NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = B.M.Spicer Found 81 matches. 1999MU20 Phys.Rev. C60, 067601 (1999) M.C.Munro, B.M.Spicer, W.P.Alford, A.Celler, R.S.Henderson, K.P.Jackson, S.Koutsoliotas, S.A.Long, S.C.McDonald, C.A.Miller, B.W.Pointon, K.J.Raywood, G.G.Shute, S.Yen The 20Ne(n, p) Reaction at High Momentum Transfer NUCLEAR REACTIONS 20Ne(n, p), E=298 MeV; measured proton spectra, σ(E, θ). Enriched target, DWIA analysis, comparison with large-basis shell model calculations.
doi: 10.1103/PhysRevC.60.067601
1998LO12 Phys.Rev. C57, 3191 (1998) S.A.Long, B.M.Spicer, K.J.Raywood, R.Abegg, W.P.Alford, A.Celler, D.Frekers, P.E.Green, O.Hausser, R.L.Helmer, R.S.Henderson, K.H.Hicks, K.P.Jackson, R.G.Jeppesen, N.S.P.King, C.A.Miller, M.A.Moinester, V.C.Officer, G.G.Shute, A.Trudel, M.C.Vetterli, A.I.Yavin, S.Yen Spin-Isovector Giant Resonances Induced by (n, p) Reactions on Heavy Nuclei NUCLEAR REACTIONS 120Sn, 181Ta(n, p), E=298 MeV; 238U(n, p), E=318 MeV; measured σ(Ep, θ). 90Zr, 208Pb(n, p), E=198 MeV; analyzed σ(Ep, θ). 90Y, 120In, 181Hf, 208Tl, 238Pa deduced L=0, 1, 2, 3 giant resonances energy distributions, quasi-free contributions, comparison with sum rules for L=1, 3. Multipole decomposition procedure.
doi: 10.1103/PhysRevC.57.3191
1997HE06 Phys.Rev. C55, 2802 (1997) R.L.Helmer, M.A.Punyasena, R.Abegg, W.P.Alford, A.Celler, S.El-Kateb, J.Engel, D.Frekers, R.S.Henderson, K.P.Jackson, S.Long, C.A.Miller, W.C.Olsen, B.M.Spicer, A.Trudel, M.C.Vetterli Gamow-Teller Strength from the 76Se(n, p)76As Reaction: Implications for the double β decay of 76Ge NUCLEAR REACTIONS 76Se(n, p), E=198 MeV; measured σ(θ). 76As deduced Gamow-Teller strength distribution. 76Ge deduced 2ν-accompanied 2β-decay T1/2. Quasi-particle RPA comparison, other data analyzed.
doi: 10.1103/PhysRevC.55.2802
1997RA32 Nucl.Phys. A625, 675 (1997) K.J.Raywood, S.A.Long, B.M.Spicer Gamow-Teller and Dipole Strength in the 208Pb(n, p) Reaction NUCLEAR REACTIONS 208Pb(n, p), E=198 MeV; analyzed σ(θ); deduced Gamow-Teller transition strength distributions. Multipole decomposition technique.
doi: 10.1016/S0375-9474(97)00321-7
1994EL05 Phys.Rev. C49, 3128 (1994) S.El-Kateb, K.P.Jackson, W.P.Alford, R.Abegg, R.E.Azuma, B.A.Brown, A.Celler, D.Frekers, O.Hausser, R.Helmer, R.S.Henderson, K.H.Hicks, R.Jeppesen, J.D.King, K.Raywood, G.G.Shute, B.M.Spicer, A.Trudel, M.Vetterli, S.Yen Spin-Isospin Strength Distributions for fp Shell Nuclei: Results for the 55Mn(n, p), 56Fe(n, p), and 58Ni(n, p) reactions at 198 MeV NUCLEAR REACTIONS 55Mn, 56Fe, 58Ni(n, p), E=198 MeV; measured σ(θ, Ep). 55Mn, 56Fe, 58Ni deduced Gamow-Teller transition strength distribution.
doi: 10.1103/PhysRevC.49.3128
1994FA05 Nucl.Phys. A572, 349 (1994) Measurement of the Nuclear Bremsstrahlung Cross Section from the 12C(p, p)12C Reaction Near the 1.734 MeV Resonance NUCLEAR REACTIONS 12C(p, p), E=1.80, 1.83 MeV; measured σ(θ), bremsstrahlung γ p-coin; deduced structure. Feshbach-Yennie calculations comparison.
doi: 10.1016/0375-9474(94)90179-1
1994SP03 Phys.Rev. C49, 2398 (1994) B.M.Spicer, N.Dytlewski, S.Koutsoliotas, D.D.Cohen, M.Geso Excitation Function for the Population of the 4.51 MeV State of 27Al in Inelastic Proton Scattering: Evidence for 6- strength ( Question ) NUCLEAR REACTIONS, ICPND 27Al(p, p'γ), E=5.6-7.3 MeV; measured Eγ, Iγ, σ(E). 28Si deduced resonance, 6- strength fragmentation features.
doi: 10.1103/PhysRevC.49.2398
1991LE22 Nucl.Phys. A532, 583 (1991) P.R.Lewis, G.G.Shute, B.M.Spicer, R.S.Henderson, R.Abegg, D.Frekers, O.Hausser, K.P.Jackson, C.A.Miller, S.Yen Intermediate-Energy Proton Scattering from 10B NUCLEAR REACTIONS 10B(p, p), (p, p'), E=200 MeV; measured σ(θ). Optical model, DWA analyses, density-dependent Bonn t-matrix, other data analyzed.
doi: 10.1016/0375-9474(91)90599-2
1990RA13 Phys.Rev. C41, 2836 (1990) K.J.Raywood, B.M.Spicer, S.Yen, S.A.Long, M.A.Moinester, R.Abegg, W.P.Alford, A.Celler, T.E.Drake, D.Frekers, P.E.Green, O.Hausser, R.L.Helmer, R.S.Henderson, K.H.Hicks, K.P.Jackson, R.G.Jeppesen, J.D.King, N.S.P.King, C.A.Miller, V.C.Officer, R.Schubank, G.G.Shute, M.Vetterli, J.Watson, A.I.Yavin Spin-Flip Isovector Giant Resonances from the 90Zr(n, p)90Y Reaction at 198 MeV NUCLEAR REACTIONS 90Zr(n, p), E=198 MeV; measured σ(Ep, θ); deduced σ(θ). 90Y deduced spin isovector dipole transition strengths.
doi: 10.1103/PhysRevC.41.2836
1989MO19 Phys.Lett. 230B, 41 (1989) M.A.Moinester, A.Trudel, K.Raywood, S.Yen, B.M.Spicer, R.Abegg, W.P.Alford, N.Auerbach, A.Celler, D.Frekers, O.Hausser, R.L.Helmer, R.Henderson, K.H.Hicks, K.P.Jackson, R.G.Jeppesen, N.S.P.King, S.Long, C.A.Miller, M.Vetterli, J.Watson, A.I.Yavin A Study of Spin Isovector Giant Resonances with the 208Pb(n, p)208Tl Reaction NUCLEAR REACTIONS 208Pb(n, p), E=198, 458 MeV; measured σ(θp, Ep). 208Tl deduced spin isovector giant resonances.
doi: 10.1016/0370-2693(89)91650-X
1989WA17 Phys.Rev. C40, 570 (1989) J.W.Watson, W.Pairsuwan, B.D.Anderson, A.R.Baldwin, B.S.Flanders, C.Lebo, R.Madey, J.D.Brown, C.C.Foster, D.L.Friesel, H.Nann, E.J.Stephenson, P.B.Foot, G.G.Shute, B.M.Spicer 48Ca(d, n)49Sc Reaction at 79 MeV NUCLEAR REACTIONS 48Ca(polarized d, n), E=79 MeV; measured σ(En), σ(θ), vector analyzing power; deduced model parameters. 49Sc levels deduced C2S. DWBA, Johnson-Soper adiabatic approximation analyses.
doi: 10.1103/PhysRevC.40.570
1988CO05 Nucl.Phys. A481, 494 (1988) S.F.Collins, G.G.Shute, B.M.Spicer, V.C.Officer, D.W.Devins, D.L.Friesel, W.P.Jones The Spectroscopy of 13C by Inelastic Proton Scattering NUCLEAR REACTIONS 13C(p, p)(p, p'), E=135 MeV; 13C(polarized p, p)(polarized p, p'), E=119 MeV; measured σ(θ), A(θ). Optical model, DWA analyses, density-dependent t-matrices.
doi: 10.1016/0375-9474(88)90342-9
1988JA01 Phys.Lett. 201B, 25 (1988) K.P.Jackson, A.Celler, W.P.Alford, K.Raywood, R.Abegg, R.E.Azuma, C.K.Campbell, S.El-Kateb, D.Frekers, P.W.Green, O.Hausser, R.L.Helmer, R.S.Henderson, K.H.Hicks, R.Jeppesen, P.Lewis, C.A.Miller, A.Moalem, M.A.Moinester, R.B.Schubank, G.G.Shute, B.M.Spicer, M.C.Vetterli, A.I.Yavin, S.Yen The (n, p) Reaction as a Probe of Gamow-Teller Strength NUCLEAR REACTIONS 6Li, 12,13C(n, p), E=198 MeV; measured σ(θ), σ(θp).
doi: 10.1016/0370-2693(88)90073-1
1988YE01 Phys.Lett. 206B, 597 (1988) S.Yen, B.M.Spicer, M.A.Moinester, K.Raywood, R.Abegg, W.P.Alford, A.Celler, T.E.Drake, D.Frekers, O.Hausser, R.L.Helmer, R.S.Henderson, K.H.Hicks, K.P.Jackson, R.Jeppesen, J.D.King, N.S.P.King, K.Lin, S.Long, C.A.Miller, V.C.Officer, R.Schubank, G.G.Shute, M.C.Vetterli, A.I.Yavin Gamow-Teller Strength and Giant Resonances in 90Zr(n, p) at 198 MeV NUCLEAR REACTIONS 90Zr(n, p), E=198 MeV; measured σ(θp, Ep). 90Y deduced giant resonances, Gamow-Teller Strength.
doi: 10.1016/0370-2693(88)90703-4
1987AN04 Nucl.Phys. A468, 43 (1987) P.R.Andrews, B.M.Spicer, G.G.Shute, V.C.Officer, J.M.R.Wastell, H.Nann, Q.Li, A.D.Bacher, D.L.Friesel, W.P.Jones Spectroscopy of 14C from the 11B(α, p)14C Reaction at 118 MeV NUCLEAR REACTIONS 11B(α, p), E=118.1 MeV; measured σ(Ep), σ(θ); deduced model parameters. 14C deduced levels, J, π. DWBA calculations.
doi: 10.1016/0375-9474(87)90318-6
1987FO21 J.Phys.(London) G13, 1531 (1987) P.B.Foot, D.Barker, C.O.Blyth, J.B.A.England, O.Karban, M.C.Mannion, J.M.Nelson, C.A.Ogilvie, C.Pinder, L.Potvin, S.Roman, G.G.Shute, L.Zybert, R.Zybert, J.M.O'Donnell, M.J.Smithson, N.M.Clarke, K.I.Pearce, P.Simmonds, B.M.Spicer The 12C(t, α)11B Reaction at 33 MeV NUCLEAR REACTIONS, MECPD 12C(t, α), E=33 MeV; measured σ(Eα), σ(θ); deduced model parameters. DWBA, coupled-reaction channel analyses.
doi: 10.1088/0305-4616/13/12/011
1987FO22 Aust.J.Phys. 40, 611 (1987) P.B.Foot, G.G.Shute, B.M.Spicer, C.C.Foster, J.D.Brown, D.L.Friesel, H.Nann, J.W.Seubert, E.J.Stephenson, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, W.Pairsuwan, J.W.Watson D State Effects in the 11B(d(pol), n)12C Reaction at 79 MeV NUCLEAR REACTIONS 11B(polarized d, n), E=79 MeV; measured σ(θ), vector analyzing power vs θ; deduced 2H D-state effects role. DWBA analysis.
1987LE24 Nucl.Phys. A474, 499 (1987) P.R.Lewis, G.G.Shute, B.M.Spicer, V.C.Officer, P.R.Andrews, S.M.Banks The 13C(p(pol), d)12C Reaction at 119 MeV NUCLEAR REACTIONS, MECPD 13C(polarized p, d), E=200 MeV; measured σ(θ), A(θ). 12C levels deduced spectroscopic factors. Exact finite-range DWBA, coupled channels analysis, adiabatic model. Enriched target.
doi: 10.1016/0375-9474(87)90628-2
1987RE10 Nucl.Phys. A472, 1 (1987) K.Reiner, P.Grabmayr, G.J.Wagner, S.M.Banks, B.G.Lay, V.C.Officer, G.G.Shute, B.M.Spicer, C.W.Glover, W.P.Jones, D.W.Miller, H.Nann, E.J.Stephenson Deeply-Bound Hole States in 57Co and the Spreading of the 1d5/2 Hole Strength Distribution NUCLEAR REACTIONS, MECPD 58Ni(polarized d, 3He), E=80 MeV; measured σ(E(3He)), σ(θ), vector analyzing powers. 57Co deduced levels, J, π, d3/2-d5/2 hole strength distributions.
doi: 10.1016/0375-9474(87)90217-X
1986AN30 Nucl.Phys. A459, 317 (1986) P.R.Andrews, G.G.Shute, B.M.Spicer, S.F.Collins, V.C.Officer, J.M.Wastell, H.Nann, D.W.Devins, Q.Li, W.P.Jones, C.Olmer, A.D.Bacher, G.T.Emery Location of Multiparticle-Multihole Strength in 16N via the 3-Particle Transfer Reaction 13C(α, p)16N at 118 MeV NUCLEAR REACTIONS 13C(α, p), E=118 MeV; measured σ(θ). 16N levels deduced J, π, multiparticle-multihole strength. DWBA analysis, microscopic form factors.
doi: 10.1016/0375-9474(86)90137-5
1986FO08 Can.J.Phys. 64, 1348 (1986) P.B.Foot, G.G.Shute, B.M.Spicer The Anomalous Analyzing Power for the 11B(d, n)12C Reaction to the 2+ State at 4.44 MeV NUCLEAR REACTIONS 11B(polarized d, n), E=79 MeV; calculated analyzing power vs θ. 12C level deduced anomaly. DWBA.
doi: 10.1139/p86-237
1986OH01 Nucl.Phys. A448, 205 (1986) H.Ohnuma, N.Hoshino, O.Mikoshiba, K.Raywood, A.Sakaguchi, G.G.Shute, B.M.Spicer, M.H.Tanaka, M.Tanifuji, T.Terasawa, M.Yasue The 12C(d, p)13C Reaction at E(d) = 30 MeV and Positive-Parity States in 13C NUCLEAR REACTIONS 12C(d, p), E=30 MeV; measured σ(θ). 13C levels deduced Γ, spectroscopic factors. CCBA, DWBA analysis.
doi: 10.1016/0375-9474(86)90087-4
1985BA14 Nucl.Phys. A437, 381 (1985) S.M.Banks, B.M.Spicer, G.G.Shute, V.C.Officer, G.J.Wagner, W.E.Dollhopf, Li Qingli, C.W.Glover, D.W.Devins, D.L.Friesel The 48Ca(d(pol), 3He)47K Reaction at 80 MeV NUCLEAR REACTIONS 48Ca(polarized d, 3He), (polarized d, d) E=79.2 MeV; measured σ(E(3He)), σ(θ), vector analyzing powers; deduced optical model parameters. 47K levels deduced J, π, configurations.
doi: 10.1016/0375-9474(85)90096-X
1985FO05 Phys.Rev. C31, 1133 (1985) P.B.Foot, G.G.Shute, B.M.Spicer, C.C.Foster, H.Nann, E.J.Stephenson, B.D.Anderson, A.R.Baldwin, B.S.Flanders, C.Lebo, R.Madey, J.W.Watson 11B(d, n)12C Reaction and the Adiabatic Approximation NUCLEAR REACTIONS 11B(d, n), E=79 MeV; measured σ(θ); deduced deuteron optical model parameters. 12C levels deduced L, S. Adiabatic model, DWBA analysis.
doi: 10.1103/PhysRevC.31.1133
1985LA15 Phys.Rev. C32, 440 (1985) B.G.Lay, S.M.Banks, B.M.Spicer, G.G.Shute, V.C.Officer, R.M.Ronningen, G.M.Crawley, N.Anantaraman, R.P.DeVito Multipole Moments of 176Yb and 182W Nuclei from Inelastic Scattering of 134 MeV Protons NUCLEAR REACTIONS 176Yb, 182W(polarized p, p), (polarized p, p'), E=134 MeV; measured σ(Ep'), σ(θ), asymmetry vs θ; deduced optical model parameters. 176Yb, 182W deduced β2, β4, β6, multipole moments. Phenomenological optical model, coupled-channels analysis.
doi: 10.1103/PhysRevC.32.440
1984AM04 Nucl.Phys. A413, 255 (1984) K.Amos, W.Bauhoff, I.Morrison, S.F.Collins, R.S.Henderson, B.M.Spicer, G.G.Shute, V.C.Officer, D.W.Devins, D.L.Friesel, W.P.Jones Microscopic and Macroscopic Aspects of 135 MeV Proton Scattering from 16O NUCLEAR REACTIONS 16O(p, p'), E=135 MeV; measured σ(θ). 16O deduced level, tentative J, π. Optical model, DWBA analyses, collective, shell model wave functions, density-dependent t-matricies.
doi: 10.1016/0375-9474(84)90375-0
1984BA22 Z.Phys. A316, 241 (1984) S.M.Banks, B.M.Spicer, G.G.Shute, V.C.Officer, G.J.Wagner, W.E.Dollhopf, Li Quingli, C.W.Glover, D.W.Devins, D.L.Friesel Evidence for Proton Ground State Correlations in 48Ca NUCLEAR REACTIONS 48Ca(polarized d, 3He), E=80 MeV; measured σ(E(3He)), σ(θ), A(θ). 48Ca deduced ground state configuration. 47K deduced level, J, π, C2S.
doi: 10.1007/BF01412270
1984HA55 Aust.J.Phys. 37, 475 (1984) M.F.Harrigan, B.M.Spicer, D.D.Cohen L-Subshell X-Ray Production by 100-250 keV/a.m.u. Ions ATOMIC PHYSICS Gd(p, X), E=100-200 keV; Au, W(α, X), E=600-100 keV; measured X-ray yields; deduced L-subshell ionization σ.
doi: 10.1071/PH840475
1983BA48 Aust.J.Phys. 36, 287 (1983) L-Shell Ionization of Sn and Gd by 20-100 keV Electron Impact ATOMIC PHYSICS Sn, Gd(e, X), E=20-100 keV; measured L X-ray production σ ratios. Thin targets.
doi: 10.1071/PH830287a
1983BA57 Nucl.Phys. A410, 180 (1983) W.Bauhoff, S.F.Collins, R.S.Henderson, G.G.Shute, B.M.Spicer, V.C.Officer, K.A.Amos, I.Morrison, D.W.Devins, D.L.Friesel, W.P.Jones Density-Dependent Forces and Large-Basis Structure Models in the Analyses of 12C(p, p') Reactions at 135 MeV NUCLEAR REACTIONS 12C(p, p'), (p, p), E=135 MeV; measured σ(θ). Optical model, DWBA analyses, density-dependent t-matrices.
doi: 10.1016/0375-9474(83)90198-7
1983RO11 Phys.Rev. C28, 123 (1983) R.M.Ronningen, G.M.Crawley, N.Anantaraman, S.M.Banks, B.M.Spicer, G.G.Shute, V.C.Officer, J.M.R.Wastell, D.W.Devins, D.L.Friesel Multipole Moments of 154Sm and 166Er by Inelastic Scattering of 134 MeV Protons NUCLEAR REACTIONS 154Sm, 166Er(polarized p, p'), E=134 MeV; measured σ(Ep'), σ(θ), A(θ); deduced deformed optical model parameters. 154Sm, 166Er deduced β2, β4, β6. Enriched targets, magnetic spectrograph. Coupled-channels calculations.
doi: 10.1103/PhysRevC.28.123
1982CO08 Nucl.Phys. A380, 445 (1982) S.F.Collins, G.G.Shute, B.M.Spicer, V.C.Officer, I.Morrison, K.A.Amos, D.W.Devins, D.L.Friesel, W.P.Jones A Study of the 13C(p, p') Reactions at 135 MeV NUCLEAR REACTIONS 13C(p, p), (p, p'), E=135 MeV; measured σ(θ). 13C levels deduced possible configuration. Optical model, DWBA analyses.
doi: 10.1016/0375-9474(82)90570-X
1982RI05 Aust.J.Phys. 35, 9 (1982); Corrigendum Aust.J.Phys. 35, 351 (1982) L.Rikus, S.F.Collins, K.A.Amos, B.M.Spicer, G.G.Shute, I.Morrison, V.C.Officer, R.Smith, D.W.Devins, D.L.Friesel, W.P.Jones Excitation of the 9.50 MeV (9/2+) States of 13C in Intermediate Energy Scattering Experiments NUCLEAR REACTIONS 13C(p, p'), E=135 MeV; measured σ(θ). 13C state deduced total angular momentum transfer, configuration. Microscopic DWBA analysis.
1981DE19 Phys.Rev. C24, 59 (1981) D.W.Devins, D.L.Friesel, W.P.Jones, A.C.Attard, S.F.Collins, G.G.Shute, B.M.Spicer, V.C.Officer, I.D.Svalbe, R.S.Henderson, W.E.Dollhopf 40Ca(d, 3He)39K Reaction at 76 MeV NUCLEAR REACTIONS 40Ca(d, 3He), E=76 MeV; measured σ(θ, E(3He)). 39K deduced levels, J, π, L, C2S. Enriched targets. DWBA, CCBA analyses.
doi: 10.1103/PhysRevC.24.59
1981HE21 Nucl.Phys. A372, 117 (1981) R.S.Henderson, S.F.Collins, B.M.Spicer, G.G.Shute, V.C.Officer, D.W.Devins, D.L.Friesel, W.P.Jones The Scattering of 136 MeV Protons from 6Li NUCLEAR REACTIONS 6Li(p, p), (p, p'), E=136 MeV; measured σ(θ). Optical model, DWBA analyses.
doi: 10.1016/0375-9474(81)90090-7
1980CR02 Phys.Rev. C22, 316 (1980) G.M.Crawley, S.Gales, D.Weber, B.Zwieglinski, W.Benenson, D.Friesel, A.Bacher, B.M.Spicer Deep Hole States Observed in (p, t) Reactions NUCLEAR REACTIONS 120,122,124Sn(p, t), E=89 MeV; measured σ(Et, θ). 118,120,122Sn deduced levels, Γ. DWBA, enriched targets.
doi: 10.1103/PhysRevC.22.316
1979DE35 Aust.J.Phys. 32, 323 (1979) D.W.Devins, D.L.Friesel, W.P.Jones, A.C.Attard, I.D.Svalbe, V.C.Officer, R.S.Henderson, B.M.Spicer, G.G.Shute The 12C(p, 2p)11B Reaction at 100 MeV NUCLEAR REACTIONS 12C(p, 2p), E=100 MeV; measured pp-coin, pp(θ). 11B levels deduced excitation mechanism. Symmetric, asymmetric geometry. DWIA calculations.
doi: 10.1071/PH790323
1979HE09 Aust.J.Phys. 32, 411 (1979) R.S.Henderson, B.M.Spicer, I.D.Svalbe, V.C.Officer, G.G.Shute, D.W.Devins, D.L.Friesel, W.P.Jones, A.C.Attard 4- Particle-Hole States in 16O NUCLEAR REACTIONS 16O(p, p'), E=135 MeV; measured σ(Ep, θ). 16O levels deduced J, π, T, configuration. QDDM spectrograph.
doi: 10.1071/PH790411
1979WI09 Aust.J.Phys. 32, 187 (1979) Partial Wave Analysis of the 18O(p, α0)15N Reaction NUCLEAR REACTIONS 18O(p, α), E=6.6-10.4 MeV; measured σ(E, θ); 19F deduced resonances, Γ, J, π. Gas target, partial wave analysis.
doi: 10.1071/PH790187
1978RO09 Phys.Rev.Lett. 40, 1439 (1978) P.G.Roos, N.S.Chant, D.W.Devins, D.L.Friesel, W.P.Jones, A.C.Attard, R.S.Henderson, I.D.Svalbe, B.M.Spicer, V.C.Officer, G.G.Shute Experimental Test of the Factorization Approximation in the Reaction 40Ca(p, 2p)39K at 148.2 MeV NUCLEAR REACTIONS 40Ca(p, 2p), E=148.2 MeV; measured σ. 39K levels deduced S. DWIA analysis.
doi: 10.1103/PhysRevLett.40.1439
1977SP06 Aust.J.Phys. 30, 127(1977) Evidence for Two-Step Processes in Photonuclear Reactions NUCLEAR STRUCTURE 15N, 16O, 28Si, 32S; analyzed structure from photodisintegration data.
doi: 10.1071/PH770127
1977SU07 Aust.J.Phys. 30, 677 (1977) Su Su, R.H.Sambell, E.G.Muirhead, B.M.Spicer The Photoneutron Cross Section of Natural Osmium NUCLEAR REACTIONS Os(γ, xn), E ≤ 28 MeV bremsstrahlung; measured σ(E).
doi: 10.1071/PH770677
1977SW04 Phys.Rev. C16, 1264 (1977) Z.E.Switkowski, S.R.Kennett, D.G.Sargood, B.M.Spicer, R.O'Brien Cross Sections for 18O(α, n3, 4γ)21Ne Reactions Populating the (1/2-, 1/2+) Doublet NUCLEAR REACTIONS 18O(α, nγ), E=4.3-6.5 MeV; measured σ(E). 21Ne deduced levels. Enriched target.
doi: 10.1103/PhysRevC.16.1264
1975CR04 Nucl.Phys. A244, 67 (1975) G.B.Crinean, L.W.J.Wild, B.M.Spicer Proton Reactions with 17O (I). Elastic and Inelastic Scattering Reactions NUCLEAR REACTIONS 17O(p, p'), E=8.5-10.5 MeV; measured σ(E;Ep', θ); deduced optical model parameters. Enriched target.
doi: 10.1016/0375-9474(75)90007-X
1975CR05 Nucl.Phys. A244, 77 (1975) G.B.Crinean, G.M.Hudson, L.W.J.Wild, B.M.Spicer Proton Reactions with 17O (II). The 17O(p, d)16O Reaction NUCLEAR REACTIONS 17O(p, d), E=8.6-11.4 MeV; measured σ(E, Ed, θ); analyzed σ(E, Ed, θ). 17O(p, d), E=9, 9.7, 10 MeV; calculated analyzing power A(θ). BHMM, DWBA analysis. Enriched target.
doi: 10.1016/0375-9474(75)90008-1
1975HA33 Aust.J.Phys. 28, 247 (1975) J.Havloujian, G.Ravalli, B.M.Spicer Differential Cross Sections for the 13C(3He, p0) and 15N(3He, p0) Reactions at 15 MeV NUCLEAR REACTIONS 13C, 15N(3He, p), E=15 MeV; measured σ(Ep, θ). 13C, 15N(3He, 3He), E=15 MeV; measured σ(θ); deduced optical parameters.
doi: 10.1071/PH750247
1975HU03 Nucl.Phys. A238, 189 (1975) R.J.Hughes, R.H.Sambell, E.G.Muirhead, B.M.Spicer The Photoneutron Cross Section of 9Be NUCLEAR REACTIONS 9Be(γ, xn), E < 28 MeV; measured neutron yields; deduced total, integrated σ. 9Be deduced resonances.
doi: 10.1016/0375-9474(75)90348-6
1975MC15 Aust.J.Phys. 28, 127 (1975) A Particle-Hole-Rotator Coupling Model for the Giant Resonance of Carbon-12 NUCLEAR STRUCTURE 12C; calculated giant resonance structure.
doi: 10.1071/PH750127
1975MC16 Aust.J.Phys. 28, 241 (1975) Radiative Decay of the Low-Lying States of 12C NUCLEAR STRUCTURE 12C; calculated B(E2).
1973HI10 Aust.J.Phys. 26, 585 (1973) The Dynamic Collective Model Interpretation of the Photoneutron Cross Section of 181Ta NUCLEAR REACTIONS 181Ta(γ, xn), E(max)=7-28.8 MeV; measured σ(E). 181Ta deduced resonances, level-width.
doi: 10.1071/PH730585
1973SA07 Nucl.Phys. A205, 139 (1973) The Photoneutron Cross Section of 45Sc NUCLEAR REACTIONS 45Sc(γ, xn), E=10-25 MeV measured yield curves; deduced σ(E). Natural target.
doi: 10.1016/0375-9474(73)90125-5
1973SP02 Aust.J.Phys. 26, 7 (1973) The Dipole States of Mass-11 Nuclei NUCLEAR STRUCTURE 11B, 11C calculated dipole states.
doi: 10.1071/PH730007
1973SP03 Aust.J.Phys. 26, 269 (1973) An Interpretation of de-Excitation Gamma Ray Measurements Following the Photodisintegration of 12C, 16O, and 40Ca NUCLEAR REACTIONS 12C, 16O, 40Ca(γ, Xγ); analyzed photodisintegration data.
doi: 10.1071/PH730269
1972HU03 Nucl.Phys. A184, 175 (1972) G.M.Hudson, G.B.Crinean, D.T.Kelly, B.M.Spicer The 9Be(p, d0)8Be Reaction and the BHMM Theory of Stripping Reactions NUCLEAR REACTIONS 9Be(p, d0), E=5, 6, 7, 8, 9, 10, 11 MeV; measured σ(θ). 8Be deduced S.
doi: 10.1016/0375-9474(72)90452-6
1971DA12 Nucl.Phys. A168, 399 (1971) W.F.Davidson, J.L.Black, M.R.Najam, B.M.Spicer Note on the Cross Section of the 25Mg(t, γ)28Si Reaction NUCLEAR REACTIONS 25Mg(3He, γ), E=4.44, 6.08, 6.15, 8.26 MeV; measured σ(Eγ, 0). Enriched target.
doi: 10.1016/0375-9474(71)90801-3
1971SP09 Z.Phys. 246, 97 (1971) Quartet Structure and Collective Effects in the Scandium Isotopes NUCLEAR STRUCTURE 41,42,43,44,45,46,47,48,49Sc; analyzed systematics of non-normal parity states. 43Sc; calculated B(E2). Quartet structure, collective effects.
doi: 10.1007/BF01394726
1971WE11 Nucl.Phys. A171, 324 (1971) D.V.Webb, E.G.Muirhead, B.M.Spicer The 39K Photoneutron Cross Section to the 38K Isomeric State NUCLEAR REACTIONS 39K(γ, n), E=13.2-29.0 MeV; measured isomeric σ(E). Natural target.
doi: 10.1016/0375-9474(71)90026-1
1970DA13 Z.Phys. 237, 320 (1970) Quartet Structure in Light Nuclei NUCLEAR STRUCTURE 12C, 16O, 32S, 40Ca, 60Ni; analyzed low-lying even-parity, even-spin states. Quartet model.
doi: 10.1007/BF01399051
1970DR06 Z.Phys. 238, 1 (1970) A Test of the Collective Correlations Calculation of the Dipole States of 28Si NUCLEAR REACTIONS 28Si(γ, p), E=17.6 MeV; calculated population of 27Al states. Collective correlations model.
doi: 10.1007/BF01399572
1970FR11 Nucl.Phys. A156, 489 (1970) R.F.Fraser, R.K.Garnsworthy, B.M.Spicer Shell Model of the Dipole States of Mass-15 Nuclei NUCLEAR STRUCTURE 15N, 15O; calculated dipole states. NUCLEAR REACTIONS 15N, 15O(γ, p), E < 30 MeV; calculated σ(E).
doi: 10.1016/0375-9474(70)90246-0
1970HI13 Nucl.Phys. A159, 265 (1970) The Photoneutron Cross Section of Strontium NUCLEAR REACTIONS Sr(γ, n), E < 27 MeV; measured σ(E). 88Sr deduced resonance structure.
doi: 10.1016/0375-9474(70)90042-4
1970OW01 Nucl.Phys. A140, 523 (1970) D.G.Owen, E.G.Muirhead, B.M.Spicer Studies in the Vibrational Splitting of the Giant Dipole Resonance (II). 58Ni and 60Ni NUCLEAR REACTIONS 58Ni, 60Ni(γ, xn), E=11-24 MeV; measured yield curves; deduced σ(E).
doi: 10.1016/0375-9474(70)90577-4
1970RA02 Aust.J.Phys. 23, 255 (1970) The Low-Lying Odd Parity States of 46Sc NUCLEAR REACTIONS 45Sc(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin, γγ(θ). 46Sc deduced rotational structure, B(EL), γ-mixing.
1970WE12 Nucl.Phys. A159, 81 (1970) D.V.Webb, E.G.Muirhead, B.M.Spicer The Photoneutron Cross Sections of 28Si and 24Mg NUCLEAR REACTIONS 24Mg, 28Si(γ, n), E=16.0-31.0 MeV; measured σ(E); deduced integrated σ.
doi: 10.1016/0375-9474(70)90028-X
1969DE26 Nucl.Phys. A139, 501 (1969) T.K.Deague, E.G.Muirhead, B.M.Spicer Structure in the Giant Resonance of 108Pd and of 110Pd NUCLEAR REACTIONS 108Pd(γ, pn), (γ, xn), 108Pd(γ, p), 110Pd(γ, n), E=8-29 MeV; measured yield curves; deduced σ(E). Natural, enriched targets.
doi: 10.1016/0375-9474(69)90274-7
1969OW01 Phys.Letters 30B, 242 (1969) The 29.5 MeV Dipole State of 12C NUCLEAR REACTIONS 12C(γ, nα), E = 25-31 MeV; measured σ(E). 12C deduced dipole resonance.
doi: 10.1016/0370-2693(69)90428-6
1968CA05 Nucl.Phys. A109, 385 (1968) P.H.Cannington, R.J.J.Stewart, B.M.Spicer, M.G.Huber The Photoneutron Cross Section of 141Pr NUCLEAR REACTIONS 141Pr(γ, n), Eγ=9 to 17 MeV; measured yield curve; deduced σ(E). Natural targets.
doi: 10.1016/0375-9474(68)90603-9
1968OW01 Nucl.Phys. A122, 177(1968) D.G.Owen, E.G.Muirhead, B.M.Spicer Structure in the Giant Resonance of 64Zn and 63Cu NUCLEAR REACTIONS 64Zn, 63Cu(γ, n), Eγ=11-23 MeV; measured yield curves, deduced σ(E). Natural targets.
doi: 10.1016/0375-9474(68)90711-2
1965TH04 Nucl.Phys. 64, 486(1965) M.N.Thompson, J.M.Taylor, B.M.Spicer, J.E.E.Baglin The Al27(γ, n)Al26m Cross Section NUCLEAR REACTIONS 27Al(γ, n), E=13-25 MeV; measured σ(E). 27Al deduced resonances.
doi: 10.1016/0029-5582(65)90573-0
1964AL08 Nucl. Phys. 51, 177 (1964) F.R.Allum, G.M.Crawley, B.M.Spicer The Emission of Photoneutrons from Natural Lithium NUCLEAR STRUCTURE Li; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90262-7
1964AL33 Nucl.Phys. 53, 545 (1964) F.R.Allum, T.W.Quirk, B.M.Spicer Angular Distributions Of Fast Photoneutrons NUCLEAR REACTIONS 9Be(γ, n), 12C(γ, n), Sn(γ, n), 181Ta(γ, n), Pb(γ, n), 209Bi(γ, n), E=34 MeV; measured products, 8Be, Eν, Iν; deduced σ(θ). Data were imported from EXFOR entry M0443.
doi: 10.1016/0029-5582(64)90634-0
1964BA24 Nucl. Phys. 54, 549 (1964) Photodisintegration of Ca40 NUCLEAR REACTIONS 40Ca(γ, n), Eγ=15-30 MeV; measured σ(E), Q. 40Ca deduced resonance peaks. Natural target. 39Ca[from 40Ca(γ, n)]; measured T1/2.
doi: 10.1016/0029-5582(64)90433-X
1964SP10 Nuovo Cimento, Suppl. 2, 243 (1964) The Present Status of Photoneutron Cross-Section Measurements
1963CH08 Nucl.Phys. 41, 675 (1963) Application of a Rotational Model to Li7 NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90547-9
1963SP05 Phys.Letters 6, 88 (1963) A Search for H4 NUCLEAR STRUCTURE 4H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90232-4
1961BA54 Nucl.Phys. 22, 207 (1961) J.E.E.Baglin, M.N.Thompson, B.M.Spicer Photodisintegration of Al27: (I) Photoneutron cross section NUCLEAR REACTIONS 27Al(γ, n), E=13.1-18.3 MeV; measured products, 26Al, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry M0268.
doi: 10.1016/0029-5582(61)90453-9
1960SP07 Contrib.Karlsruhe Photonuclear Conf., Karlsruhe, Germany, Paper P11 (1960) B.M.Spicer, J.R.Allum, G.M.Crawley Photonuclear Cross Section in Lithium NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1959TH15 Australian J.Phys. 12, 21 (1959) H.H.Thies, B.M.Spicer, J.E.Baglin The Photoneutron Cross Section of 9Be in the Intermediate Energy Range
doi: 10.1071/PH590021
1959TH16 Australian J.Phys. 12, 293 (1959) Spins and Parities of Levels of 9Be below 15 MeV
doi: 10.1071/PH590293
1958SP19 Australian J.Phys. 11, 298 (1958) B.M.Spicer, H.H.Theis, J.E.Baglin, F.R.Allum The Giant Resonance of Photodisintegration of Tantalum
doi: 10.1071/PH580298
1955SP76 Phys.Rev. 100, 1375 (1955) C12 (γ, n) Yield Curve Near Threshold NUCLEAR REACTIONS 12C(γ, n), E<22 MeV; measured reaction products, Eβ, Iβ; deduced yields, Q-value. Comparison with available data.
doi: 10.1103/physrev.100.1375
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