NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = A.B.McDonald Found 84 matches. 2016AM03 Astropart.Phys. 85, 1 (2016) P.-A.Amaudruz, M.Batygov, B.Beltran, J.Bonatt, K.Boudjemline, M.G.Boulay, B.Broerman, J.F.Bueno, A.Butcher, B.Cai, T.Caldwell, M.Chen, R.Chouinard, B.T.Cleveland, D.Cranshaw, K.Dering, F.Duncan, N.Fatemighomi, R.Ford, R.Gagnon, P.Giampa, F.Giuliani, M.Gold, V.V.Golovko, P.Gorel, E.Grace, K.Graham, D.R.Grant, R.Hakobyan, A.L.Hallin, M.Hamstra, P.Harvey, C.Hearns, J.Hofgartner, C.J.Jillings, M.Kuzniak, I.Lawson, F.La Zia, O.Li, J.J.Lidgard, P.Liimatainen, W.H.Lippincott, R.Mathew, A.B.McDonald, T.McElroy, K.McFarlane, D.N.McKinsey, R.Mihdiyev, J.Monroe, A.Muir, C.Nantais, K.Nicolics, J.Nikkel, A.J.Noble, E.O'Dwyer, K.Olsen, C.Ouellet, P.Pasuthip, S.J.M.Peeters, T.Pollmann, W.Rau, F.Retiere, M.Ronquest, N.Seeburn, P.Skensved, B.Smith T.Sonley, J.Tang, E.Vazquez-Jauregui, L.Veloce, J.Walding, M.Ward, K.Olsen, C.Ouellet, P.Pasuthip, S.J.M.Peeters, T.Pollmann, W.Rau, F.Retiere, M.Ronquest, N.Seeburn, P.Skensved, B.Smith, T.Sonley, J.Tang, E.Vazquez-Jauregui, L.Veloce, J.Walding, M.Ward Measurement of the scintillation time spectra and pulse-shape discrimination of low-energy β and nuclear recoils in liquid argon with DEAP-1 NUCLEAR REACTIONS Ar(n, n), E<100 keV; measured nuclear recoils, Eβ, Iβ; deduced pulse-shape discrimination of recoils. Implications for dark matter sensitivities.
doi: 10.1016/j.astropartphys.2016.09.002
2016MC04 Ann.Phys.(Leipzig) 528, 469 (2016) The Sudbury Neutrino Observatory: Observation of flavor change for solar neutrinos
doi: 10.1002/andp.201600031
2016MC06 Rev.Mod.Phys. 88, 030502 (2016) Nobel Lecture: The Sudbury Neutrino Observatory: Observation of flavor change for solar neutrinos
doi: 10.1103/RevModPhys.88.030502
2005MC06 Nucl.Phys. A751, 53c (2005) Evidence for Neutrino Oscillations I: Solar and Reactor Neutrinos
doi: 10.1016/j.nuclphysa.2005.02.102
2003MC03 Nucl.Phys. A721, 104c (2003) Summary of solar neutrino measurements
doi: 10.1016/S0375-9474(03)01022-4
2002DR03 Nucl.Instrum.Methods Phys.Res. A481, 284 (2002) M.R.Dragowsky, A.Hamer, Y.D.Chan, R.Deal, E.D.Earle, W.Frati, E.Gaudette, A.Hallin, C.Hearns, J.Hewett, G.Jonkmans, Y.Kajiyama, A.B.McDonald, B.A.Moffat, E.B.Norman, B.Sur, N.Tagg The 16N Calibration Source for the Sudbury Neutrino Observatory RADIOACTIVITY 16N(β-) [from 16O(n, p)]; measured Eγ, Iγ. Application to calibration of neutrino detector discussed.
doi: 10.1016/S0168-9002(01)02062-9
1996MC06 Nucl.Phys. B(Proc.Suppl.) S48, 357 (1996) Future Solar Neutrino Experiments
doi: 10.1016/0920-5632(96)00272-1
1990CO09 Nucl.Instrum.Methods Phys.Res. A288, 463 (1990) K.P.Coulter, T.E.Chupp, A.B.McDonald, C.D.Bowman, J.D.Bowman, J.J.Szymanski, V.Yuan, G.D.Cates, D.R.Benton, E.D.Earle Neutron Polarization with a Polarized 3He Spin Filter NUCLEAR REACTIONS 139La(polarized n, X), E=low; measured transmission; deduced helicity dependence on 140La resonance. Polarized 3He spin filter.
doi: 10.1016/0168-9002(90)90139-W
1989CH01 Phys.Rev. C39, 248 (1989) A.E.Champagne, R.T.Kouzes, A.B.McDonald, M.M.Lowry, D.R.Benton, K.P.Coulter, Z.Q.Mao 127I(3He, t)127Xe Reaction with Relevance to Neutrino Detection NUCLEAR REACTIONS 127I(3He, t), E=29.78 MeV; measured σ(Et); deduced 127I neutrino capture relevant information.
doi: 10.1103/PhysRevC.39.248
1988CH25 Phys.Rev. C38, 900 (1988) A.E.Champagne, G.E.Dodge, R.T.Kouzes, M.M.Lowry, A.B.McDonald, M.W.Roberson Gamma Decays of Isobaric Analog States Relevant to Neutrino Detection NUCLEAR REACTIONS 81Br, 27Al, 71Ga(3He, t), E=29.9 MeV; 27Al(3He, d), E=29.9 MeV; measured σ(Et), σ(Ed), Eγ, Iγ, γt-, γd-coin. 71Ge, 81Kr deduced IAS γ-branching ratios, neutron decay dominance.
doi: 10.1103/PhysRevC.38.900
1988CH38 Phys.Rev. C38, 2430 (1988) A.E.Champagne, R.T.Kouzes, M.M.Lowry, A.B.McDonald, Z.Q.Mao Decay of the First Isobaric Analog State in 69Ge NUCLEAR REACTIONS 69Ga(3He, t), E=29.8 MeV; measured σ(Et). 69Ge deduced IAS α-decay branching ratio. Natural target.
doi: 10.1103/PhysRevC.38.2430
1988EA01 Can.J.Phys. 66, 534 (1988) E.D.Earle, A.B.McDonald, S.H.Kidner, E.T.H.Clifford, J.J.Hill, G.H.Keech, T.E.Chupp, M.B.Schneider Measurement of Parity Violation in the Photodisintegration of Deuterium and in the Production of Bremsstrahlung on Tantalum NUCLEAR REACTIONS 2H(polarized γ, np), E=4.1 MeV bremsstrahlung; measured CP dependent photodisintegration σ component; deduced parity dependent observables.
doi: 10.1139/p88-089
1987LO06 Phys.Rev. C35, 1950 (1987) M.M.Lowry, R.T.Kouzes, F.Loeser, A.B.McDonald, R.A.Naumann Electron Capture Decay of 81mKr RADIOACTIVITY 81mKr(EC) [from 81Rb(β++EC)-decay]; measured E X-ray, I X-ray, (ce)(X-ray)-coin; deduced log ft, solar neutrino capture rate reduction. 81Br deduced EC-branching ratio.
doi: 10.1103/PhysRevC.35.1950
1987PA07 Phys.Rev. C35, 1119 (1987) S.A.Page, H.C.Evans, G.T.Ewan, S.-P.Kwan, J.R.Leslie, J.D.MacArthur, W.McLatchie, P.Skensved, S.-S.Wang, H.-B.Mak, A.B.McDonald, C.A.Barnes, T.K.Alexander, E.T.H.Clifford Weak Pion-Nucleon Coupling Strength: New constraint from parity mixing in 18F NUCLEAR REACTIONS 16O(3He, p), E=4.05 MeV; measured γ CP; deduced weak pion-nucleon coupling strength. 19F levels deduced parity mixing.
doi: 10.1103/PhysRevC.35.1119
1986CH09 Nucl.Phys. A451, 498 (1986) A.E.Champagne, A.B.McDonald, T.F.Wang, A.J.Howard, P.V.Magnus, P.D.Parker Threshold States in 26Al Revisited NUCLEAR REACTIONS 27Al(3He, α), 25Mg(3He, d), E=20 MeV; measured σ(E), dγ-coin. 26Al deduced levels, Γp. Enriched target.
doi: 10.1016/0375-9474(86)90073-4
1986YU01 Phys.Rev.Lett. 57, 1680 (1986) V.Yuan, H.Frauenfelder, R.W.Harper, J.D.Bowman, R.Carlini, D.W.MacArthur, R.E.Mischke, D.E.Nagle, R.L.Talaga, A.B.McDonald Measurement of Parity Nonconservation in the Proton-Proton Total Cross Section at 800 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=800 MeV; measured longitudinal asymmetry; deduced parity nonconservation in σ. Liquid hydrogen unpolarized target, integrating ion chambers.
doi: 10.1103/PhysRevLett.57.1680
1985BE01 Phys.Rev. C31, 197 (1985) C.L.Bennett, A.B.McDonald, P.T.Springer, T.E.Chupp. M.L.Tate Measurements of Atomic Level Widths in Thulium: Effect on the measurement of neutrino mass from tritium beta decay spectra RADIOACTIVITY 169Yb(EC); measured E X-ray, I X-ray; deduced 169Tm atomic level widths. 3H(β-); analyzed β-spectra; deduced neutrino mass limits.
doi: 10.1103/PhysRevC.31.197
1985CH06 Phys.Rev. C31, 1023 (1985) T.E.Chupp, R.T.Kouzes, A.B.McDonald, P.D.Parker, T.F.Wang, A.Howard Total Width of the 5.17 MeV 1- State in 14O and the Hot-CNO Cycle NUCLEAR REACTIONS 14N(3He, t), E=29.8 MeV; measured residual, triton momentum spectra. 14O level deduced Γ, Γγ/Γ, γ-branching ratio.
doi: 10.1103/PhysRevC.31.1023
1985EV03 Phys.Rev.Lett. 55, 791 (1985) H.C.Evans, G.T.Ewan, S.-P.Kwan, J.R.Leslie, J.D.MacArthur, H.-B.Mak, W.McLatchie, S.A.Page, P.Skensved, S.-S.Wang, A.B.McDonald, C.A.Barnes, T.K.Alexander, E.T.H.Clifford Parity Mixing of 0+ and 0- Levels in 18F NUCLEAR REACTIONS 16O(3He, p), E=4.05 MeV; measured Eγ, Iγ, γ CP; deduced weak pion-nucleon coupling constant. 18F transition deduced parity nonconserving matrix element.
doi: 10.1103/PhysRevLett.55.791
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
1983EA01 Nucl.Phys. A396, 221c (1983) E.D.Earle, A.B.McDonald, E.G.Adelberger, K.A.Snover, H.E.Swanson, R.von Lintig, H.B.Mak, C.A.Barnes Parity Mixing in 21Ne; Evidence for weak neutral currents in nuclei NUCLEAR STRUCTURE 18,19F, 21Ne; analyzed data; deduced isoscalar, isovector weak nucleon-nucleon coupling constants. NUCLEAR REACTIONS 21Ne(p, p'γ), E=4.08 MeV; measured Eγ, Iγ, γ CP; deduced isoscalar, isovector weak nucleon-nucleon coupling constants. 21Ne levels deduced parity mixing matrix element. Parity mixing input from 19,18F data.
doi: 10.1016/0375-9474(83)90021-0
1983KN10 Nucl.Phys. A411, 195 (1983) D.A.Knapp, A.B.McDonald, C.L.Bennett Measurement of the Electron Capture Branching Ratio of 7Be Using Internal Bremsstrahlung RADIOACTIVITY 7Be(EC); measured internal bremsstrahlung spectra. 7Li levels deduced EC branching ratios.
doi: 10.1016/0375-9474(83)90387-1
1981MC14 Phys.Rev.Lett. 47, 1720 (1981) A.B.McDonald, E.D.Earle, J.J.Simpson, R.G.H.Robertson, H.B.Mak Measurement of Pair Emission from the 2.8-MeV Parity-Mixed Doublet of 21Ne RADIOACTIVITY 21Ne [from 18O(α, n), E=4.48, 4.85, 4.95 MeV]; measured pair emission relative branching ratios. 21Ne transition deduced γ-multipolarity, δ lower limit.
doi: 10.1103/PhysRevLett.47.1720
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
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
1979FR04 Phys.Rev. C19, 1907 (1979) S.J.Freedman, C.A.Gagliardi, M.A.Oothoudt, A.V.Nero, R.G.H.Robertson, F.J.Zutavern, E.G.Adelberger, A.B.McDonald Decays of the Lowest T = 2 States in A = 4N Nuclei from 8Be to 44Ti NUCLEAR REACTIONS 10Be, 14C, 18O, 26Mg, 30Si, 34S, 38Ar, 42Ca, 46Ti(p, t), E=42, 46 MeV; measured t-charged particle-coin, tnγ-coin. 8Be, 12C, 16O, 24Mg, 28Si, 32S, 36Ar, 40Ca, 44Ti deduced lowest J=0, T=2 positive parity level, systematics of isospin forbidden decay widths.
doi: 10.1103/PhysRevC.19.1907
1979IK02 Nucl.Phys. A319, 109 (1979) P.G.Ikossi, K.A.Snover, J.L.Osborne, E.G.Adelberger, A.B.McDonald The α-Width of the Lowest T = 2 State in 28Si NUCLEAR REACTIONS 24Mg(α, α), E=5.9-6.25 MeV; measured σ(Eα, θ). 28Si deduced resonances, L, J, π, Γ, Γα, T. Enriched target.
doi: 10.1016/0375-9474(79)90174-X
1979KI12 Nucl.Phys. A327, 172 (1979) W.E.Kieser, R.E.Azuma, I.Berka, K.P.Jackson, A.B.McDonald, H.B.Mak, W.McLatchie The Jπ = 3- Doublet at E = 6241 keV in 18F: Isospin Mixing NUCLEAR REACTIONS 4He(14N, α), E=8.19-8.32 MeV; measured Iα(E, θ). 14N(α, γ), E=2.35, 2.53 MeV; measured Eγ, Iγ(θ), absolute strength of γ-transition. 17O(p, γ), E=0.67 MeV; measured Eγ, Iγ(θ), absolute strength of γ-transition. 17O(p, α), E=0.67 MeV; measured Iα, absolute strength of γ-transition. 18F levels deduced J, π, Eα, T, Γp, Γα, Γγ. Natural, enriched targets.
doi: 10.1016/0375-9474(79)90323-3
1979SJ01 Phys.Rev. C20, 960 (1979) T.P.Sjoreen, U.Garg, D.B.Fossan, J.R.Beene, T.K.Alexander, E.D.Earle, O.Hausser, A.B.McDonald High-Spin States in the Odd-Odd Nucleus 212At NUCLEAR REACTIONS 208Pb(7Li, 3n), E=32-44 MeV; measured Eγ, Iγ, γγ-coin, γ(θ, H, t), γ(t), Iγ(θ). 212At deduced levels, J, π, T1/2, g, δ, B(λ), configurations.
doi: 10.1103/PhysRevC.20.960
1978BE17 Phys.Rev. C17, 1359 (1978) J.R.Beene, O.Hausser, T.K.Alexander, A.B.McDonald Electromagnetic Properties of Particle-Vibration Coupling States in 209Bi NUCLEAR REACTIONS 208Pb(7Li, 2nαγ), E=36 MeV; measured Eγ, γγ-coin, γ(θ, H, t). 209Bi deduced levels, J, π, T1/2, g, δ. Ge(Li) detectors.
doi: 10.1103/PhysRevC.17.1359
1978FR10 Phys.Rev. C17, 2071 (1978) S.J.Freedman, C.A.Gagliardi, M.A.Oothoudt, A.V.Nero, R.G.H.Robertson, F.J.Zutavern, E.G.Adelberger, A.B.McDonald Decays of the Lowest T = 2 State in 44Ti NUCLEAR REACTIONS 46Ti(p, t), E=42 MeV; measured tγ-coin, tα-coin. 44Ti levels deduced Γγ/Γ, Γα/Γ.
doi: 10.1103/PhysRevC.17.2071
1978HA50 Hyperfine Interactions 4, 219 (1978) O.Hausser, J.R.Beene, T.Faestermann, T.K.Alexander, D.Horn, A.B.McDonald, A.J.Ferguson Knight Shifts and Absolute Magnetic Moments in Trans-Bismuth Nuclei NUCLEAR REACTIONS 204Hg(13C, 5n), E=78 MeV; measured σ(θ, H, t); deduced Knight shift for Rn in Hg. 212Rn deduced levels, configuration, g, γ-branching, γ-multipolarity. 214Ra, 212,213Fr, 207Rn level deduced g.
1978MC04 Phys.Rev.Lett. 40, 1692 (1978) Schematic Model for Isospin Mixing in Light Nuclei NUCLEAR STRUCTURE 36Ar, 32S, 28Si, 24Mg, 20Ne, 16O, 12C, 8Be, 4He; calculated isospin mixing matrix elements.
doi: 10.1103/PhysRevLett.40.1692
1978MC07 Nucl.Phys. A305, 151 (1978) A.B.McDonald, E.D.Earle, W.McLatchie, H.B.Mak, D.J.Martin, P.G.Ikossi Isospin-Forbidden Particle Decays in Light Nuclei (IV). Total Width of the Lowest T = 2 Level of 24Mg NUCLEAR REACTIONS 23Na(p, γ), (p, p), (p, α), E ≈ 3.9 MeV; measured σ(E). 24Mg deduced lowest T=2, J, π=0+ level, total Γ.
doi: 10.1016/0375-9474(78)90169-0
1978RO08 Phys.Rev. C17, 1535 (1978) R.G.H.Robertson, T.L.Khoo, G.M.Crawley, A.B.McDonald, E.G.Adelberger, S.J.Freedman Mass of Lowest T = 2 State of 12C NUCLEAR REACTIONS 14C(p, t), E ≈ 45 MeV; measured σ; deduced Q. 12C deduced level, T, Γ. 12C(p, t), E=45 MeV; measured σ; deduced Q. 10C deduced level.
doi: 10.1103/PhysRevC.17.1535
1978SN01 Phys.Rev.Lett. 41, 145 (1978) K.A.Snover, R.von Lintig, E.G.Adelberger, H.E.Swanson, T.A.Trainor, A.B.McDonald, E.D.Earle, C.A.Barnes Upper Limit on Parity Mixing in 21Ne NUCLEAR REACTIONS 21Ne(p, p'), E=4.08 MeV; measured parity nonconserving γ-CP. 21Ne levels deduced parity-mixing matrix element.
doi: 10.1103/PhysRevLett.41.145
1977BE56 Hyperfine Interactions 3, 397 (1977) J.R.Beene, O.Hausser, A.B.McDonald, T.K.Alexander, A.J.Ferguson, B.Herskind Knight Shifts and Absolute Magnetic Moments of (h9/2)n Proton States in Trans-Bismuth Nuclei NUCLEAR REACTIONS 205Tl, 206Pb(12C, 4nγ), E=78 MeV; 203Tl(13C, 4nγ), E=78 MeV; measured Eγ, γγ-coin, γ(θ, H, t). 212,213Fr deduced levels, J, π, T1/2, g, Knight shift. 214Ra level deduced T1/2, Knight shift.
1977HO17 Phys.Rev.Lett. 39, 389 (1977) D.Horn, O.Hausser, T.Faestermann, A.B.McDonald, T.K.Alexander, J.R.Beene, C.J.Herrlander Core-Excited High-Spin Isomers in 212Rn NUCLEAR REACTIONS 204Hg(13C, 5n), E=72-85 MeV; measured Iγ(E, t), γγ-coin, γ(θ), linear polarization. 212Rn deduced levels, J, π, T1/2, λ, δ, g.
doi: 10.1103/PhysRevLett.39.389
1977LO10 Nucl.Instrum.Methods 143, 331 (1977) M.A.Lone, C.B.Bigham, J.S.Fraser, H.R.Schneider, T.K.Alexander, A.J.Ferguson, A.B.McDonald Thick Target Neutron Yields and Spectral Distributions from the 7Li(dp, n) and 9Be(dp, n) Reactions NUCLEAR REACTIONS 7Li, 9Be(p, n), (d, n), E=15, 18, 23 MeV; measured thick target yields.
doi: 10.1016/0029-554X(77)90616-4
1977MC05 Nucl.Phys. A281, 325 (1977) A.B.McDonald, E.D.Earle, M.A.Lone, F.C.Khanna, H.C.Lee Doubly Radiative Thermal Neutron Capture in 2H and 16O: Experiment and Theory NUCLEAR REACTIONS 2H, 16O(n, γ), E=th; measured σ(Eγ); deduced upper limit for σ(2γ). 17O levels deduced γ-branching. Enriched target.
doi: 10.1016/0375-9474(77)90029-X
1977MC08 Nucl.Phys. A287, 189 (1977) A.B.McDonald, T.K.Alexander, J.R.Beene, J.C.Hardy, K.P.Jackson, H.B.Mak Search for a 0+ Level Near the 8.87 Mev, 2- Level of 16O NUCLEAR REACTIONS 4He(12C, α), 6.76 < E < 7.0 MeV; measured excitation functions. 16O deduced no resonance. Differentially pumped target.
doi: 10.1016/0375-9474(77)90571-1
1977MC10 Nucl.Phys. A288, 529 (1977) A.B.McDonald, T.K.Alexander, J.R.Beene, H.B.Mak The Low Solar Neutrino Flux: A Search for a Resonance in 6Be NUCLEAR REACTIONS 4He(3He, n), E=38.61 MeV; measured σ(θ), neutron tof.
doi: 10.1016/0375-9474(77)90348-7
1976CO02 Nucl.Phys. A256, 277 (1976) G.J.Costa, T.K.Alexander, J.S.Forster, A.B.McDonald, I.S.Towner Recoil-Distance Lifetime Measurements of Levels in 36Ar and 36Cl NUCLEAR REACTIONS 2H(35Cl, n), 2H(35Cl, p), E=60 MeV; measured Eγ, Iγ, recoil distance. 36Cl levels deduced T1/2, γ-branching, B(λ). 36Ar levels deduced, T1/2, B(λ).
doi: 10.1016/0375-9474(76)90109-3
1976EA04 Phys.Rev. C14, 1298 (1976) E.D.Earle, A.B.McDonald, M.A.Lone Upper Limit for the 1H(n, γγ)2H Cross Section NUCLEAR REACTIONS 1H(n, γ), E=th; measured σ(2γ). Ge(Li) detectors.
doi: 10.1103/PhysRevC.14.1298
1976HA37 Phys.Lett. 63B, 279 (1976) O.Hausser, J.R.Beene, A.B.McDonald, T.K.Alexander, E.D.Earle, F.C.Khanna, I.S.Towner, G.A.Beer, A.Olin Precise Magnetic Moments of (h9/2)n Proton States NUCLEAR REACTIONS 205Tl(12C, 4n), E=71-80 MeV; measured γγ(θ, H, t). Fr, Ra recoils in Tl Knight shift. 213Fr deduced levels, T1/2, B(λ), g. 214Ra level deduced g.
doi: 10.1016/0370-2693(76)90263-X
1976HA44 Phys.Lett. 64B, 273 (1976) O.Hausser, J.R.Beene, T.K.Alexander, A.B.McDonald, T.Faestermann Isomeric Yrast States in 206Tl NUCLEAR REACTIONS 204Hg(7Li, nαγ), E=37 MeV; measured γ(t), γγ(t), γγ(θ, H, t). 206Tl deduced levels, T1/2, g.
doi: 10.1016/0370-2693(76)90199-4
1976HA56 Nucl.Phys. A273, 253 (1976) O.Hausser, T.K.Alexander, J.R.Beene, E.D.Earle, A.B.McDonald, F.C.Khanna, I.S.Towner Magnetic Moments and Half-Lives of Isomeric States in Polonium Isotopes NUCLEAR REACTIONS 206,207,208Pb(α, 2n), E=35-30 MeV; 194Pt(12C, 4n), E=80 MeV; measured Iγ(γ, H, t). 202,208,209,210Po levels deduced g, T1/2. 209Bi deduced quadrupole moment. Natural Pb, enriched 194Pt targets. Ge(Li) detectors. RADIOACTIVITY 210At; measured γγ(t). 210Po levels deduced T1/2.
doi: 10.1016/0375-9474(76)90312-2
1976HA62 Hyperfine Interactions 2, 334 (1976) O.Hausser, T.K.Alexander, J.R.Beene, E.D.Earle, A.B.McDonald, F.C.Khanna, I.S.Towner Measurements of Accurate g-Factors in Translead Nuclei with Heavy-Ion Induced Reactions
1976LE27 Phys.Lett. 65B, 201 (1976) H.C.Lee, F.C.Khanna, M.A.Lone, A.B.McDonald Doubly Radiative Neutron Capture by 2H, 3He, 16O and 208Pb NUCLEAR REACTIONS 2H, 3He, 16O, 208Pb(n, γ), E=th; calculated σ(2γ), σ(2γ)/σ(γ).
doi: 10.1016/0370-2693(76)90162-3
1976MC02 Nucl.Phys. A258, 152 (1976) A.B.McDonald, T.K.Alexander, C.Broude, J.S.Forster, O.Hausser, F.C.Khanna, I.V.Mitchell Lifetime of the 1.89 MeV 2+ Level of 18Ne: Two-Body Contributions to E2 Transition Rates NUCLEAR REACTIONS 3He(16O, nγ), E=38 MeV; measured nγ-coin, Doppler broadened line shape. 18Ne level deduced T1/2, B(E2).
doi: 10.1016/0375-9474(76)90536-4
1976MC10 Nucl.Phys. A273, 451 (1976) A.B.McDonald, T.K.Alexander, O.Hausser, D.Disdier, E.G.Adelberger, H.B.Mak, A.P.Shukla, A.V.Nero Isospin-Forbidden Particle Decays in Light Nuclei (I). T = 3/2 Levels of 9Be, 9B NUCLEAR REACTIONS 7Li(3He, n), (3He, p), E=8.25 11 MeV; measured np-, pn-coin. 9Be deduced Γn/Γ. 9B deduced Γp/Γ. Enriched target.
doi: 10.1016/0375-9474(76)90603-5
1976MC11 Nucl.Phys. A273, 464 (1976) A.B.McDonald, T.K.Alexander, O.Hausser Isospin-Forbidden Particle Decays in Light Nuclei (II). Widths of T = 3/2 Levels of 17O NUCLEAR REACTIONS 13C(α, n), E=4.2-8.7 MeV; measured σ(E, En, θ). 17O deduced T=3/2 levels, Γ. Enriched target.
doi: 10.1016/0375-9474(76)90604-7
1976MC12 Nucl.Phys. A273, 477 (1976) A.B.McDonald, H.B.Mak, H.C.Evans, G.T.Ewan, H.B.Trautvetter Isospin-Forbidden Particle Decays in Light Nuclei (III). Decay Widths of the Lowest T = 3/2 Level of 21Ne NUCLEAR REACTIONS 17O(α, n), (α, nγ), E=1.4-2.3 MeV; measured n, γ yields. 21Ne deduced T=3/2 levels, Γ, Γα, Γn. Enriched target.
doi: 10.1016/0375-9474(76)90605-9
1975EA04 Phys.Rev.Lett. 35, 908 (1975) E.D.Earle, A.B.McDonald, O.Hausser, M.A.Lone Search for Two-Photon Decay in Thermal np Capture NUCLEAR REACTIONS 1H(n, γ), E=thermal; measured upper limit for branching ratio of two-photon decay.
doi: 10.1103/PhysRevLett.35.908
1975MA34 Phys.Rev. C12, 1158 (1975) H.-B.Mak, H.C.Evans, G.T.Ewan, A.B.McDonald, T.K.Alexander Radiative Decay of the Second Excited State of 12C NUCLEAR REACTIONS 13C(3He, α), E=4.0 MeV; measured α-12C coin. 12C level deduced Γ(rad)/Γ. Enriched target.
doi: 10.1103/PhysRevC.12.1158
1975WI01 Nucl.Phys. A238, 141 (1975) W.Witthuhn, O.Hausser, D.B.Fossan, A.B.McDonald, A.Olin The Magnetic Moment of the 8+ State in 212Rn NUCLEAR REACTIONS 204Hg(12C, 4n), E=70 MeV; measured γ(θ, H, t). 212Rn level deduced g. Enriched target.
doi: 10.1016/0375-9474(75)90344-9
1974AL07 Phys.Rev. C9, 1748 (1974) T.K.Alexander, G.J.Costa, J.S.Forster, O.Hausser, A.B.McDonald, A.Olin, W.Witthuhn Magnetic Moment of the 97-ps, Iπ = 3- Level in 14C NUCLEAR REACTIONS 3H(12C, p), E=21 MeV; measured γ(θ, t), recoil distance. 14C level deduced T1/2, g.
doi: 10.1103/PhysRevC.9.1748
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
1974MC17 Can.J.Phys. 52, 1381 (1974) A.B.McDonald, T.K.Alexander, O.Hausser, G.J.Costa, J.S.Forster, A.Olin Lifetimes of Low Lying Levels of 18O, 18Ne NUCLEAR REACTIONS 3H(16O, pγ), E=25 MeV; measured Eγ, Iγ, recoil distance. 16O(3He, nγ), E=7.5, 9 MeV; measured Eγ, Iγ, nγ-coin, DSA. 18O, 18Ne levels deduced T1/2.
doi: 10.1139/p74-184
1973AD02 Phys.Rev. C7, 889 (1973) E.G.Adelberger, A.B.McDonald, C.L.Cocke, C.N.Davids, A.P.Shukla, H.B.Mak, D.Ashery Isospin-Forbidden Particle Decay of T = 3/2 Levels in Mirror Nuclei NUCLEAR REACTIONS 11B(3He, np), E=7.0 MeV; measured σ(Ep, En, θ(n), θ(p)), αn-, pn-coin. 13N deduced level-width(γ), level-width(p), level-width(α). 11B(3He, np), E=7.5, 6.6 MeV; measured σ(En, Ep, θ(n), θ(p)), np-coin. 13C deduced level-width(γ), level-width(n). 15N(3He, np), E=8.25, 8.44 MeV; measured σ(En, Ep, θ(n), θ(p)), np-coin. 17F deduced level-width(p). 15N(3He, np), E=9.6 MeV; measured σ(En, Ep, θ(n), θ(p)), np-coin. 17O deduced level-width(n). 18O(3He, nα), E=12 MeV; measured σ(En, Eα, θ(α), θ(n))nα-coin. 17O deduced level-width(n).
doi: 10.1103/PhysRevC.7.889
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
1973HA32 Phys.Rev.Lett. 31, 323 (1973) O.Hausser, W.Witthuhn, T.K.Alexander, A.B.McDonald, J.C.D.Milton, A.Olin Short-Lived α Emitters of Thorium; New Isotopes 218-220Th NUCLEAR REACTIONS 204,206,207,208Pb(16O, 3nα), (16O, 4nα); measured Iα(t), Eα. 218,219,220Th deduced T1/2, Qα.
doi: 10.1103/PhysRevLett.31.323
1973HA47 Nucl.Phys. A212, 613 (1973) O.Hausser, A.B.McDonald, T.K.Alexander, A.J.Ferguson, R.E.Warner E1 Polarization in Coulomb Excitation of 7Li NUCLEAR REACTIONS 208Pb(7Li, 7Li'γ), E=18-30 MeV; measured σ(E;E(7Li)', Eγ, θ). 7Li levels deduced E1 interference effects, B(E2); enriched targets.
doi: 10.1016/0375-9474(73)90826-9
1973HA63 Nucl.Phys. A216, 617 (1973) O.Hausser, T.K.Alexander, D.L.Disdier, A.J.Ferguson, A.B.McDonald, I.S.Towner Alpha-Decay Widths in 20Ne NUCLEAR REACTIONS 16O(α, α), (α, α'), E approx 4.6 MeV, 14.1-17.1 MeV; measured σ(Eα, θ(α)). 20Ne deduced levels, J, π, α-widths. Natural targets.
doi: 10.1016/0375-9474(73)90174-7
1973OL05 Phys.Rev. D8, 1633 (1973) A.Olin, T.K.Alexander, O.Hausser, A.B.McDonald Measurement of the Relativistic Doppler Effect Using 8.6-MeV Capture γ Rays NUCLEAR REACTIONS 4He(16O, γ), E=27.65-27.75 MeV; measured DSA; deduced relativistic time-dilation effect.
doi: 10.1103/PhysRevD.8.1633
1972AL05 Nucl.Phys. A179, 477 (1972) T.K.Alexander, O.Hausser, A.B.McDonald, A.J.Ferguson, W.T.Diamond, A.E.Litherland A Measurement of the Radiative Width of the 8+ 11.948 MeV Level of 20Ne NUCLEAR REACTIONS 4He(16O, γ), E approx 36 MeV; measured omegaγ. 20Ne deduced E2 transition strength. He gas target.
doi: 10.1016/0375-9474(72)90384-3
1972AL28 Can.J.Phys. 50, 2198 (1972) T.K.Alexander, O.Hausser, A.B.McDonald, G.T.Ewan The Lifetimes of the 3/2+, 975 keV Level in 25Mg and the 3/2+, 945 keV Level in 25Al NUCLEAR REACTIONS 2H(24Mg, pγ), (24Mg, nγ), E=48 MeV; measured σ(Eγ, θ(γ)), recoil distance. 25Mg, 25Al levels deduced T1/2.
doi: 10.1139/p72-291
1972HA06 Phys.Lett. 38B, 75 (1972) O.Hausser, A.B.McDonald, T.K.Alexander, A.J.Ferguson, R.E.Warner Nuclear Polarizability of 7Li from Coulomb Excitation NUCLEAR REACTIONS 208Pb(7Li, 7Li), 208Pb(7Li, Xγ), E=18-30 MeV; measured σ(E;θ), σ(E;Eγ, θ). 7Li deduced nuclear polarizability.
doi: 10.1016/0370-2693(72)90743-5
1972HA07 Nucl.Phys. A179, 465 (1972) O.Hausser, A.J.Ferguson, A.B.McDonald, I.M.Szoghy, T.K.Alexander, D.L.Disdier High Spin States in 20Ne from 16O(α, α) Scattering NUCLEAR REACTIONS 16O(α, α), E=5-11 MeV; measured σ(Eα, θ(α)). 20Ne deduced levels, J, π, α-widths. Natural targets.
doi: 10.1016/0375-9474(72)90383-1
1971AL29 Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 2287 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 2076 (1972) T.K.Alexander, O.Hausser, A.B.McDonald, G.T.Ewan The Lifetime of the 3/2+ 975 keV Level in 25Mg NUCLEAR REACTIONS 2H(24Mg, γ), E=48 MeV; measured Doppler shift attenuation. 25Mg deduced T1/2 for 975-keV level. Plunger method.
1971HA26 Nucl.Phys. A168, 17 (1971) O.Hausser, T.K.Alexander, A.B.McDonald, G.T.Ewan, A.E.Litherland Gamma-Decay Properties of 20Ne Levels below 12 MeV NUCLEAR REACTIONS 12C(12C, αγ), E=20-30 MeV; measured σ(Eα, Eγ, θ(γ), θ(pγ)), Doppler shift attenuation, recoil distance. 20Ne deduced levels, T1/2, γ-branching, γ-mixing. Natural target.
doi: 10.1016/0375-9474(71)90649-X
1971HA47 Nucl.Phys. A175, 593 (1971) O.Hausser, T.K.Alexander, A.B.McDonald, W.T.Diamond Coulomb Reorientation of 2+ States in 32S and 112Cd NUCLEAR REACTIONS 112Cd(32S, 32S'γ), E=90, 100 MeV; measured σ(Eγ, θ(S)). 32S, 112Cd levels deduced B(E2), q2. Enriched target.
doi: 10.1016/0375-9474(71)90452-0
1971MC20 Can.J.Phys. 49, 2886 (1971) A.B.McDonald, T.K.Alexander, O.Hausser, G.T.Ewan Lifetimes of States in 29Si, 27Al, and 26Mg NUCLEAR REACTIONS 12C(19F, npγ), E=25 MeV; 12C(19F, αpγ), E=25 MeV; 27Al(35Cl, 35Cl'γ), E=67 MeV; measured recoil distance. 27Al(35Cl, 35Cl'γ), E=67 MeV; measured Doppler shift attenuation. 29Si, 27Al, 26Mg levels deduced T1/2.
doi: 10.1139/p71-346
1970AD01 Nucl.Phys. A143, 97 (1970) E.G.Adelberger, A.V.Nero, A.B.McDonald Low-Lying T = 2 States of 16O NUCLEAR REACTIONS 12C, 14C(3He, n), E=11.3-18.0 MeV; measured σ(E;En, θ). 14O, 16O deduced levels, T, level-width, J, π, L. Enriched target.
doi: 10.1016/0375-9474(70)90682-2
1970AD02 Nucl.Phys. A145, 497 (1970) A Study of the 16O(3He, n) and 12C(3He, n) Stripping Reactions and a Comparison of Analogous (3He, n), (3He, p) and (t, p) Transitions NUCLEAR REACTIONS 16O, 12C(3He, n), E=9.0-13.5 MeV; measured σ(E;En, θ). 18Ne, 14O deduced levels, J, π. Compared with (3He, p), (t, p) reactions. Natural targets.
doi: 10.1016/0375-9474(70)90438-0
1970MC02 Phys.Lett. 31B, 119 (1970) A.B.McDonald, E.G.Adelberger, H.B.Mak, D.Ashery, A.P.Shukla, C.L.Cocke, C.N.Davids Isospin-Nonconserving Particle Decays of the Lowest T = 3/2 Levels in 17F and 17O NUCLEAR REACTIONS 15N(3He, n), E=8.44 MeV; 18O(3He, α), E=12 MeV; measured σ(En, Ep), σ(Eα, En). 17F, 17O T=3/2 levels deduced level-width, branching ratios.
doi: 10.1016/0370-2693(70)90126-7
1970MC06 Nucl.Phys. A144, 593 (1970) A Study of 22Mg by the 20Ne(3He, n) Reaction NUCLEAR REACTIONS 20Ne(3He, n), E=3.4-9.4 MeV; measured σ(E;En, θ), Q. 22Mg deduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(70)90347-7
1969AD01 Phys.Rev.Letters 22, 352(1969) E.G.Adelberger, C.L.Cocke, C.N.Davids, A.B.McDonald Isospin-Nonconserving Decays in Mirror Nuclei NUCLEAR REACTIONS 11B(3He, pn), (3He, np), E=7 MeV; measured σ(En, Ep). 13C, 13N levels deduced n-, p-decay branching, form of isospin impurity.
doi: 10.1103/PhysRevLett.22.352
1969AD02 Nucl.Phys. A124, 49(1969) E.G.Adelberger, A.B.McDonald, C.A.Barnes A Study of Low-Lying T = 3/2 and T = 2 States in Some Light Nuclei (I) NUCLEAR REACTIONS 11B, 15N, 18O, 19F, 22Ne(3He, n), E=4.2-13.5 MeV; measured σ(En, θ). 13N, 17F, 20Ne, 21Na, 24Mg deduced levels, T, level-width, J, π, L. Enriched targets.
doi: 10.1016/0375-9474(69)90520-X
1969MC14 Nucl.Phys. A137, 545 (1969) A.B.McDonald, J.R.Patterson, H.Winkler T=3/2 States in 21Na as Seen in the 20Ne(p, p)20Ne Reaction NUCLEAR REACTIONS 20Ne(p, p), (p, p'), E = 6.76-7.33 MeV; measured σ(E;Ep', θ). 21Na deduced resonances, T, J, level-width. Natural gas target.
doi: 10.1016/0375-9474(69)90092-X
1968MC03 Phys.Letters 26B, 380 (1968) T = 3/2 Levels in 21Na NUCLEAR STRUCTURE 21Na, 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(68)90619-9
1967AD01 Phys.Letters 24B, 270 (1967); Erratum Phys.Letters 24B, 618 (1967) Lowest T = 2 States in 20Ne and 24Mg NUCLEAR STRUCTURE 24Mg, 20Ne, 18O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90444-3
1967AD05 Phys.Letters 25B, 595 (1967) E.G.Adelberger, A.B.McDonald, T.A.Tombrello, F.S.Dietrich, A.V.Nero A Lower Limit on the Mass of 5Be
doi: 10.1016/0370-2693(67)90125-6
1967MC15 Bull.Am.Phys.Soc. 12, No.8, 1145, FB14 (1967) Study of the 20Ne(3He, N)22Mg reaction NUCLEAR STRUCTURE 22Mg; measured not abstracted; deduced nuclear properties.
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