NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = G.G.Shute Found 47 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
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
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
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
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
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
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
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
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
1977KA10 J.Phys.(London) G3, 571 (1977) O.Karban, A.K.Basak, C.O.Blyth, W.Dahme, J.B.A.England, J.M.Nelson, N.T.Okumusoglu, S.Roman, G.G.Shute, R.Vlastou Scattering of 33 MeV Polarized 3He Particles by Hydrogen and Helium Isotopes NUCLEAR REACTIONS 1,2,3H, 3,4He(polarized 3He, 3He), E=33.3 MeV; measured A(θ); deduced optical-model parameters.
doi: 10.1088/0305-4616/3/4/017
1976KA23 Nucl.Phys. A269, 312 (1976) O.Karban, A.K.Basak, J.B.A.England, G.C.Morrison, J.M.Nelson, S.Roman, G.G.Shute The j-Dependence of (3He, d) and (3He, α) Reaction Analysing Powers in the 1p Shell NUCLEAR REACTIONS 9Be, 12C(polarized 3He, d), (polarized 3He, α), E=33.3 MeV; measured σ(θ), A(θ); deduced J-dependence. 10B, 8Be, 13N, 11C levels deduced S.
doi: 10.1016/0375-9474(76)90683-7
1966SH10 Nucl.Phys. 83, 460(1966) Angular Correlations for 12C(p, p'γ)12C (II.) Overlapping Resonances and the Missing 5/2- Level in 13N NUCLEAR REACTIONS 12C(p, p'γ), E = 5.9 MeV; measured σ(θ p', θ γ). 13N level deduced J, π. Natural target.
doi: 10.1016/0029-5582(66)90584-0
1964BA14 Nucl. Phys. 52, 385 (1964) A.M.Baxter, K.G.McIntyre, G.G.Shute, D.Robson Angular Correlations for C12(p, p'γ)C12 in a Resonance-Free Region NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90702-3
1963PA10 Gordon Comf.On Photonuclear Reactions, p.113 (1963) A.W.Parker, G.G.Shute, R.R.Whitehead Inverse Photodisintegration of Neon-20 and Silicon 28 in the Giant Resonance Region NUCLEAR STRUCTURE 20Ne, 28Si; measured not abstracted; deduced nuclear properties.
1962PA07 Australian J.Phys. 15, 443 (1962) NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1962SH22 Nuclear Phys. 37, 535 (1962) G.G.Shute, D.Robson, V.R.McKenna, A.T.Berztiss Elastic Scattering of Protons by Carbon NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90289-4
1961BA25 Australian J.Phys. 14, 196 (1961) Nuclear Sci.Abstr. 15, 2957, Abstr.22942 (1961); See Keynumber 1961MC11 V.R.McKenna, A.M.Baxter, G.G.Shute Energy Levels in 13N NUCLEAR STRUCTURE 12C, 13N; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0934. 1961MC11 Australian J.Phys. 14, 196 (1961) Nuclear Sci.Abstr. 15, 2957, Abstr.22942 (1961) V.R.McKenna, A.M.Baxter, G.G.Shute Energy Levels in 13N NUCLEAR REACTIONS 12C(p, p), E=5-11.5 MeV; measured reaction products, Ep, Ip. 13N; deduced σ(θ), resonance structures, level energies.
1961MC16 Australian J.Phys. 14, 432 (1961) NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1960SH06 Proc.Roy.Soc.(London) 257A, 52 (1960) Lifetime of the 961 keV Level in 152Sm NUCLEAR STRUCTURE 152Sm; measured not abstracted; deduced nuclear properties.
doi: 10.1098/rspa.1960.0133
1959BO44 Nuclear Phys. 11, 341 (1959) N.E.Booth, G.W.Hutchinson, A.M.Segar, G.G.Shute, D.H.White β-η Correlation in Ne23 with Resonance Fluorescence
doi: 10.1016/0029-5582(59)90273-1
1958MO96 Phys.Rev.Letters 1, 21 (1958) Electron-Capture Energy and Level Lifetime by Temperature Effect in Sm152 Gamma-Ray Resonance
doi: 10.1103/PhysRevLett.1.21
1958SH62 Phil.Mag. 3, 726 (1958) Polarization Measurements of Gamma Radiation from Sulphur-34
doi: 10.1080/14786435808237009
1957FI12 Phil.Mag. 2, 1255 (1957) The Angular Correlation of the Gamma Cascade in Sulphur 34
doi: 10.1080/14786435708244014
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