NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.King Found 102 matches. Showing 1 to 100. [Next]2022MO03 Nucl.Instrum.Methods Phys.Res. A1021, 165864 (2022) M.Monterial, K.T.Schmitt, C.Prokop, E.Leal-Cidoncha, M.Anastasiou, N.S.Bowden, J.Bundgaard, R.J.Casperson, D.A.Cebra, T.Classen, D.H.Dongwi, N.Fotiades, J.Gearhart, V.Geppert-Kleinrath, U.Greife, C.Hagmann, M.Heffner, D.Hensle, D.Higgins, L.D.Isenhower, K.Kazkaz, A.Kemnitz, J.King, J.L.Klay, J.Latta, W.Loveland, J.A.Magee, B.Manning, M.P.Mendenhall, S.Mosby, D.Neudecker, S.Sangiorgio, B.Seilhan, L.Snyder, F.Tovesson, R.S.Towell, N.Walsh, T.S.Watson, L.Yao, W.Younes Measurement of material isotopics and atom number ratio with α-particle spectroscopy for a NIFFTE fission Time Projection Chamber actinide target NUCLEAR REACTIONS 235U, 239Pu(n, F), E not given; measured fission products, Eα, Iα; deduced isotopic concentrations and atomic number ratio.
doi: 10.1016/j.nima.2021.165864
2018LO19 Eur.Phys.J. A 54, 140 (2018) W.Loveland, A.M.Vinodkumar, R.Yanez, L.Yao, J.King, J.Lassen, A.Rojas Sub-barrier fusion of 11Li with 208Pb NUCLEAR REACTIONS 208Pb(11Li, x), E=26.1-32.7[sub-barrier]; measured reaction products isotopes; deduced complete, incomplete, total fusion σ, added published σ of the same group at different energies; calculated nuclidic σ using HIVAP statistical model code.
doi: 10.1140/epja/i2018-12572-8
2018WA06 Phys.Rev. C 97, 021602 (2018) A.Wakhle, K.Hammerton, Z.Kohley, D.J.Morrissey, K.Stiefel, J.Yurkon, J.Walshe, K.J.Cook, M.Dasgupta, D.J.Hinde, D.J.Jeung, E.Prasad, D.C.Rafferty, C.Simenel, E.C.Simpson, K.Vo-Phuoc, J.King, W.Loveland, R.Yanez Capture cross sections for the synthesis of new heavy nuclei using radioactive beams NUCLEAR REACTIONS 181Ta(39K, X), E=180-210 MeV; 181Ta(46K, X), E=190-215 MeV; measured time of flight and relative position of fission fragments, capture-fission σ(E) from a binary event using 14UD Heavy-ion accelerator facility of Australian National University (ANU), and Coupled Cyclotron Facility (CCF) projectile fragmentation facility at NSCL-MSU, and the Coincident Fission Fragment Detector (CFFD) at the ReA3 facility at NSCL; deduced velocity vectors of the coincident fragments, masses and angular distributions of fission fragments. Comparison with several phenomenological models and microscopic time-dependent Hartree-Fock calculations. Discussed implications for the synthesis of heavy nuclei at radioactive beam facilities. 197Au(31Al, X), E(cm), 248Cm(26Mg, X), E(cm)=110-160 MeV; 248Cm(48Ca, X), E(cm)=195-230 MeV; 154Sm(31Al, X), E(cm)=125-190 MeV; 238U(48Ca, X), E(cm)=185-235 MeV; 238U(64Ni, X), E(cm)=260-300 MeV; compiled theoretical and experimental values of capture fission σ(E). Comparison with several theoretical results.
doi: 10.1103/PhysRevC.97.021602
2018YA05 Nucl.Phys. A970, 65 (2018) R.Yanez, J.King, J.S.Barrett, W.Loveland, N.Fotiades, H.Y.Lee Total kinetic energy release in the fast neutron induced fission of 235U NUCLEAR REACTIONS 235U(n, F), E=2-100 MeV; measured En, In, fission products; deduced (post neutron emission) TKE. Fusion σ calculated within semi-empirical GEF model.
doi: 10.1016/j.nuclphysa.2017.11.007
2017KI14 Eur.Phys.J. A 53, 238 (2017) J.King, R.Yanez, W.Loveland, J.S.Barrett, B.Oscar, N.Fotiades, F.Tovesson, H.Y.Lee The total kinetic energy release in the fast neutron-induced fission of 232Th NUCLEAR REACTIONS 232Th(n, F), E=3-91 MeV; measured post-emission TKE release; calculated compound nucleus E* vs En, neutron multiplicity; deduced fragment mass distribution, average excitation energy of the fissioning system vs En, neutron multiplicity. Compared to 232Th(p, F) published data.
doi: 10.1140/epja/i2017-12436-9
2014YA10 Phys.Rev. C 89, 051604 (2014) R.Yanez, L.Yao, J.King, W.Loveland, F.Tovesson, N.Fotiades Excitation energy dependence of the total kinetic energy release in 235U(n, f) NUCLEAR REACTIONS 235U(n, F), E=3.2-50 MeV; measured (fission fragment)(fission fragment)-coin, time-of-flight, total kinetic energy (ETKE) release as function of incident neutron energy at WNR-LANSCE-LANL facility; deduced dependence of ETKE and total excitation energy (ETXE) on E(n). Comparison with GEF model predictions, and with previous experimental results.
doi: 10.1103/PhysRevC.89.051604
2009SC13 Astrophys.J. 701, 837 (2009) S.C.Schuler, J.R.King, L.-S.The Stellar Nucleosynthesis in the Hyades Open Cluster
doi: 10.1088/0004-637X/701/1/837
2005CH30 Nucl.Phys. A752, 510c (2005) A.A.Chen, R.E.Azuma, S.Bishop, L.Buchmann, M.L.Chatterjee, J.M.D'Auria, S.Engel, D.Gigliotti, U.Greife, D.Hunter, A.Hussein, D.Hutcheon, C.C.Jewett, J.Jose, J.D.King, A.M.Laird, M.Lamey, R.Lewis, W.Liu, A.Olin, D.Ottewell, P.Parker, J.Rogers, C.Ruiz, M.Trinczek, C.Wrede The 21Na(p, γ)22Mg reaction in novae and x-ray bursts NUCLEAR REACTIONS 1H(21Na, γ), E(cm) ≈ 200-1100 keV; measured thick-target yield. 21Na(p, γ), E=low; deduced resonance parameters, astrophysical reaction rate.
doi: 10.1016/j.nuclphysa.2005.02.136
2005KI16 Nucl.Phys. A758, 300c (2005) J.R.King, A.M.Boesgaard, C.P.Deliyannis Abundances in Near-Turnoff Stars in the Globular Cluster M 71
doi: 10.1016/j.nuclphysa.2005.05.053
2005SC16 Nucl.Phys. A758, 332c (2005) S.C.Schuler, J.R.King, L.M.Hobbs, M.H.Pinsonneault λ7774 Oxygen Triplet in Open Cluster Dwarfs: Pleiades and M34
doi: 10.1016/j.nuclphysa.2005.05.060
2004DA17 Phys.Rev. C 69, 065803 (2004) J.M.D'Auria, R.E.Azuma, S.Bishop, L.Buchmann, M.L.Chatterjee, A.A.Chen, S.Engel, D.Gigliotti, U.Greife, D.Hunter, A.Hussein, D.Hutcheon, C.C.Jewett, J.Jose, J.D.King, A.M.Laird, M.Lamey, R.Lewis, W.Liu, A.Olin, D.Ottewell, P.Parker, J.Rogers, C.Ruiz, M.Trinczek, C.Wrede The 21Na(p, γ)22Mg reaction from Ec.m. = 200 to 1103 keV in novae and x-ray bursts NUCLEAR REACTIONS 1H(21Na, γ), E(cm)=200-1103 keV; measured Eγ, Iγ, (particle)γ-coin; deduced resonance energies and strengths. 21Na(p, γ), E=low; deduced astrophysical reaction rates.
doi: 10.1103/PhysRevC.69.065803
2003AZ05 Nucl.Phys. A718, 119c (2003) R.E.Azuma, S.Bishop, L.Buchmann, M.L.Chatterjee, A.A.Chen, J.M.D'Auria, T.Davinson, S.Engel, B.R.Fulton, D.Gigliotti, U.Greife, D.Groombridge, D.Hunter, A.Hussein, D.Hutcheon, C.Jewett, J.D.King, N.Khan, S.Kubono, A.M.Laird, M.Lamey, R.Lewis, L.Ling, W.Liu, S.Michimasa, A.S.Murphy, A.Olin, D.Ottewell, P.Parker, J.Pearson, I.Roberts, A.Robinson, J.G.Rogers, G.Roy, C.Ruiz, F.Sarazin, A.C.Shotter, H.Sprenger, F.Strieder, P.Walden, P.J.Woods, C.Wrede Results of 21Na + p Experiments at ISAC NUCLEAR REACTIONS 1H(21Na, 21Na), E=0.45-1.4 MeV; measured recoil proton spectra; deduced excitation function. 1H(21Na, γ), E=220, 855 keV/nucleon; measured Eγ, (particle)γ-coin. 22Mg deduced resonance features.
doi: 10.1016/S0375-9474(03)00688-2
2003BI03 Phys.Rev.Lett. 90, 162501 (2003); Erratum Phys.Rev.Lett. 90, 229902 (2003) S.Bishop, R.E.Azuma, L.Buchmann, A.A.Chen, M.L.Chatterjee, J.M.D'Auria, S.Engel, D.Gigliotti, U.Greife, M.Hernanz, D.Hunter, A.Hussein, D.Hutcheon, C.Jewett, J.Jose, J.King, S.Kubono, A.M.Laird, M.Lamey, R.Lewis, W.Liu, S.Michimasa, A.Olin, D.Ottewell, P.D.Parker, J.G.Rogers, F.Strieder, C.Wrede 21Na(p, γ)22Mg Reaction and Oxygen-Neon Novae NUCLEAR REACTIONS 1H(21Na, γ), E(cm) ≈ 202-223 keV; measured Eγ, (particle)γ-coin, thick-target yields; deduced resonance energy, width. 21Na(p, γ), E=low; deduced astrophysical reaction rate.
doi: 10.1103/PhysRevLett.90.162501
2003BI08 Nucl.Phys. A718, 263c (2003) S.Bishop, R.Azuma, L.Buchmann, A.A.Chen, M.L.Chatterjee, J.M.D'Auria, S.Engel, D.Gigliotti, U.Greife, D.Hunter, A.Hussein, D.Hutcheon, C.Jewett, J.King, S.Kubono, M.Lamey, R.Lewis, W.Liu, S.Michimasa, A.Olin, D.Ottewell, P.D.Parker, J.Rogers, C.Wrede Nuclear Astrophysics Studies at DRAGON: The 21Na(p, γ)22Mg Reaction and Oxygen-Neon Novae NUCLEAR REACTIONS 1H(21Na, γ), E(cm) ≈ 202-224 keV; measured thick target yields. 21Na(p, γ), E=low; deduced astrophysical reaction rate. Recoil mass separator.
doi: 10.1016/S0375-9474(03)00726-7
2003OL08 Nucl.Phys. A721, 1019c (2003) A.Olin, S.Bishop, L.Buchmann, M.L.Chatterjee, A.Chen, J.M.D'Auria, S.Engel, D.Gigliotti, U.Greife, D.Hunter, A.Hussein, D.Hutcheon, C.Jewett, J.King, S.Kubono, M.Lamey, A.M.Laird, R.Lewis, W.Liu, S.Michimasa, D.Ottewell, P.Parker, J.Rogers, F.Strieder, C.Wrede Nuclear Astrophysics at ISAC with DRAGON: Initial Studies NUCLEAR REACTIONS 1H(21Na, γ), E(cm) ≈ 212, 822 keV/nucleon; measured resonance excitation functions.
doi: 10.1016/S0375-9474(03)01275-2
2002AN06 Phys.Rev. C65, 034310 (2002) D.Anthony, L.Buchmann, P.Bergbusch, J.M.D'Auria, M.Dombsky, U.Giesen, K.P.Jackson, J.D.King, J.Powell, F.C.Barker β-Delayed Deuteron Emission from 6He RADIOACTIVITY 6He(β-) [from C(p, X)]; measured Eβ, β-delayed deuteron spectra, dα-coin, T1/2; deduced branching ratio. Comparison with model predictions.
doi: 10.1103/PhysRevC.65.034310
2002CH61 Phys.Rev. C 66, 064316 (2002) J.C.Chow, J.D.King, N.P.T.Bateman, R.N.Boyd, L.Buchmann, J.M.D'Auria, T.Davinson, M.Dombsky, E.Gete, U.Giesen, C.Iliadis, K.P.Jackson, A.C.Morton, J.Powell, A.Shotter β-delayed particle decay of 17Ne into p+α+12C through the isobaric analog state in 17F RADIOACTIVITY 17Ne(β+α), (β+p); measured Ep, Eα pα(12C)-coin following decay of intermediate IAS state; deduced branching ratios. 17F deduced branching ratios for particle decay from IAS.
doi: 10.1103/PhysRevC.66.064316
2002MO19 Nucl.Phys. A706, 15 (2002) A.C.Morton, J.C.Chow, J.D.King, R.N.Boyd, N.P.T.Bateman, L.Buchmann, J.M.D'Auria, T.Davinson, M.Dombsky, W.Galster, E.Gete, U.Giesen, C.Iliadis, K.P.Jackson, J.Powell, G.Roy, A.Shotter Beta-Delayed Particle Decay of 17Ne RADIOACTIVITY 17Ne(β+p), (β+α); measured Ep, Eα, pγ-coin, angular correlations; deduced log ft, Gamow-Teller strength. 17F deduced levels, J, π, particle decay branching ratios.
doi: 10.1016/S0375-9474(02)00862-X
2001BU05 Phys.Rev. C63, 034303 (2001) L.Buchmann, E.Gete, J.C.Chow, J.D.King, D.F.Measday β-Delayed Particle Decay of 9C and the A = 9, T = 1/2 Nuclear System: R-matrix fits, the A = 9 nuclear system, and the stellar reaction rate of 4He(αn, γ)9Be RADIOACTIVITY 9C(β+); analyzed β-spectra, β-delayed particle spectra, coincidences. 9B deduced levels, J, π, Gamow-Teller strengths. Multichannel, multistate R-matrix approach, astrophysical implications discussed. Shell model calculations.
doi: 10.1103/PhysRevC.63.034303
2000GE09 Phys.Rev. C61, 064310 (2000) E.Gete, L.Buchmann, R.E.Azuma, D.Anthony, N.Bateman, J.C.Chow, J.M.D'Auria, M.Dombsky, U.Giesen, C.Iliadis, K.P.Jackson, J.D.King, D.F.Measday, A.C.Morton β-Delayed Particle Decay of 9C and the A = 9, T = 1/2 Nuclear System: Experiment, data, and phenomenological analysis RADIOACTIVITY 9C(β+); measured Eβ, Iβ, β-delayed particle spectra, coincidences, angular correlations. 9B levels deduced excitation and decay branching ratios.
doi: 10.1103/PhysRevC.61.064310
1998CH05 Phys.Rev. C57, R475 (1998) J.C.Chow, A.C.Morton, R.E.Azuma, N.Bateman, R.N.Boyd, L.Buchmann, J.M.D'Auria, T.Davinson, M.Dombsky, W.Galster, E.Gete, U.Giesen, C.Iliadis, K.P.Jackson, J.D.King, G.Roy, T.Shoppa, A.Shotter Three-Particle Breakup of the Isobaric Analog State in 17F RADIOACTIVITY 17Ne(β+) [from Mg, O(p, X)]; measured β-delayed pα(12C)-coin. 17F deduced IAS p, α branching ratios. Implications for stellar helium burning discussed.
doi: 10.1103/PhysRevC.57.R475
1997IL03 Nucl.Phys. A621, 211c (1997) C.Iliadis, R.E.Azuma, J.Chow, J.D.King, A.C.Morton, L.Buchmann, M.Dombsky, K.P.Jackson, J.M.D'Auria, U.Giesen, J.G.Ross, H.Schatz, M.Wiescher Decay Studies of Importance to Explosive Hydrogen Burning RADIOACTIVITY 36K(β+p), (β+α) [from Ca(p, X), E=500 MeV]; measured α-, proton spectra; deduced log ft. 36Ar deduced α-emitting resonance.
doi: 10.1016/S0375-9474(97)00240-6
1997KI18 Nucl.Phys. A621, 19c (1997) J.R.King, C.P.Deliyannis, A.M.Boesgaard Constraints on the Origin of the Remarkable Lithium Abundance of the Halo Star BD+23 3912
doi: 10.1016/S0375-9474(97)00204-2
1997KI19 Nucl.Phys. A621, 169c (1997) J.D.King, R.E.Azuma, C.Iliadis, A.C.Morton, L.Buchmann, M.Dombsky, K.P.Jackson, J.M.D'Auria, U.Giesen, G.Roy, T.Davinson, A.Shotter, W.Galster, R.N.Boyd Investigation of the 12C(α, γ)16O Reaction Via the β-Delayed Proton Decay of 17Ne RADIOACTIVITY 17Ne(β+p); measured β-delayed proton spectra, pγ-coin. 16O levels deduced β-delayed proton branching ratios. Implications for 12C(α, γ) reaction.
doi: 10.1016/S0375-9474(97)00232-7
1996IL02 Nucl.Phys. A609, 237 (1996) C.Iliadis, R.E.Azuma, L.Buchmann, J.Chow, J.M.D'Auria, M.Dombsky, U.Giesen, J.D.King, A.C.Morton Beta-Delayed Particle Decay of 36K RADIOACTIVITY 36K(β+); measured decay products, β-delayed Ep, Ip, Eα, Iα. 36Ar; deduced levels, particle branching ratios, associated log ft upper limits. Microchannel plate in back-to-back geometry, surface barrier detector.
doi: 10.1016/0375-9474(96)00297-7
1994AZ03 Phys.Rev. C50, 1194 (1994); Erratum Phys.Rev. C56, 1655 (1997) R.E.Azuma, L.Buchmann, F.C.Barker, C.A.Barnes, J.M.D'Auria, M.Dombsky, U.Giesen, K.P.Jackson, J.D.King, R.G.Korteling, P.McNeely, J.Powell, G.Roy, J.Vincent, T.R.Wang, S.S.M.Wong, P.R.Wrean Constraints on the Low-Energy E1 Cross Section of 12C(α, γ)16O from the β-Delayed α Spectrum of 16N RADIOACTIVITY 16N(β-) [from on-line separation]; measured β-delayed α-spectrum, (α)(12C)-coin; deduced R-matrix, K-matrix level parameters relevant to 12C(α, γ) reaction. Thin Si surface barrier detector. NUCLEAR REACTIONS, ICPND 12C(α, γ), E(cm) ≤ 3 MeV; calculated E1 part of astrophysical S-factor, σ(E); deduced R-matrix, K-matrix level parameters. Data of β--delayed α-spectrum of 16N-decay input.
doi: 10.1103/PhysRevC.50.1194
1994DO08 Phys.Rev. C49, 1867 (1994) M.Dombsky, L.Buchmann, J.M.D'Auria, U.Giesen, K.P.Jackson, J.D.King, E.Korkmaz, R.G.Korteling, P.McNeely, J.Powell, G.Roy, M.Trinczek, J.Vincent β-Delayed α Decay of 17N RADIOACTIVITY 17N(β-); measured β-delayed Eα, Iα, α(13C)-coin; deduced log ft, total βα-branching ratio. 17O deduced levels contributing to α-decay.
doi: 10.1103/PhysRevC.49.1867
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
1994GI01 Nucl.Phys. A567, 146 (1994) U.Giesen, C.P.Browne, J.Gorres, J.G.Ross, M.Wiescher, R.E.Azuma, J.D.King, J.B.Vise, M.Buckby The Influence of Low-Energy Resonances on the Reaction Rate of 18O(α, γ)22Ne NUCLEAR REACTIONS, ICPND 18O(6Li, 6Li), (6Li, d), E=32 MeV; measured σ(θ); deduced model parameters. 18O(α, γ), E < 1 MeV; measured γ(θ). 18O(p, γ), E ≈ resonance; measured thick target yield curve. 22Ne deduced resonances, J, π, spectroscopic factors, role in 18O(α, γ) reaction rate.
doi: 10.1016/0375-9474(94)90731-5
1994KI02 Nucl.Phys. A567, 354 (1994) J.D.King, R.E.Azuma, J.B.Vise, J.Gorres, C.Rolfs, H.P.Trautvetter, A.E.Vlieks Cross Section and Astrophysical S-Factor for the 13C(p, γ)14N Reaction NUCLEAR REACTIONS, ICPND 13C(p, γ), E=120-950 keV; measured γ-ray yield 14N. 13C(p, γ), E=120-950 keV; calculated astrophysical S-factor, thermonuclear reaction rate. 14N deduced resonance parameters, branching ratios, direct capture contributions, spectroscopic factors for proton-bound states.
doi: 10.1016/0375-9474(94)90154-6
1993BU03 Phys.Rev.Lett. 70, 726 (1993) L.Buchmann, R.E.Azuma, C.A.Barnes, J.M.D'Auria, M.Dombsky, U.Giesen, K.P.Jackson, J.D.King, R.G.Korteling, P.McNeely, J.Powell, G.Roy, J.Vincent, T.R.Wang, S.S.M.Wong, P.R.Wrean β-Delayed α Spectrum of 16N and the 12C(α, γ)16O Cross Section at Low Energies RADIOACTIVITY 16N(β-); measured β-delayed Eα, Iα, α(12C)-coin; deduced E1 part of 12C(α, γ) reaction, astrophysical S-factor.
doi: 10.1103/PhysRevLett.70.726
1993BU18 J.Phys.(London) G19, S115 (1993) L.Buchmann, R.E.Azuma, C.A.Barnes, A.Chen, J.Chen, J.M.D'Auria, M.Dombsky, U.Giesen, K.P.Jackson, J.D.King, R.Korteling, P.McNeely, J.Powell, G.Roy, M.Trinczek, J.Vincent, P.R.Wrean, S.S.M.Wong The β-Delayed α Spectrum of 16N and the Low-Energy Extrapolation of the 12C(α, γ)16O Cross Section RADIOACTIVITY 16N(β-); measured β-delayed Eα, Iα, βα-coin; deduced 12C(α, γ) reaction σ(E=low) implications.
doi: 10.1088/0954-3899/19/S/010
1993BU21 Nucl.Instrum.Methods Phys.Res. B79, 330 (1993) L.Buchmann, R.E.Azuma, C.A.Barnes, J.M.D'Auria, M.Dombsky, U.Giesen, K.P.Jackson, J.D.King, R.Korteling, P.McNeely, J.Powell, G.Roy, J.Vincent, S.S.M.Wong, P.R.Wrean A Study of Beta Delayed Alpha Emission from 16N RADIOACTIVITY 16N(β-); measured β-delayed α(12C)-coin. 18,17N(β-); measured β-delayed Eα, Iα; deduced 12C(α, γ) reaction p-wave capture amplitude.
doi: 10.1016/0168-583X(93)95357-B
1993GI04 Nucl.Phys. A561, 95 (1993) U.Giesen, C.P.Browne, J.Gorres, S.Graff, C.Iliadis, H.-P.Trautvetter, M.Wiescher, V.Harms, K.L.Kratz, B.Pfeiffer, R.E.Azuma, M.Buckby, J.D.King The Astrophysical Implications of Low-Energy Resonances in 22Ne + α NUCLEAR REACTIONS 22Ne(6Li, d), E=32 MeV; measured σ(θ), σ(Ed). 22Ne(α, n), E=0.6-9 MeV; measured neutron yield vs E; deduced model parameters, resonance yield, reaction rates. 26Mg deduced resonances, J, π, α-spectroscopic factors, resonance strength.
doi: 10.1016/0375-9474(93)90167-V
1991IL01 Nucl.Phys. A533, 153 (1991) C.Iliadis, U.Giesen, J.Gorres, S.Graff, M.Wiescher, R.E.Azuma, J.King, M.Buckby, C.A.Barnes, T.R.Wang The Reaction Branching 31P(p, γ)/31P(p, α) in the rp-Process NUCLEAR REACTIONS, ICPND 31P(p, γ), E=0.28-0.62 MeV; 31P(p, α), E=0.28-0.45 MeV; measured σ(E), relative yield. 32S, 28Si deduced resonances, J, π, resonance strengths. Hauser-Feshbach calculations.
doi: 10.1016/0375-9474(91)90824-P
1991KI06 Can.J.Phys. 69, 828 (1991) Branching Ratios for the Decay of the 8.78 and 8.91 MeV States of 14N NUCLEAR REACTIONS 13C(p, γ), E=1.25-1.465 MeV; measured γ-spectra. 14N levels deduced transitions branching ratios.
doi: 10.1139/p91-135
1991KI08 Phys.Rev. C44, 1077 (1991) J.D.King, D.Frekers, R.Abegg, R.E.Azuma, L.Buchmann, C.Chan, T.E.Drake, R.Helmer, K.P.Jackson, L.Lee, C.A.Miller, E.Rost, R.Sawafta, R.Schubank, S.S.M.Wong, S.Yen, X.Q.Zhu Excitation of the 10.957 MeV 0-; T = 0 State in 16O by 400 MeV Protons NUCLEAR REACTIONS 16O(polarized p, p'), E=400 MeV; measured σ(θ), analyzing power vs θ; deduced reaction mechanism.
doi: 10.1103/PhysRevC.44.1077
1990FR07 Phys.Lett. 244B, 178 (1990) D.Frekers, H.J.Wortche, A.Richter, R.Abegg, R.E.Azuma, A.Celler, C.Chan, T.E.Drake, R.Helmer, K.P.Jackson, J.D.King, C.A.Miller, R.Schubank, M.C.Vetterli, S.Yen Spin Excitations in the Deformed Nuclei 154Sm, 158Gd and 168Er NUCLEAR REACTIONS 154,158Gd, 168Er(p, p'), E=200 MeV; measured σ(θ), σ(Ep'). 154Sm deduced B(M1) strength function. 158Gd, 168Er deduced B(λ).
doi: 10.1016/0370-2693(90)90051-7
1990GR04 Nucl.Phys. A510, 346 (1990) S.Graff, J.Gorres, M.Wiescher, R.E.Azuma, J.King, J.Vise, G.Hardie T.R.Wang Proton Capture on 28Si and Its Astrophysical Implications NUCLEAR REACTIONS, ICPND 28Si(p, γ), E=0.37-2.95 MeV; measured σ(E); deduced astrophysical S-factor, total reaction rate. 29P deduced resonances, resonance strengths, Γ, spectroscopic factors.
doi: 10.1016/0375-9474(90)90244-G
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
1989FR03 Phys.Lett. 218B, 439 (1989) D.Frekers, D.Bohle, A.Richter, R.Abegg, R.E.Azuma, A.Celler, C.Chan, T.E.Drake, K.P.Jackson, J.D.King, C.A.Miller, R.Schubank, J.Watson, S.Yen Spin Response of Magnetic Dipole Transitions in 156Gd and 164Dy NUCLEAR REACTIONS 164Dy, 156Gd(p, p'), E=200 MeV; measured σ(θ), σ(Ep). 164Dy deduced magnetic dipole transition spin response, B(M1). 156Gd deduced magnetic dipole transition spin response.
doi: 10.1016/0370-2693(89)91443-3
1989LE04 Nucl.Phys. A492, 607 (1989) L.Lee, T.E.Drake, S.S.M.Wong, D.Frekers, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Abegg, R.Helmer, K.P.Jackson, C.A.Miller, S.Yen Intermediate-Energy Proton Scattering to the Ground and Negative-Parity States of 40Ca, 90Zr and 208Pb NUCLEAR REACTIONS 40Ca(polarized p, p'), E=362 MeV; 90Zr(polarized p, p'), E=400 MeV; 208Pb(polarized p, p'), E=200, 400 MeV; measured σ(θ), A(y)(θ). Natural 40Ca, enriched 90Zr, 208Pb targets. Nonrelativistic microscopic density-dependent model analysis.
doi: 10.1016/0375-9474(89)90111-5
1989LE06 J.Phys.(London) G15, L91 (1989) L.Lee, T.E.Drake, S.S.M.Wong, D.Frekers, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Abegg, R.Helmer, K.P.Jackson, C.A.Miller, S.Yen Inelastic Proton Scattering to the Positive-Parity States in 90Zr at 400 MeV NUCLEAR REACTIONS 90Zr(polarized p, p'), E=400 MeV; measured σ(θ), A(θ). Enriched target. Nonrelativistic microscopic density-dependent model analysis.
doi: 10.1088/0954-3899/15/5/006
1988LE10 Phys.Lett. 205B, 219 (1988) L.Lee, T.E.Drake, S.S.M.Wong, D.Frekers, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Abegg, R.Helmer, K.P.Jackson, C.A.Miller, S.Yen, H.V.von Geramb Intermediate Energy Proton Scattering from 40Ca, 90Zr and 208Pb NUCLEAR REACTIONS 40Ca, 90Zr, 208Pb(polarized p, p), E=200, 362, 400 MeV; measured σ(θ), analyzing power vs θ, spin rotation parameter vs θ.
doi: 10.1016/0370-2693(88)91653-X
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
1987BU12 Nucl.Instrum.Methods Phys.Res. B26, 151 (1987) L.Buchmann, J.M.D'Auria, J.D.King, G.Mackenzie, H.Schneider, R.B.Moore, C.Rolfs An ISOL/Post-Accelerator Facility for Nuclear Astrophysics at TRIUMF NUCLEAR REACTIONS 13N(p, γ), E(cm)=260-700 keV; compiled thin target yields; 19Ne(p, γ), E ≈ 0.694-1.565 MeV; compiled thick target yields.
doi: 10.1016/0168-583X(87)90744-0
1987FR05 Phys.Rev. C35, 2236 (1987) D.Frekers, S.S.M.Wong, R.E.Azuma, T.E.Drake, J.D.King, R.Abegg, K.P.Jackson, C.A.Miller, S.Yen, W.P.Alford, R.L.Helmer, C.Broude, S.Mattsson, E.Rost Elastic and Inelastic Scattering of 362 MeV polarized Protons from 40Ca NUCLEAR REACTIONS 40Ca(polarized p, p), (polarized p, p'), E=362 MeV; measured σ(θ), analyzing power. Magnetic spectrometer. Model calculations.
doi: 10.1103/PhysRevC.35.2236
1987MA31 Nucl.Phys. A470, 206 (1987) P.V.Magnus, M.S.Smith, P.D.Parker, R.E.Azuma, C.Campbell, J.D.King, J.Vise Measurement of the 15N(α, γ)19F Resonances at E(cm)=536 keV and 542 keV NUCLEAR REACTIONS 15N(α, γ), E(cm)=536, 542 keV; measured Eγ, Iγ. 19F resonances deduced γ transition strength.
doi: 10.1016/0375-9474(87)90128-X
1987SC10 Nucl.Phys. A467, 240 (1987) U.Schroder, H.W.Becker, G.Bogaert, J.Gorres, C.Rolfs, H.P.Trautvetter, R.E.Azuma, C.Campbell, J.D.King, J.Vise Stellar Reaction Rate of 14N(p, γ)15O and Hydrogen Burning in Massive Stars NUCLEAR REACTIONS, ICPND 14N(p, γ), E=0.2-3.6 MeV; measured σ(E, E(γ), θ(γ)); deduced astrophysical S-factor, capture σ . 15O deduced levels, J, π, Γ, spectroscopic factors. Windowless gas, implanted 14N targets. Ge(Li) detectors.
doi: 10.1016/0375-9474(87)90528-8
1987SC18 Phys.Lett. 192B, 55 (1987) U.Schroder, A.Redder, C.Rolfs, R.E.Azuma, L.Buchmann, C.Campbell, J.D.King, T.R.Donoghue Astrophysical S Factor of 3H(α, γ)7Li NUCLEAR REACTIONS, ICPND 3H(α, γ), E(cm)=79-464 keV; measured Eγ, Iγ, branching ratio, σ(E), γ yield; deduced astrophysical S-factor vs E. Ge(Li) detectors.
doi: 10.1016/0370-2693(87)91141-5
1987TI05 Aust.J.Phys. 40, 319 (1987) C.I.W.Tingwell, J.D.King, D.G.Sargood Angular Distributions for 6Li(p, γ)7Be NUCLEAR REACTIONS 6Li(p, γ), E=0.5-0.8, 1 MeV; measured γ yield vs θ; deduced reaction mechanism. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0053. 1986MI06 Phys.Lett. 169B, 166 (1986) C.A.Miller, A.Scott, R.Abegg, R.Helmer, K.P.Jackson, M.Whiten, S.Yen, L.Lee, T.E.Drake, D.Frekers, S.S.M.Wong, R.E.Azuma, L.Buchmann, A.Galindo-Uribarri, J.D.King, R.Schubank, R.Dymarz, H.V.von Geramb, C.J.Horowitz Large Angle Elastic Scattering of 200 MeV Protons from 208Pb NUCLEAR REACTIONS 208Pb(polarized p, p), (polarized p, p'), E=200 MeV; measured σ(θ), analyzing power vs θ; deduced exchange medium effects role. Microscopic Schrodinger, relativistic impulse approximation analyses.
doi: 10.1016/0370-2693(86)90643-X
1985ZH07 Nucl.Phys. A439, 619 (1985) X.Zhu, R.E.Azuma, T.E.Drake, J.D.King, S.S.M.Wong Wolfenstein Parameters in the Helicity Representation for Intermediate-Energy Proton-Nucleus Scattering NUCLEAR REACTIONS 12C(polarized p, p), E=200 MeV; measured polarization, analyzing power, Wolfenstein parameters vs θ. Distorted wave approximation, momentum helicity representation.
doi: 10.1016/0375-9474(85)90330-6
1984BU04 Can.J.Phys. 62, 134 (1984) Cross Sections and Thermonuclear Reaction Rates for the 28Si(α, p)31P and 54Fe(α, p)57Co Reactions NUCLEAR REACTIONS, ICPND 28Si(α, p), E(cm)=4.5-10 MeV; 54Fe(α, p), E(cm)=6-12 MeV; measured absolute σ(E); deduced stellar reaction rates. 31P, 57Co deduced ground state reaction rates. Statistical model.
doi: 10.1139/p84-023
1984WO12 Phys.Lett. 149B, 299 (1984) S.S.M.Wong, R.E.Azuma, T.E.Drake, J.D.King, X.Zhu Wolfenstein Parameters for 0+ → 0- Transitions Excited by Proton Scattering at Intermediate Energies NUCLEAR REACTIONS 16O(polarized p, p'), E=135 MeV; calculated σ(θ), analyzing power vs θ. 16O(polarized p, p'), E=200 MeV; calculated Wolfenstein parameters; deduced exchange term role. DWIA analysis.
doi: 10.1016/0370-2693(84)90410-6
1983BU01 J.Phys.(London) G9, 85 (1983) Cross Sections for the 39K(α, p)42Ca and 42Ca(α, p)45Sc Reactions NUCLEAR REACTIONS, ICPND 39K(α, p), E=4.31-9.53 MeV; 42Ca(α, p), E=4.57-8.9 MeV; measured absolute σ(E). Enriched targets, Si detectors. Statistical model.
doi: 10.1088/0305-4616/9/1/013
1983WI09 Phys.Rev. C28, 1431 (1983) M.Wiescher, R.N.Boyd, S.L.Blatt, L.J.Rybarcyk, J.A.Spizuoco, R.E.Azuma, E.T.H.Clifford, J.D.King, J.Gorres, C.Rolfs, A.Vlieks 11C Level Structure via the 10B(p, γ) Reaction NUCLEAR REACTIONS, ICPND 10B(p, γ), E=0.07-2.2 MeV; measured Eγ, Iγ, γ yield, capture σ vs E, γ(θ); deduced direct capture contributions. 11C deduced resonances, J, π, Γ, γ-branching ratios, Γγ/Γ.
doi: 10.1103/PhysRevC.28.1431
1980CH12 Can.J.Phys. 58, 697 (1980) Cross Sections and Thermonuclear Reaction Rates for the 24Mg(α, n)27Si, 25Mg(p, n)25Al, 27Al(p, n)27Si, and 28Si(α, n)31S Reactions NUCLEAR REACTIONS 24Mg(α, n), E(cm)=7.27-10.27 MeV; 28Si(α, n), E(cm)=8.3-10.93 MeV; 25Mg(p, n), E=5.28-8.89 MeV; 27Al(p, n), E=5.77-9.63 MeV; measured annihilation γγ-coin; deduced σ(E), reaction rates. Statistical model analysis. Enriched Mg targets.
doi: 10.1139/p80-095
1980CH33 Can.J.Phys. 58, 1677 (1980) Cross Section and Thermonuclear Reaction Rates for the 58Ni(p, γ)59Cu Reaction NUCLEAR REACTIONS 58Ni(p, γ), E(cm)=0.98-5 MeV; measured σ(E); dedued thermonuclear reaction rates. Thin, thick, enriched targets, annihilation γβ+-coin technique, NaI(Tl) detector.
doi: 10.1139/p80-222
1980PR09 Nucl.Phys. A345, 278 (1980) G.Proudfoot, H.S.Bradlow, P.S.Fisher, N.S.Godwin, J.King, D.Sinclair, W.D.M.Rae Sequential Calculations for Heavy-Ion Induced Two-Nucleon Transfer on 14N, 15N and 16O NUCLEAR REACTIONS 14N(13C, X), E=105 MeV; 14N(11B, 9Be), E=115 MeV; measured σ(θ). 15,16,17,18O, 19F deduced S. DWBA analysis, sequential transfer. Gas target.
doi: 10.1016/0375-9474(80)90425-X
1979CH23 J.Phys.(London) G5, 1261 (1979); see 79Ch29 Cross Sections for the 42Ca(p, γ)43Sc, 42Ca(α, n)45Ti and 44Ca(p, n)44Sc Reactions
doi: 10.1088/0305-4616/5/9/010
1979CH29 J.Phys.(London) G5, 1261 (1979) Cross Sections for the 42Ca(p, γ)43Sc, 42Ca(α, n)45Ti and 44Ca(p, n)44Sc Reactions NUCLEAR REACTIONS 42Ca(p, γ), E=0.66-5.39 MeV; 42Ca(α, n), E=5.41-10.95 MeV; 44Ca(p, n), E=4.49-7.57 MeV; measured σ(E). Enriched targets. NaI(Tl) detectors. Statistical model interpretation.
doi: 10.1088/0305-4616/5/9/010
1979KI02 Can.J.Phys. 57, 286 (1979) Cross Sections for the 26Mg(p, n)26gAl (7.3 X 105 yr) and 26Mg(p, n)26mAl (6.35 s) Reactions NUCLEAR REACTIONS 26Mg(p, n), E=4.8-7.0 MeV; measured nothing; calculated production σ. Statistical compound nuclear model. 26Al, 26mAl deduced ratio of production σ.
doi: 10.1139/p79-036
1979RA10 Nucl.Phys. A319, 239 (1979) W.D.M.Rae, N.S.Godwin, D.Sinclair, H.S.Bradlow, P.S.Fisher, J.D.King, A.A.Pilt, G.Proudfoot Few-Nucleon Transfer Reactions on 15N and 16O NUCLEAR REACTIONS 16O, 15N(13C, 10B), (13C, 11C), 16O(13C, 13C), (13C, 12C), (13C, 12B), E=105 MeV; 16O, 15N(11B, 8Li), (11B, 9Li), (11B, 9Be), (12C, 7Li), (12C, 8Li), (12C, 9Be), 15N(11B, 10Be), 16O(11B, 7Li), (11B, 10B), (11B, 10C), (11B, 11B), (11B, 11C), (11B, 12C), (12C, 12C), E=115 MeV; 16O(18O, 16O), E=126 MeV; measured σ(θ). 16,17O, 17F levels deduced S, parity. 18O deduced parity. Optical model, DWBA analysis. Weak coupling, shell, cluster models. Enriched gas targets.
doi: 10.1016/0375-9474(79)90184-2
1978VL02 Nucl.Phys. A309, 506 (1978) A.E.Vlieks, C.W.Cheng, J.D.King Cross Section and Stellar Reaction Rates for the 42Ca(p, γ) Reaction NUCLEAR REACTIONS 42Ca(p, γ), E=0.7-5.5 MeV; measured σ(E); deduced reaction rates for stellar nucleosynthesis.
doi: 10.1016/0375-9474(78)90492-X
1975SC08 Nucl.Phys. A243, 202 (1975) R.L.Schulte, J.D.King, H.W.Taylor States in 53Mn from the 52Cr(p, γ)53Mn Reaction NUCLEAR REACTIONS 52Cr(p, γ), E=0.9-1.03 MeV; measured σ(E, Eγ, θ), DSA. 53Mn deduced levels, J, T1/2, branching ratios. Enriched target.
doi: 10.1016/0375-9474(75)90244-4
1974SC02 Can.J.Phys. 52, 131 (1974) R.L.Schulte, J.D.King, H.W.Taylor Levels in 45Sc from Radiative Proton Capture in 44Ca NUCLEAR REACTIONS 44Ca(p, γ), E=600-930 keV; measured σ(E;Eγ, θ). 45Sc deduced levels, J, π, γ-mixing.
doi: 10.1139/p74-020
1974SC07 Phys.Rev. C9, 1436 (1974) R.L.Schulte, J.D.King, H.W.Taylor Lifetime Measurements in 45Sc NUCLEAR REACTIONS 44Ca(p, γ), E=860 keV; measured DSA. 45Sc levels deduced T1/2, J.
doi: 10.1103/PhysRevC.9.1436
1973IN02 Nucl.Phys. A203, 164 (1973) H.Ing, J.D.King, R.L.Schulte, H.W.Taylor Levels in 44Ca Excited by the β-Decay of 44K RADIOACTIVITY 44K[from 44Ca(n, p)]; measured T1/2, Eγ, Iγ, γγ-coin; deduced log ft. 44Ca deduced levels, J, π, γ-branching. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(73)90430-2
1972TA02 Nucl.Phys. A179, 417 (1972) H.W.Taylor, B.Singh, F.S.Prato, J.D.King The Decay of 129Ba RADIOACTIVITY 129Ba[from 130Ba(γ, n)]; measured T1/2, Eγ, Iγ, γ-γcoin. 129Cs deduced levels, ICC, γ-multipolarity, J, π. Natural targets;Ge(Li), NaI(Tl) detectors.
doi: 10.1016/0375-9474(72)90381-8
1971TA19 Can.J.Phys. 49, 2614 (1971) Low-Energy Gamma-Ray Spectrum of 184m,184Re RADIOACTIVITY 184Re, 184mRe; measured Eγ, Iγ. 184W deduced levels, J, π.
doi: 10.1139/p71-313
1970KU05 Nucl.Phys. A143, 545 (1970) A.H.Kukoc, B.Singh, J.D.King, H.W.Taylor The Decay of 184gRe and 184mRe RADIOACTIVITY 184Re[from 185Re(γ, n)]; measured Eγ, Iγ, γγ-coin. 184W deduced levels. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(70)90548-8
1970WA22 Nucl.Phys. A154, 467 (1970) R.E.Wahrer, J.D.King, A.H.Kukoc, P.J.Pan, H.W.Taylor A Study of the States of 116In Excited Through Radiative Resonance Neutron Capture in 115In NUCLEAR REACTIONS 115In(n, γ), E=1.457, 3.86 eV resonances; measured Eγ, Iγ; deduced Q. 116In deduced levels. Natural target. Ge(Li) detector.
doi: 10.1016/0375-9474(70)90119-3
1969IN02 Can.J.Phys. 47, 1133 (1969) H.Ing, J.J.Gameson, J.D.King, H.W.Taylor Radiative Capture of Neutrons by the 5.2 eV Resonance in 109Ag NUCLEAR REACTIONS 109Ag(n, γ), E = 5.2 eV; measured Eγ, Iγ; deduced Q. 110Ag deduced levels. Ge(Li) detector, time-of-flight method.
doi: 10.1139/p69-141
1969IN03 Nucl.Phys. A137, 561 (1969) H.Ing, A.Kukoc, J.D.King, H.W.Taylor Radiative Capture of Neutrons by the 6.24, 15.5 and 29.7 eV Resonances in 121Sb and the 21.6 eV Resonance in 123Sb NUCLEAR REACTIONS Sb(n, γ), E = 2-105 eV; measured Eγ, Iγ; deduced Q. 122,124Sb resonances deduced J, π. 122,124Sb deduced levels, J, π.
doi: 10.1016/0375-9474(69)90093-1
1969SI03 Nucl.Phys. A129, 104 (1969) B.Singh, R.J.Cox, A.H.Kukoc, J.D.King, H.W.Taylor A Study of the Gamma Rays Emitted by 97Nb RADIOACTIVITY 97Nb [from 98Mo(γ, p), beta decay] measured Eγ, Iγ. 97Mo deduced levels. Enriched target, Ge(Li) detector.
doi: 10.1016/0375-9474(69)90911-7
1969TA03 Nucl.Phys. A125, 358(1969) H.W.Taylor, J.D.King, H.Ing, R.J.Cox Decay of 22 min 44K RADIOACTIVITY 44K[from 44Ca(n, p)]; measured Eγ, Iγ. 44Ca deduced levels.
doi: 10.1016/0375-9474(69)91079-3
1969TA07 Can.J.Phys. 47, 1539 (1969) H.W.Taylor, J.D.King, H.Ing, R.J.Cox Note on the Decay of 43K RADIOACTIVITY 43K; measured T1/2; Eγ, Iγ, deduced log ft. 43Ca deduced levels. Ge(Li) detector.
doi: 10.1139/p69-196
1969TA12 Can.J.Phys. 47, 2873 (1969) H.W.Taylor, B.Singh, A.H.Kukoc, J.D.King Measurement of the Directional Correlation of the 1038-605 keV Gamma Cascade in 134Ba RADIOACTIVITY 134Cs; measured γγ(θ), γγ-coin. 134Ba levels deduced J, γ-mixing. Ge(Li), NaI detectors.
doi: 10.1139/p69-350
1968IN04 Bull. Am. Phys. Soc, 13, No. 11, 1390, BG9 (1968) H.Ing, J.Gameson, H.W.Taylor, J.D.King Gamma Rays Following Resonance Neutron Capture in 109Ag NUCLEAR STRUCTURE 110Ag; measured not abstracted; deduced nuclear properties.
1968KI03 Can.J.Phys. 46, 2119 (1968) J.D.King, B.Lalovic, H.W.Taylor Evidence Against Proposed High-Spin Levels at 3660 and 2824 keV in 44Ca NUCLEAR STRUCTURE 44Sc; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p68-559
1968KU09 Nucl.Phys. A115, 625 (1968) A.H.Kukoc, J.D.King, H.W.Taylor A Study of the Decay of 17.9 d 74As RADIOACTIVITY 74As [from 75As(γ, n)]; measured Eγ, Iγ, γγ-coin. 74Ge, 74Se deduced levels, J, π, log ft.
doi: 10.1016/0375-9474(68)90753-7
1968TA01 Nucl.Phys. A106, 49 (1968) The Decay of 8 d 106mAg RADIOACTIVITY 106Ag[from 107Ag(γ, n)]; measured Eγ, Iγ. Natural taradioactivity 106Ag[from 107Ag(γ, n)]; measured Eγ, Iγ. 106Pd deduced levels. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(67)90827-5
1967KI05 Nucl.Phys. A99, 433(1967) The Decay of 139Pr RADIOACTIVITY 139Pr[from 141Pr(γ, 2n)]; measured Eγ. 139Ce deduced levels, J, π. Natural target.
doi: 10.1016/0375-9474(67)90941-4
1967KI07 Can.J.Phys. 45, 2446 (1967) A Note on the Decay of Scandium-44m NUCLEAR STRUCTURE 44Sc; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p67-197
1967KI10 Nucl.Instr.Methods 52, 349 (1967) The Energy of the 40K Gamma Ray and its Use as a Calibration Standard NUCLEAR STRUCTURE 40K, 228Ac, 212Bi; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-554X(67)90246-7
1967TA03 Phys.Letters 24B, 659 (1967) A New Determination of the Deuteron Binding Energy NUCLEAR STRUCTURE 1H, 2H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90372-3
1966BR03 Phys.Rev. 142, 53 (1966) Hyperfine Structure and Octopole Interaction in Stable Bromine Isotopes NUCLEAR STRUCTURE 81Br, 79Br; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.142.53
1963KN04 Phys.Rev. 131, 331 (1963) G.F.Knoll, J.S.King, W.C.Parkinson O16(d, n)F17 and Ca40(d, n)Sc41 Reactions by Time of Flight NUCLEAR STRUCTURE 16O, 41Sc; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.131.331
1962KN02 Bull.Am.Phys.Soc. 7, No.4, 302, JB11 (1962) G.Knoll, J.S.King, W.C.Parkinson Levels in Sc41 from the Ca40(d, n) Reaction NUCLEAR STRUCTURE 41Sc; measured not abstracted; deduced nuclear properties.
1960KI02 Can.J.Phys. 38, 231 (1960) J.D.King, R.N.H.Haslam, R.W.Parsons The Gamma-Neutron Cross Section for N14 NUCLEAR STRUCTURE 14N, 13N; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p60-023
1960KI06 Can.J.Phys. 38, 1069 (1960) J.D.King, R.N.H.Haslam, W.J.McDonald The Gamma-Neutron Cross Section for F19 NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1139/p60-115
1960KI07 Nuclear Phys. 19, 94 (1960) The Mg24(γ, n)Mg23 Reaction NUCLEAR STRUCTURE 24Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90222-4
1956HO02 NP-6012, p.35 (1956) J.H.Holloway, B.B.Aubrey, J.G.King Hyperfine Structure and Nuclear Magnetic Octopole Moments of the Stable Chlorine Isotopes
1954JA07 Phys.Rev. 94, 1798 (1954) V.Jaccarino, J.G.King, R.A.Satten, H.H.Stroke Hyperfine Structure of I127. Nuclear Magnetic Octupole Moment
doi: 10.1103/PhysRev.94.1798
1954KI11 Phys.Rev. 94, 1610 (1954) Hyperfine Structure and Nuclear Moments of the Stable Bromine Isotopes
doi: 10.1103/PhysRev.94.1610
1953KI14 Phys.Rev. 91, 476A (1953) J.G.King, H.H.Stroke, V.Jaccarino The Hyperfine Structure of Iodine
doi: 10.1103/PhysRev.91.476A
1953KI75 Phys.Rev. 89, 1080 (1953) Angular Distribution of Protons from Vanadium 52 NUCLEAR REACTIONS 51V(d, p), E(cm)=7.05 MeV; measured reaction products; deduced σ(θ).
doi: 10.1103/PhysRev.89.1080
1952KI33 Phys.Rev. 88, 141 (1952) A Further Test of the Shell Model NUCLEAR REACTIONS 35Cl(d, p), E(cm)=6.90 MeV; measured reaction products; deduced σ(θ), J. Comparison with theoretical calculations.
doi: 10.1103/PhysRev.88.141
1952PA03 Phys.Rev. 87, 387 (1952) W.C.Parkinson, E.H.Beach, J.S.King An Experimental Test of the Shell Model NUCLEAR REACTIONS 31P(d, p), E(cm)=7.2 MeV; measured reaction products; deduced σ(θ), J. Comparison with theoretical calculations.
doi: 10.1103/PhysRev.87.387.2
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