, W.T.Conner, G.C.Ball, W.G.Davies, A.J.Ferguson Mechanism of the 6Li(6Li, 2α)α Reaction from 36 to 46 MeV NUCLEAR REACTIONS 6Li(6Li, 2α), E=36-46 MeV; measured αα-coin, σ(Eα1, Eα2); deduced reaction mechanism. 8Be deduced levels. Isotopic target.
doi: 10.1016/0375-9474(80)90379-6
1979AL01 Nucl.Phys. A313, 425 (1979) T.K.Alexander, G.C.Ball, W.G.Davies, J.S.Forster Lifetime of the 6+ Member of the Ground-State in 22Ne NUCLEAR REACTIONS 4He(19F, pγ), E=41 MeV; measured pγ-coin, Doppler-shift attenuation. 22Ne levels deduced T1/2, B(λ).
doi: 10.1016/0375-9474(79)90510-4
1979BA31 Nucl.Phys. A325, 305 (1979) G.C.Ball, W.G.Davies, J.S.Forster, H.R.Andrews, D.Horn, W.McLatchie The Use of Exotic Heavy Ion Transfer Reactions to Study Light Neutron Rich Nuclei NUCLEAR REACTIONS 207,208Pb(18O, 21O), (18O, 22O), (18O, 19N), (18O, 17O), E=93 MeV; measured position spectra; deduced Q. 21,22O, 19N, 17C deduced mass excess. Enriched targets, QD3 spectrometer analysis.
doi: 10.1016/0375-9474(79)90165-9
1979FO02 Nucl.Phys. A313, 397 (1979) J.S.Forster, T.K.Alexander, G.C.Ball, W.G.Davies, I.V.Mitchell, K.B.Winterbon Lifetime Measurements in 22Ne, 28Si and 31P Relevant to the Interpretation of the Z2 Variation in Low Velocity DSAM Results NUCLEAR REACTIONS 4He(19F, p), E=23.25, 28.5 MeV; 4He(28Si, α), (28Si, p), E=55 MeV; measured Doppler broadened lineshapes, particle-γ-coin. 22Ne, 28Si, 31P levels deduced T1/2.
doi: 10.1016/0375-9474(79)90509-8
1979WA02 Phys.Rev. C19, 293 (1979) R.E.Warner, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Search for αα* Rotational Levels in 8Be NUCLEAR REACTIONS 2H(6Li, α), E=10-31 MeV; measured σ(θ). 8Be deduced evidence for rotational band around 24-28 MeV excitation.
doi: 10.1103/PhysRevC.19.293
1979WA13 Nucl.Phys. A326, 209 (1979) R.E.Warner, D.C.Martin, G.C.Ball, W.G.Davies, A.J.Ferguson, D.Horn Double Spectator Poles and Quasi-Free Inelastic Scattering in the 6Li + 6Li → 2α + 2d Reaction NUCLEAR REACTIONS 6Li(6Li, d2α), (6Li, 2dα), E=45 MeV; observed triple coin energy spectra; deduced reaction mechanism. Isotopic target.
doi: 10.1016/0375-9474(79)90376-2
1978AL06 Phys.Lett. 74B, 183 (1978) T.K.Alexander, J.S.Forster, G.C.Ball, W.G.Davies, K.B.Winterbon Z1 and Z2 Variations in the Stopping Powers of Z1 = 10 to 18 Ions Deduced from DSAM Lifetime Measurements NUCLEAR STRUCTURE 22Ne, 22Na, 24Mg, 27Al, 30Si, 31P, 34S, 38Ar; analyzed T1/2 (level) data, stopping power effects.
doi: 10.1016/0370-2693(78)90548-8
1978RE06 Phys.Rev. C18, 1927 (1978) T.R.Renner, J.P.Schiffer, D.Horn, G.C.Ball, W.G.Davies Elastic Excitation Function of 12C on 40Ca at 180° NUCLEAR REACTIONS 40Ca(12C, 12C), E=135-150 MeV; measured σ(E), θ=180°.
doi: 10.1103/PhysRevC.18.1927
1977DA11 Phys.Rev.Lett. 38, 1119 (1977) W.G.Davies, G.C.Ball, A.J.Ferguson, J.S.Forster, D.Horn, R.E.Warner Search for High-Energy Deuterons in the 3He + 3He Reaction and the Solar Neutrino Problem NUCLEAR REACTIONS 3He(3He, d), E=15, 25 MeV; measured σ for production of high energy deuterons; deduced upper, lower σ limits.
doi: 10.1103/PhysRevLett.38.1119
1976BA03 Phys.Lett. 60B, 265 (1976) G.C.Ball, W.G.Davies, J.S.Forster, H.R.Andrews Use of the 208Pb(18O, 21O)205Pb Reaction to Measure the Mass of 21O NUCLEAR REACTIONS 208Pb(18O, 21O), (18O, 20O), E=93 MeV; measured σ(θ). 208Pb(18O, 21O) deduced Q. 21O deduced mass excess.
doi: 10.1016/0370-2693(76)90296-3
1976BR06 Phys.Rev. C13, 953 (1976) C.Broude, W.G.Davies, J.S.Forster, G.C.Ball Gamma-Emitting States in 22Ne NUCLEAR REACTIONS 19F(α, pγ), E=20.0 MeV; measured σ(E, Ep, Eγ, θ). 22Ne deduced levels, J, π, δ, γ-branching.
doi: 10.1103/PhysRevC.13.953
1976DA18 Nucl.Phys. A269, 477 (1976) W.G.Davies, R.M.DeVries, G.C.Ball, J.S.Forster, W.McLatchie, D.Shapira, J.Toke, R.E.Warner A Comparison of α-Transfer and α-Decay in the Lead Region NUCLEAR REACTIONS 204,207,208Pb, 209Bi(16O, 12C), E=93 MeV; measured σ(θ). 208,211,212Po, 213At levels deduced S, Γα. DWBA analysis, resolution 200 keV, θ=60-104°.
doi: 10.1016/0375-9474(76)90694-1
1976FO12 Phys.Rev. C14, 596 (1976) J.S.Forster, G.C.Ball, C.Broude, W.G.Davies, I.V.Mitchell Lifetimes from the Doppler Shift Attenuation Method Using High Velocity Recoils from the 4He(35Cl, p)38Ar Reaction NUCLEAR REACTIONS 4He(35Cl, p), E=55 MeV; measured DSA. 38Ar first excited state deduced T1/2. Implanted targets.
doi: 10.1103/PhysRevC.14.596
1976FO20 Nucl.Instrum.Methods 136, 349 (1976) J.S.Forster, D.Ward, H.R.Andrews, G.C.Ball, G.J.Costa, W.G.Davies, I.V.Mitchell Stopping Power Measurements for 19F, 24Mg, 27Al, 32S and 35Cl at Energies ≈0.2 to ≈3.5 MeV/Nucleon in Ti, Fe, Ni, Cu, Ag and Au NUCLEAR REACTIONS Ti, Fe, Ni, Cu, Ag(19F, X), (24Mg, X), (27Al, X), (32S, X), (35Cl, X), E ≈ 0.2-3.5 MeV/nucleon; measured stopping power.
doi: 10.1016/0029-554X(76)90218-4
1976WA12 Nucl.Phys. A269, 286 (1976) R.E.Warner, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Three-Body Final States of the 3He + 7Li Reaction and Clustering in 7Li NUCLEAR REACTIONS 7Li(3He, t3He), (3He, d3He), (3He, t6Li), (3He, 3He6Li), 7Li(3He, 3He6He), E=37.5 MeV; measured absolute coin σ(E1, θ1, θ2). Enriched target. Modified PWBA analysis. Cluster probabilities, momentum distributions.
doi: 10.1016/0375-9474(76)90681-3
1975DE22 Phys.Rev.Lett. 35, 835 (1975) R.M.DeVries, D.Shapira, W.G.Davies, G.C.Ball, J.S.Forster, W.McLatchie Inverse α Decay via the Reaction 208Pb(16O, 12C)212Po NUCLEAR REACTIONS 208Pb(16O, 12C), E=93 MeV; measured σ(E(12C), θ). 212Po levels deduced S.
doi: 10.1103/PhysRevLett.35.835
1975WA09 Nucl.Phys. A243, 189 (1975) R.E.Warner, S.B.Di Cenzo, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Final-State Interactions in the 2H(d, pp)nn Reaction NUCLEAR REACTIONS 2H(d, 2p), E=23.15 MeV; measured absolute σ(θ), pp-coin; deduced 2n, 2p relative energy spectra. Watson-Migdal, double distorted wave analysis. Enriched target.
doi: 10.1016/0375-9474(75)90243-2
1975WA31 Nucl.Phys. A255, 95 (1975) R.E.Warner, R.L.Ruyle, W.G.Davies, G.C.Ball, A.J.Ferguson, J.S.Forster Initial-State Distortion and Final-State Interactions in the 2H(3He, 3He p)n and 2H(3He, 3H p)p Reactions NUCLEAR REACTIONS 2H(3He, p3He), (3He, pt), E=35.9 MeV; measured absolute coin σ(E1, θ1, θ2). Enriched target. Antisymmetrized DWBA, PWBA-FSI analysis of present, previous 26.8, 35.9 MeV data for same reactions.
doi: 10.1016/0375-9474(75)90150-5
1974BA15 Phys.Lett. 49B, 33 (1974) G.C.Ball, J.G.Costa, W.G.Davies, J.S.Forster, J.C.Hardy, A.B.McDonald Use of the 14C(18O, 12Be)20Ne Reaction to Measure the Mass of 12Be NUCLEAR REACTIONS 12C(18O, 9Be), (18O, 10Be), E=80.0 MeV; 14C(18O, 9Be), (18O, 11Be), E=88.7 MeV; measured σ(E(9,10,11Be)). 12C(18O, 12Be); measured σ(E(12Be)), Q. 20,21,23Ne, 12Be deduced levels.
doi: 10.1016/0370-2693(74)90573-5
1974FO13 Phys.Lett. 51B, 133 (1974) J.S.Forster, D.Ward, G.J.Costa, G.C.Ball, W.G.Davies, I.V.Mitchell The Use of 4He Ion-Implanted Targets to Obtain Accurate Nuclear Lifetimes from Analysis of Doppler Broadened Lineshapes NUCLEAR REACTIONS 4He(24Mg, αγ), E=40 MeV; 4He(35Cl, pγ), E=55 MeV; measured DSA, αγ-coin, pγ-coin. 24Mg, 38Ar levels deduced T1/2.
doi: 10.1016/0370-2693(74)90197-X
1974MI13 Nucl.Phys. A228, 382 (1974) G.F.Millington, J.R.Leslie, W.McLatchie, G.C.Ball, W.G.Davies, J.S.Forster Hole States of 20F and 20Ne NUCLEAR REACTIONS 21Ne(d, 3He), E=26 MeV; measured σ(E(3He), θ). 20F deduced levels, L(p), J, π, S. 21Ne(d, t), E=26 MeV; measured σ(Et, θ). 20Ne deduced levelsln, J, π, S. Enriched 21Ne target.
doi: 10.1016/0375-9474(74)90609-5
1974RA19 Phys.Rev. C10, 632 (1974) K.Ramavataram, S.Ramavataram, W.G.Davies, A.J.Ferguson, J.S.Fraser Coulomb Excitation and Direct Inelastic Effects in the Decay of the 5- Analog Resonance in 208Bi NUCLEAR REACTIONS 207Pb(p, p), (p, p'), E=14-15.5 MeV; measured σ(E, θ), σ(E). 208Bi deduced IAR, p-width, S. 207Pb level deduced B(E2).
doi: 10.1103/PhysRevC.10.632
1974WA06 Nucl.Phys. A221, 593 (1974) R.E.Warner, S.A.Gottlieb, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Effects of Exchange and Final-State Interactions in the Reactions 2H(3He, 3H p)p and 2H(3He, 3He p)n NUCLEAR REACTIONS 2H(3He, 3Hep), (3He, pt), E=35.9 MeV; measured absolute coin σ(E1, θ(1), θ(2)). Enriched target.
doi: 10.1016/0375-9474(74)90485-0
1973BA34 Phys.Rev.Lett. 31, 395 (1973) G.C.Ball, G.J.Costa, W.G.Davies, J.S.Forster, J.C.Hardy, A.B.McDonald Mass Excess and Low-Lying Level Structure of 14B NUCLEAR REACTIONS 12,14C, 14N, 16O(7Li, 7Be), E=52 MeV; measured σ(E(7Be)).Q. 14B deduced levels, mass excess.
doi: 10.1103/PhysRevLett.31.395
1973HA02 Nucl.Phys. A199, 560 (1973) S.I.Hayakawa, S.K.Mark, J.K.Lee, J.E.Kitching, G.C.Ball, W.G.Davies Study of Low-Lying States in 92Tc with the 92Mo(3He, t) Reaction NUCLEAR REACTIONS 92Mo(3He, t), E=27.5 MeV; measured Q, σ(Et, θ). 92Tc deduced levels, J, π, mass excess, isobaric analog. Enriched target.
doi: 10.1016/0375-9474(73)90598-8
1973MO11 Z.Phys. 261, 155 (1973) D.G.Montague, K.Ramavataram, N.S.Chant, W.G.Davies, J.E.Kitching, W.McLatchie, J.M.Morton States in 86Sr, 84Sr and 87Y Populated in the (p, t) Reaction NUCLEAR REACTIONS 86,88Sr, 89Y(p, t), E=49.5 MeV; measured σ(Et, θ). 84,86Sr, 87Y deduced levels, J, π, L.
doi: 10.1007/BF01394557
1972BA15 Nucl.Phys. A182, 529 (1972) G.C.Ball, W.G.Davies, J.S.Forster, A.N.James, D.Ward Lifetimes of Levels in 38Ar NUCLEAR REACTIONS 35Cl(α, pγ), E=11.5 MeV; measured recoil distance, Doppler-shift attenuation. 38Ar levels deduced, mean T1/2. Enriched target.
doi: 10.1016/0375-9474(72)90532-5
1972BA35 Phys.Rev.Lett. 28, 1069 (1972); Erratum Phys.Rev.Lett. 28, 1497 (1972) G.C.Ball, W.G.Davies, J.S.Forster, J.C.Hardy Use of the (7Li, 7Be) Reaction to Measure the Mass of 26Na NUCLEAR REACTIONS 26Mg(7Li, 7Be), E=36 MeV; measured Q. 26Na deduced mass excess.
doi: 10.1103/PhysRevLett.28.1069
1972WA22 Nucl.Phys. A192, 341 (1972) R.E.Warner, G.R.Flierl, W.G.Davies, G.C.Ball, A.J.Ferguson, J.S.Forster, S.A.Gottlieb Coincidence Study and DWBA Analysis of the 3He+d → d+d+p Reaction NUCLEAR REACTIONS 2H(3He, dd)p, 2H(3He, dp)d, E=26.8 MeV; measured absolute coin σ(E1, θ(1), θ(2)); deduced reaction mechanisms. Enriched target.
doi: 10.1016/0375-9474(72)90264-3
1971FO02 Nucl.Phys. A161, 375 (1971) J.S.Forster, C.Broude, W.G.Davies Angular Correlation Measurements of the First Three Excited States in 29P NUCLEAR REACTIONS 32S(p, αγ), E=14.0 MeV; measured σ(Eα, Eγ, θ(γ), θ(αγ)). 29P deduced levels, γ-branching ratios, J, γ-mixing ratios. Natural target.
doi: 10.1016/0375-9474(71)90375-7
1971HA52 Priv.Comm. (December 1971) S.I.Hayakawa, S.K.Mark, J.K.P.Lee, J.E.Kitching, G.C.Ball, W.G.Davies
1971KI16 Nucl.Phys. A177, 433 (1971) J.E.Kitching, W.G.Davies, W.J.Darcey, W.McLatchie, J.Morton Effective Interaction among 1g9/2 and 2p1/2 Neutrons in the Strontium Isotopes NUCLEAR STRUCTURE 83,84,85,86,87Sr; calculated levels, one-nucleon S, wave functions. Effective interaction shell model.
doi: 10.1016/0375-9474(71)90302-2
1971MO02 Nucl.Phys. A161, 228 (1971) J.M.Morton, W.G.Davies, W.McLatchie, W.Darcey, J.E.Kitching The Level Structures of 85,87Sr from (d, p) Reactions NUCLEAR REACTIONS 84,86Sr(d, p), Ed=12.0 MeV; measured σ(Ep, θ) absolute; deduced Q. 85,87Sr deduced levels, J, L, π, S. Enriched targets.
doi: 10.1016/0375-9474(71)90330-7
1971WA18 Phys.Rev.Lett. 27, 961 (1971) R.E.Warner, G.C.Ball, W.G.Davies, A.J.Ferguson, J.S.Forster Charge-Exchange and/or Knockout Spectator Poles in the Reaction D(3He, tp)p NUCLEAR REACTIONS 2H(3He, tp), E=27 MeV; 2H(3He, 3Hep), E=27 MeV; measured σ(Et, Ep), σ(E(3He), Ep).
doi: 10.1103/PhysRevLett.27.961
1970BR28 Phys.Rev.Lett. 25, 944 (1970) C.Broude, W.G.Davies, J.S.Forster High-Spin States in 22Ne NUCLEAR REACTIONS 19F(α, pγ), E=20 MeV; measured σ(Ep, Eγ, θ(γ)). 22Ne deduced levels, J, π, γ-mixing.
doi: 10.1103/PhysRevLett.25.944
1970KI10 Phys.Lett. 32B, 343 (1970) J.E.Kitching, W.Darcey, W.G.Davies, W.McLatchie, J.M.Morton The Conservation of Seniority in the 1g9/2 Neutron Shell NUCLEAR REACTIONS 87Sr(p, d), E=20 MeV; measured σ(θ). 86Sr levels deduced L, seniority conservation in 1g9/2 shell.
doi: 10.1016/0370-2693(70)90490-9
1969DA07 Nucl.Phys. A128, 465 (1969); Erratum Nucl.Phys. A141, 675 (1970) W.G.Davies, J.C.Hardy, W.Darcey The 31P(t, p)33P Reaction and the Usefulness of Double-Stripping in Distinguishing among Shell-Model Calculations NUCLEAR REACTIONS 31P(t, p), E=12.1 MeV; measured σ(Ep, θ); 33P deduced levels, J, π, L. Natural target.
doi: 10.1016/0375-9474(69)90417-5
1969JE01 Nucl.Phys. A128, 224 (1969) A.F.Jeans, W.Darcey, W.G.Davies, K.N.Jones, P.K.Smith A Study of the 208Pb(d, p)209Pb Reaction at Energies Above and below the Coulomb Barrier NUCLEAR REACTIONS 208Pb(d, p), Ed=8.0, 9.0, 10.0, 16.5, 18.7 MeV; measured absolute σ(Ep, θ); deduced Q. 209Pb deduced levels, J, L, π, S. Enriched target.
doi: 10.1016/0375-9474(69)90988-9
1968DA08 Phys.Letters 27B, 363 (1968) W.G.Davies, J.E.Kitching, W.McLatchie, D.G.Montague, K.Ramavataram, N.S.Chant Levels Excited in the Reaction 58Ni(p, t)56Ni NUCLEAR REACTIONS 58Ni(p, t), E=50 MeV; measured σ(θ). 56Ni deduced levels, J, π.
doi: 10.1016/0370-2693(68)90183-4
1968HA34 Nucl.Phys. A121, 103 (1968) J.C.Hardy, W.G.Davies, W.Darcey 91Y and the Failure of the Closed Shell at 88Sr NUCLEAR REACTIONS 92Zr(t, α), E=12.1 MeV; measured σ(Eα, θ). 89Y(t, p), E=12.1 MeV; measured σ(Ep, θ). 91Y deduced levels, J, π, L(p), L(2n). Enriched target.
doi: 10.1016/0375-9474(68)90499-5
1968WO09 Phys.Letters 28B, 77 (1968) A Shell Model Study of the Structure of 56Ni NUCLEAR STRUCTURE 56Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90132-9
1966DA03 Nucl.Phys. 76, 65(1966) W.G.Davies, W.K.Dawson, G.C.Neilson, K.Ramavataram Nuclear Structure Studies of Phosphorous Isotopes (II). The 28Si(d, n)29P Reaction NUCLEAR REACTIONS 28Si(d, n); E = 4, 5 MeV; measured σ(En, θ). 29P deduced levels, J, π, S. Enriched target.
doi: 10.1016/0029-5582(66)90959-X
1965CU03 Phys.Letters 15, 266 (1965) B.Cujec, W.G.Davies, W.K.Dawson, T.B.Grandy, G.C.Neilson, K.Ramavataram The Si30(d, n)P31 Reaction NUCLEAR STRUCTURE 31P; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)91242-4
1965DA08 Phys.Letters 19, 576 (1965) W.G.Davies, W.K.Dawson, G.C.Neilson Negative Parity and Isobaric Analogue States in 31P NUCLEAR STRUCTURE 31P; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90783-3
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