NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = B.C.Robertson Found 51 matches. 2003PO09 Phys.Rev. C 68, 034605 (2003) A.Pouladdej, T.P.Gorringe, M.D.Hasinoff, A.J.Larabee, A.J.Noble, C.J.Virtue, D.H.Wright, G.Azuelos, B.C.Robertson Photon asymmetry measurement in radiative muon capture on 40Ca NUCLEAR REACTIONS 40Ca(μ-, ν), E at rest; measured Eγ, Iγ, energy-averaged asymmetry; deduced pseudoscalar coupling constant.
doi: 10.1103/PhysRevC.68.034605
1998WR01 Phys.Rev. C57, 373 (1998) D.H.Wright, S.Ahmad, D.S.Armstrong, G.Azuelos, W.Bertl, M.Blecher, C.Q.Chen, P.Depommier, B.C.Doyle, T.von Egidy, T.P.Gorringe, P.Gumplinger, M.D.Hasinoff, D.Healey, G.Jonkmans, A.J.Larabee, J.A.Macdonald, S.C.McDonald, M.Munro, J.-M.Poutissou, R.Poutissou, B.C.Robertson, D.G.Sample, E.Saettler, C.N.Sigler, G.N.Taylor, N.S.Zhang Measurement of the Induced Pseudoscalar Coupling using Radiative Muon Capture on Hydrogen NUCLEAR REACTIONS 1H(μ-, n), E at 63 MeV/c; measured Eγ, Iγ; deduced radiative muon capture branching ratio, weak pseudoscalar coupling.
doi: 10.1103/PhysRevC.57.373
1997HE11 Phys.Rev. C56, 922 (1997) R.K.Heaton, H.W.Lee, B.C.Robertson, E.B.Norman, K.T.Lesko, B.Sur α-Particle Induced γ-Ray Transitions in Light Elements NUCLEAR REACTIONS, ICPND 10B(α, p), (α, d), E=5.6-10 MeV; 11B(α, n), E=5.6-10 MeV; 19F(α, α'), (α, p), E=5.6-10 MeV; 23Na(α, n), (α, p), E=5.6-10 MeV; 24Mg(α, p), 25Mg(α, α'), (α, n), E ≤ 10 MeV; 26Mg(α, n), (α, p), E=5.6-10 MeV; 27Al(α, α'), E=10 MeV; 27Al(α, n), E=7-10 MeV; 27Al(α, p), E=5.6-10 MeV; 28Si(α, p), 29,30Si(α, n), (α, p), E=10 MeV; measured thick target residuals yields; deduced reaction mechanism related features. 28,29,30Si deduced excitation distribution vs Eα. Comparison of several models.
doi: 10.1103/PhysRevC.56.922
1996JO22 Phys.Rev.Lett. 77, 4512 (1996) G.Jonkmans, S.Ahmad, D.S.Armstrong, G.Azuelos, W.Bertl, M.Blecher, C.Q.Chen, P.Depommier, B.C.Doyle, T.von Egidy, T.P.Gorringe, P.Gumplinger, M.D.Hasinoff, D.Healey, A.J.Larabee, J.A.Macdonald, S.C.McDonald, M.Munro, J.-M.Poutissou, R.Poutissou, B.C.Robertson, D.G.Sample, E.Saettler, C.M.Sigler, G.N.Taylor, D.H.Wright, N.S.Zhang Radiative Muon Capture on Hydrogen and the Induced Pseudoscalar Coupling NUCLEAR REACTIONS 1H(μ-, γ), E at rest; measured photons partial branching ratio; deduced weak pseudoscalar coupling constant, related features.
doi: 10.1103/PhysRevLett.77.4512
1995HE40 Nucl.Instrum.Methods Phys.Res. A364, 317 (1995) R.K.Heaton, H.W.Lee, B.C.Robertson, E.B.Norman, K.T.Lesko, B.Sur α-Particle Induced High-Energy γ-Ray Yields from Light Elements NUCLEAR REACTIONS, ICPND 27Al, 24Mg, 10B, 19F(α, p), 10B(α, d), 11B, 19F, 25,26Mg, 27Al(α, n), E=5.6-10 MeV; measured thick target γ yields; deduced γ production intensity distributions from materials related features. Thick targets of Be also studied.
doi: 10.1016/0168-9002(95)00220-0
1992AR14 Phys.Rev. C46, 1094 (1992) D.S.Armstrong, A.Serna-Angel, S.Ahmad, G.Azuelos, W.Bertl, M.Blecher, C.Q.Chen, P.Depommier, T.von Egidy, T.P.Gorringe, M.D.Hasinoff, R.S.Henderson, A.J.Larabee, J.A.Macdonald, S.C.McDonald, J.-M.Poutissou, R.Poutissou, B.C.Robertson, D.G.Sample, G.N.Taylor, D.H.Wright, N.S.Zhang Radiative Muon Capture on Al, Si, Ca, Mo, Sn, and Pb NUCLEAR REACTIONS 27Al, 28Si, 40Ca, Mo, Sn, Pb(μ-, γ), E at rest; measured γ yield; deduced induced pseudoscalar coupling constant (g(p)).
doi: 10.1103/PhysRevC.46.1094
1992BE70 Z.Phys. C56, S150 (1992) W.Bertl, S.Ahmad, D.S.Armstrong, G.Azuelos, M.Blecher, C.Q.Chen, P.Depommier, P.Gumplinger, T.P.Gorringe, M.D.Hasinoff, R.Henderson, G.Jonkmans, A.J.Larabee, J.A.Macdonald, S.C.McDonald, J.-M.Poutissou, R.Poutissou, B.C.Robertson, D.G.Sample, W.Schott, G.N.Taylor, T.von Egidy, D.H.Wright, N.S.Zhang Radiative muon capture on hydrogen NUCLEAR REACTIONS 1H(π-, γ), (π-, π0), (μ-, X), (μ+, X), E at rest; measured Eγ, Iγ.
doi: 10.1007/BF02426790
1992FA03 Phys.Lett. 278B, 413 (1992) F.Farzanpay, P.Gumplinger, A.Stetz, J.-M.Poutissou, I.Blevis, M.Hasinoff, C.J.Virtue, C.E.Waltham, B.C.Robertson, T.Mulera, A.Shor, J.Lowe, S.H.Chew Measurement of the Slope of the π0 Electromagnetic Form Factor
doi: 10.1016/0370-2693(92)90577-Q
1991AR02 Phys.Rev. C43, 1425 (1991) D.S.Armstrong, S.Ahmad, R.A.Burnham, T.P.Gorringe, M.D.Hasinoff, A.J.Larabee, C.E.Waltham, G.Azuelos, J.A.Macdonald, T.Numao, J.-M.Poutissou, M.Blecher, D.H.Wright, E.T.H.Clifford, J.Summhammer, P.Depommier, R.Poutissou, H.Mes, B.C.Robertson Radiative Muon Capture on Carbon, Oxygen, and Calcium NUCLEAR REACTIONS 12C, 16O, 40Ca(μ-, γ), E at rest; measured Eγ, Iγ; deduced g(p)/g(a).
doi: 10.1103/PhysRevC.43.1425
1990AZ05 Ann.Phys.(Paris) 15, 13 (1990) G.Azuelos, S.Ahmad, D.S.Armstrong, W.Bertl, M.Blecher, R.A.Burnham, C.-Q.Chen, P.Depommier, T.von Egidy, T.P.Gorringe, M.D.Hasinoff, R.Henderson, A.J.Larabee, J.A.MacDonald, S.C.McDonald, J.-M.Poutissou, R.Poutissou, B.C.Robertson, A.Serna-Angel, G.N.Taylor, C.E.Waltham, D.H.Wright, N.-S.Zhang Capture Radiative des Muons sur les Noyaux et le Proton NUCLEAR REACTIONS 1H(μ-, ν), E at rest; analyzed capture reaction data; deduced g(P) inference features.
1990VI05 Nucl.Phys. A517, 509 (1990) C.J.Virtue, K.A.Aniol, F.E.Entezami, M.D.Hasinoff, D.Horvath, H.W.Roser, B.C.Robertson Photon Asymmetry in Radiative Muon Capture on Calcium NUCLEAR REACTIONS Ca(μ-, ν), E at rest; measured photon asymmetry; deduced g(p)/g(A). Natural target.
doi: 10.1016/0375-9474(90)90215-8
1989AR07 Phys.Rev. C40, R1100 (1989) D.S.Armstrong, S.Ahmad, R.A.Burnham, T.P.Gorringe, M.D.Hasinoff, A.J.Larabee, C.E.Waltham, G.Azuelos, J.A.Macdonald, J.-M.Poutissou, M.Blecher, D.H.Wright, E.T.H.Clifford, J.Summhammer, P.Depommier, R.Poutissou, H.Mes, B.C.Robertson Radiative Muon Capture on Oxygen and the Induced Pseudoscalar Coupling NUCLEAR REACTIONS 16O(μ-, γ), E at rest; measured γ spectrum. 16O deduced (gp/ga).
doi: 10.1103/PhysRevC.40.R1100
1989HE04 Nucl.Instrum.Methods Phys.Res. A276, 529 (1989) R.Heaton, H.Lee, P.Skensved, B.C.Robertson Neutron Production from Thick-Target (α, n) Reactions NUCLEAR REACTIONS, ICPND B, C, N, O, 19F, Li, 23Na, Mg, 27Al, Si, Fe(α, n), E=1-9.8 MeV; analyzed thick target neutron yields data.
doi: 10.1016/0168-9002(89)90579-2
1988BA40 Phys.Rev. C38, 875 (1988) A.Bagheri, K.A.Aniol, F.Entezami, M.D.Hasinoff, D.F.Measday, J.-M.Poutissou, M.Salomon, B.C.Robertson Reaction π-p → γn below the Δ Resonance NUCLEAR REACTIONS 1H(π-, γ), E=45.6-121.9 MeV; measured σ(θ), σ(E); deduced photomeson σ.
doi: 10.1103/PhysRevC.38.875
1988BA41 Phys.Rev. C38, 885 (1988) A.Bagheri, K.A.Aniol, F.Entezami, M.D.Hasinoff, D.F.Measday, J.-M.Poutissou, M.Salomon, B.C.Robertson Reaction π-p → π0n below the Δ Resonance NUCLEAR REACTIONS 1H(π-, π0), E=45.6-121.9 MeV; measured σ(θ), σ(E).
doi: 10.1103/PhysRevC.38.885
1987BR03 Nucl.Phys. A462, 527 (1987) The 1377 keV Level in 57Co NUCLEAR REACTIONS 56Fe(p, γ), E=1.6, 1.64 MeV; measured σ(E), Doppler shift. 57Co level deduced T(1/2). Pulsed beam-γ-delay timing.
doi: 10.1016/0375-9474(87)90402-7
1986KH01 Can.J.Phys. 64, 219 (1986) M.Khaliquzzaman, W.K.Dawson, H.W.Fielding, P.W.Green, R.L.Helmer, W.J.McDonald, G.C.Neilson, B.C.Robertson, D.M.Sheppard Energy Levels, Decay Scheme, Gamma-Ray Branching Ratios, and Lifetimes in 49V with (p, nγ) Reaction NUCLEAR REACTIONS 49Ti(p, nγ), E=5.74 MeV; measured Eγ, Iγ, γ(t). 49V deduced levels, γ-branching, J, π, T1/2.
doi: 10.1139/p86-040
1985AR14 Nucl.Phys. A441, 397 (1985) D.S.Armstrong, S.K.Saha, C.-W.Cheng, E.Adamides, A.Henrikson, M.A.Lone, B.C.Robertson Gamma-Ray Strength Function of 198Hg NUCLEAR REACTIONS, ICPND 197Au(p, γ), E=4 MeV; measured σ(Eγ); deduced γ-production σ. 198Hg deduced E1 γ-strength function. Natural target.
doi: 10.1016/0375-9474(85)90152-6
1984KH04 Nucl.Phys. A424, 191 (1984) M.Khaliquzzaman, W.K.Dawson, H.W.Fielding, P.W.Green, R.L.Helmer, W.J.McDonald, G.C.Neilson, B.C.Robertson, D.M.Sheppard Energy Levels, Decay Scheme, γ-Ray Branching Ratios and Lifetimes in 55Fe from the 55Mn(p, nγ)55Fe Reaction NUCLEAR REACTIONS 55Mn(p, nγ), E=4, 6 MeV; measured Eγ, Iγ, γ-time distribution. 55Fe deduced levels, decay scheme, γ-branching, T1/2. Natural targets.
doi: 10.1016/0375-9474(84)90181-7
1984SA03 Nucl.Phys. A414, 493 (1984) M.Salomon, D.F.Measday, J.-M.Poutissou, B.C.Robertson Radiative Capture and Charge Exchange of Negative Pions on Protons at 26.4 and 39.3 MeV NUCLEAR REACTIONS 1H(π-, γ), (π-, π0), E=27.4, 39.3 MeV; measured σ(θ); deduced pion-nucleon phase shifts, scattering lengths.
doi: 10.1016/0375-9474(84)90615-8
1984SI08 Phys.Rev.Lett. 53, 141 (1984) J.J.Simpson, P.Jagam, J.L.Campbell, H.L.Malm, B.C.Robertson New Limit for Neutrinoless Double β Decay of 76Ge RADIOACTIVITY 76Ge(2β); measured neutrinoless double β-decay T1/2. Large volume Ge detector.
doi: 10.1103/PhysRevLett.53.141
1982MU14 Phys.Rev. C26, 2698 (1982) S.F.Mughabghab, M.A.Lone, B.C.Robertson Quantitative Test of the Lane-Lynn Theory of Direct Radiative Capture of Thermal Neutrons by 12C and 13C NUCLEAR REACTIONS 12,13C(n, γ), E=thermal; measured σ(Eγ), Iγ; deduced capture mechanism. 12,13C levels deduced S.
doi: 10.1103/PhysRevC.26.2698
1981LO13 Nucl.Instrum.Methods 189, 515 (1981) M.A.Lone, A.J.Ferguson, B.C.Robertson Characteristics of Neutrons from Be Targets Bombarded with Protons, Deuterons and Alpha Particles NUCLEAR REACTIONS 9Be(p, n), E=9, 12, 14.8, 18, 23 MeV; 9Be(d, n), E=3, 5, 6, 7, 9, 12, 14.8, 23 MeV; 9Be(α, n), E=12, 20, 24, 30 MeV; measured σ(En), thick target yields.
doi: 10.1016/0029-554X(81)90438-9
1980SA07 Nucl.Phys. A339, 253 (1980) S.K.Saha, M.Maynard, B.C.Robertson Electromagnetic Properties of the 749 and 777 keV Levels in 51Cr NUCLEAR REACTIONS 51V(p, nγ), E=3.7 MeV; measured Eγ, Iγ. 51Cr levels deduced T1/2, δ , B(M1), B(E2). Pulsed-beam γ-delay timing.
doi: 10.1016/0375-9474(80)90091-3
1980SA14 Phys.Rev. C21, 2322 (1980) S.K.Saha, M.J.Maynard, B.C.Robertson, A.B.McDonald, E.D.Earle Gamma-Ray Lifetimes for Parity Doublets in 41K, 41Ca NUCLEAR REACTIONS 41K(p, p'γ), E=3.22 MeV; 40Ca(d, pγ), E=3 MeV; measured Eγ, Iγ, T1/2. 41K, 41Ca deduced doublet parity mixing. Direct timing, pulsed beam.
doi: 10.1103/PhysRevC.21.2322
1977CO03 J.Phys.(London) G3, 391 (1977) B.E.Cooke, J.R.Leslie, W.McLatchie, B.C.Robertson A Comparison of Two Independent Measurements of the Lifetime of a State in 59Cu NUCLEAR REACTIONS 58Ni(p, γ), E=1833, 3547 keV; measured σ(E, Eγ, θ), DSA. 59Cu deduced levels, resonances, J, T1/2, Γ.
doi: 10.1088/0305-4616/3/3/014
1977KO10 Phys.Rev. C16, 132 (1977) R.L.Kozub, B.E.Cooke, J.R.Leslie, B.C.Robertson Partial Widths and Gamma-Ray Decay of the 2883- and 5037-keV Levels in 41Sc NUCLEAR REACTIONS 40Ca(p, γ), E=1.84, 4.05 MeV; measured σ(Eγ, θ), polarization, Iγ; deduced Q. 41Sc deduced levels, J, π, Γγ, Γp, S, resonance strengths. Enriched target.
doi: 10.1103/PhysRevC.15.132
1976MA08 Nucl.Phys. A258, 131 (1976) D.J.Martin, W.McLatchie, B.C.Robertson, J.Szucs The 1g9/2 Analogue State in 55Co NUCLEAR REACTIONS 54Fe(p, γ), E=3.47 MeV; measured σ(E, Eγ, θ), Q, resonance strength. 55Co deduced M1, E1 rates, 9/2+ analog, antianalog states. Enriched target.
doi: 10.1016/0375-9474(76)90534-0
1975CO21 Can.J.Phys. 53, 2506 (1975) B.E.Cooke, J.R.Leslie, B.C.Robertson, W.McLatchie A Detailed Study of the g9/2 Analogue Resonance in 59Cu by the 58Ni(p, γ)59Cu Reaction NUCLEAR REACTIONS 58Ni(p, γ), E=3.5-3.6 MeV; measured σ(E, Eγ, θ). 59Cu deduced level, resonance, J, π, Γ.
doi: 10.1139/p75-304
1975FR22 Nucl.Phys. A255, 351 (1975) G.G.Frank, B.C.Robertson, W.McLatchie The Lifetime of the 8543 and 8945 keV Levels in 28Si NUCLEAR REACTIONS 27Al(p, γ), E=2.677, 3.096 MeV; measured Eγ, Doppler shift attenuation. 28Si levels deduced T1/2. Ge(Li) detector.
doi: 10.1016/0375-9474(75)90685-5
1975RO28 Can.J.Phys. 53, 2631 (1975) B.C.Robertson, M.Micklinghoff, B.Castel The 7/2- Doublet in 55Fe NUCLEAR REACTIONS 52Cr(α, nγ), E=6.75 MeV; 55Mn(p, nγ), E=3.6 MeV; measured DSA, Iγ. 55Fe levels deduced T1/2, γ-branching, μ.
doi: 10.1139/p75-322
1975TR05 Nucl.Phys. A246, 457 (1975) J.P.Trentelman, B.E.Cooke, J.R.Leslie, W.McLatchie, B.C.Robertson A Study of the 58Ni(p, γ)59Cu Reaction NUCLEAR REACTIONS 58Ni(p, γ), E=0.9-2.3 MeV; measured σ(E, Eγ, θ). 59Cu deduced levels, analog resonances, J, t, γ-mixing, γ-branching ratios.
doi: 10.1016/0375-9474(75)90659-4
1973CH25 Can.J.Phys. 51, 1840 (1973) W.-H.Chung, D.M.Sheppard, W.C.Olsen, B.C.Robertson Excited States in 53Mn by the 53Cr(p, nγ)53Mn Reaction NUCLEAR REACTIONS 53Cr(p, nγ), E=3.78-5.00 MeV; measured σ(E;Eγ, θ), DSA, nγ-coin. 53Mn deduced levels, J, π, γ-mixing, γ-branching, T1/2.
doi: 10.1139/p73-244
1973EL09 Nucl.Phys. A211, 493 (1973) S.A.Elbakr, I.J.Van Heerden, B.C.Robertson, W.J.McDonald, G.C.Neilson, W.K.Dawson The Energy Level Structure of 154Sm from the (n, n'γ) Reaction NUCLEAR REACTIONS 154Sm(n, n'γ), E=1.1-2.3 MeV; measured Eγ, σ(En;Eγ). 154Sm deduced levels, J, π, γ-branching. Enriched target; Ge(Li) detector.
doi: 10.1016/0375-9474(73)90439-9
1972RO16 Nucl.Phys. A189, 439 (1972) B.C.Robertson, G.C.Neilson, W.J.McDonald Hole States in 55Fe NUCLEAR REACTIONS 55Mn(p, nγ), E=3.6-5.5 MeV; measured DSA, pγ-delay, σ(E;Eγ). 55Fe levels deduced T1/2, γ-branching.
doi: 10.1016/0375-9474(72)90307-7
1972WH08 Nucl.Instrum.Methods 105, 29 (1972) Nuclear Resonance Fluorescence with a 5 Ci Pu-Be Radioactive Source NUCLEAR REACTIONS 63,65Cu(γ, γ), E < 4.44 MeV; measured nuclear resonance fluorescence. 63,65Cu levels deduced T1/2.
doi: 10.1016/0029-554X(72)90486-7
1972WO17 Nucl.Phys. A192, 279 (1972) E.Wong, B.C.Robertson, K.V.K.Iyengar, D.M.Sheppard, W.C.Olsen A Study of γ-Rays of 37Ar NUCLEAR REACTIONS 37Cl(p, nγ), E=3.25-5.90 MeV; measured σ(E;Eγ, En, θ(γ)), Doppler-shift attenuation. 37Ar deduced levels, T1/2, γ-branching ratios, J, π, γ-mixing. Enriched targets, neutron time-of-flight technique, Ge(Li) detector.
doi: 10.1016/0375-9474(72)90259-X
1971IY02 Nucl.Phys. A171, 73 (1971) Electromagnetic Properties of 45Ti Excited States NUCLEAR REACTIONS 45Sc(p, n), 45Sc(p, nγ);Ep=4.45-5.90 MeV; measured En, σ(E;Eγ, En, θ(γ)), Doppler shift attenuation. 45Ti deduced levels, T1/2, γ-branching ratios, J, γ-mixing. Natural target;neutron time-of-flight technique;Ge(Li) detector.
doi: 10.1016/0375-9474(71)90364-2
1971IY03 Nucl.Phys. A174, 385 (1971) Electromagnetic Properties of 51Cr Excited States NUCLEAR REACTIONS 51V(p, nγ), Ep=3.95-5.50 MeV; measured σ(E;Eγ, En, θ(γ)), Doppler shift attenuation. 51Cr levels deduced T1/2, J, γ-mixing. Natural target;Ge(Li) detector.
doi: 10.1016/0375-9474(71)90671-3
1971RO01 Nucl.Phys. A160, 137 (1971) B.C.Robertson, T.P.G.Carola, D.M.Sheppard, W.C.Olsen Electromagnetic Properties of 55Fe NUCLEAR REACTIONS 55Mn(p, nγ), Ep=3.60-5.50 MeV; measured σ(E;Eγ, En, θ(γ)), Doppler shift attenuation. 55Fe deduced levels, T1/2, γ-branching ratios, J, γ-mixing. Natural target; Ge(Li) detector.
doi: 10.1016/0375-9474(70)90178-8
1971RO27 Nucl.Phys. A176, 193 (1971) B.C.Robertson, I.J.van Heerden, W.J.McDonald Properties of Excited States in 48Sc NUCLEAR REACTIONS 48Ca(p, nγ), Ep=2.6 to 3.9 MeV; measured σ(E;Eγ, θ(γ)), Eγ, Iγ. 48Sc deduced levels, J, γ-branching, γ-mixing. Enriched target;Ge(Li) detector.
doi: 10.1016/0375-9474(71)90740-8
1971RO28 Phys.Rev. C4, 2176 (1971) B.C.Robertson, J.T.Sample, D.R.Goosman, K.Nagatani, K.W.Jones Elastic Scattering of 16,18O by 116,120Sn at Energies Near the Coulomb Barrier NUCLEAR REACTIONS 116,120Sn(16O, 16O), (18O, 18O), E=58 MeV, E=45-67.5 MeV; measured σ(θ), σ(E); deduced optical model parameters.
doi: 10.1103/PhysRevC.4.2176
1971RO29 Can.J.Phys. 49, 3051 (1971) 39K 2.82 MeV Level NUCLEAR STRUCTURE 39K 2.82 MeV level deduced M2, E3 level-width from available data.
doi: 10.1139/p71-361
1970GI09 Nucl.Phys. A152, 369 (1970) R.D.Gill, K.Bharuth-Ram, K.P.Jackson, R.A.I.Bell, B.C.Robertson, J.L'Ecuyer, N.G.Chapman, H.J.Rose Electromagnetic Transitions in 19Ne NUCLEAR REACTIONS 19F(p, n), E=8.48-10.4 MeV; 16O(α, n), E=15-19 MeV; measured σ(E;En, Eγ, θ(nγ)), Doppler shift attenuation. 19Ne deduced levels, T1/2, branching ratios, J, π, γ-mixing. Natural targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(70)90837-7
1969BE31 Nucl.Phys. A133, 337(1969) R.A.L.Bell, J.L'Ecuyer, R.D.Gill, B.C.Robertson, I.S.Towner, H.J.Rose Excitation Energies and Lifetimes of Levels in 26Si NUCLEAR REACTIONS 24Mg(3He, nγ); E = 5.5, 7.8, 10 MeV; measured σ(E; Eγ, θ(n), θ(p)), γγ-coin, Doppler shift attenuation. 26Si deduced levels, T1/2 branching ratios, J, π, transition strengths. Enriched (99.8%) target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90636-8
1969RO08 Nucl.Phys. A126, 431(1969) B.C.Robertson, R.A.I.Bell, J.L'Ecuyer, R.D.Gill, H.J.Rose A Study of the Gamma Rays in 18Ne NUCLEAR REACTIONS 16O(3He, n); E=8.5-13.15 MeV; measured σ(Eγ, θ(nγ)), Eγ, Doppler shift attenuation. 18Ne deduced levels, T1/2, γ-branching ratios, J, delta. Natural target; Ge(Li) detector.
doi: 10.1016/0375-9474(69)90477-1
1969RO15 Nucl.Phys. A132, 481 (1969) B.C.Robertson, R.D.Gill, R.A.I.Bell, J.L'Ecuyer, H.J.Rose Lifetimes of 39K Excited States: the 2s1/2 Hole State NUCLEAR REACTIONS 39K(p, p'), E=8.175 MeV; measured Eγ, Doppler shift attenuation. 39K levels deduced T1/2. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90713-1
1968BE30 Nucl.Phys. A118, 481(1968) R.A.I.Bell, R.D.Gill, B.C.Robertson, J.S.Lopes, H.J.Rose Electromagnetic Transitions in 11B and 14C NUCLEAR REACTIONS 12C(t, α), (t, p), E=7.48, 7.68 MeV; measured Iγ(Eα, Eγ, θ(αγ)), Iγ(Ep, Eγ, θ(pγ)). 11B, 14C levels; deduced J, γ-branching, delta. Natural target.
doi: 10.1016/0375-9474(68)90434-X
1968GI01 Nucl.Phys. A106, 678 (1968) R.D.Gill, J.S.Lopes, B.C.Robertson, R.A.I.Bell, H.J.Rose A Study of Positive-Parity States in 15O NUCLEAR REACTIONS 16O(3He, αγ), E = 9.1 MeV; measured σ(Eα, Eγ, θ(αγ)). 15O levels deduced J, delta. Natural target.
doi: 10.1016/0375-9474(68)90523-X
1968GI09 Phys.Letters 28B, 116 (1968) R.D.Gill, B.C.Robertson, J.L'Ecuyer, R.A.I.Bell, H.J.Rose Lifetime Measurements in 18Ne NUCLEAR REACTIONS 16O(3He, nγ), E=12 MeV; measured nγ-coin, Doppler shift attenuation. 18Ne deduced levels, J, π, T1/2.
doi: 10.1016/0370-2693(68)90146-9
1968LO03 Nucl.Phys. A109, 241(1968) J.S.Lopes, B.C.Robertson, R.D.Gill, R.A.I.Bell, H.J.Rose Electromagnetic Properties of 39K Bound States NUCLEAR REACTIONS 42Ca(p, αγ), E=10.6-11.1 MeV; 39K(p, p'γ), E=7.12-8.51 MeV; measured σ(E; Eγ, θ(γ)). 39K, deduced J, multipole mixing ratios. Enriched targets.
doi: 10.1016/0375-9474(68)90592-7
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