NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = Z.M.Koenig Found 9 matches. 2008AH02 Phys.Rev. C 77, 054302 (2008) I.Ahmad, F.G.Kondev, Z.M.Koenig, Wm.C.McHarris, S.W.Yates Two-quasiparticle states in 250Bk studied by decay scheme and transfer reaction spectroscopy NUCLEAR REACTIONS 249Bk(d, p), E=12.0 MeV; measured proton spectra, σ(θ). 250Bk; deduced levels, J, π. RADIOACTIVITY 254Es(α); measured Eα, Iα, Eγ, Iγ, ce, ICC, γα-coin. 250Bk; deduced levels, J, π, hindrance factors, γ-multipolarities, band configurations.
doi: 10.1103/PhysRevC.77.054302
1994WA37 Nucl.Instrum.Methods Phys.Res. A353, 678 (1994) T.F.Wang, J.B.Carlson, Z.M.Koenig, W.D.Ruhter, T.S.H.Lee, J.Winn Monte Carlo Simulation of Plutonium Gamma-Ray Standards RADIOACTIVITY 241Am, 235U(α); 237U(β-); 238,239,240Pu(α); 241Pu(α), (β-); analyzed Eγ, Iγ data. Monte Carlo simulation of photon transport.
doi: 10.1016/0168-9002(94)91749-3
1990GO08 Phys.Rev. C41, 2635 (1990) P.L.Gonthier, P.Harper, B.Bouma, R.Ramaker, D.A.Cebra, Z.M.Koenig, D.Fox, G.D.Westfall Breakup of the Projectile at 35 MeV/Nucleon NUCLEAR REACTIONS 58Ni(16O, αX), E=560 MeV; measured σ(Eα, fragment energy), α(fragment)-coin for X=C, B, Be; deduced projectile breakup mechanism.
doi: 10.1103/PhysRevC.41.2635
1987GO17 Phys.Rev. C35, 1946 (1987) P.L.Gonthier, B.Bouma, P.Harper, R.Ramaker, D.A.Cebra, Z.M.Koenig, D.Fox, G.D.Westfall Alpha Emission at the Fermi Energy NUCLEAR REACTIONS 58Ni(16O, αX), E=35 MeV/nucleon; measured σ(Eα, θα, fragment θ), α-particle velocity distribution; deduced reaction mechanism, nonequilibrium components. Enriched target, ΔE-E telescopes. Model calculations.
doi: 10.1103/PhysRevC.35.1946
1986FO04 Phys.Rev. C33, 1540 (1986) D.Fox, D.A.Cebra, Z.M.Koenig, P.Ugorowski, G.D.Westfall Large Angle Correlations in 40 MeV/nucleon 12C + C NUCLEAR REACTIONS 12C(12C, 2p), (12C, 2d), (12C, 2t), (12C, 23He), (12C, 2α), E=40 MeV/nucleon; measured (particle)(particle)(θ), (particle)(particle)(φ); deduced correlation functions. Momentum conservation model.
doi: 10.1103/PhysRevC.33.1540
1985HA19 Phys.Rev. C32, 145 (1985) B.E.Hasselquist, G.M.Crawley, B.V.Jacak, Z.M.Koenig, G.D.Westfall, J.E.Yurkon, R.S.Tickle, J.P.Dufour, T.J.M.Symons Light-Particle-Complex-Fragment Coincidence Cross Sections from Intermediate Energy Nucleus-Nucleus Collisions NUCLEAR REACTIONS 197Au, 27Al(12C, dX), (12C, tX), E=30 MeV/nucleon; measured inclusive σ(θp, Ep), σ(θd, Ed), σ(θt, Et). 197Au(40Ar, pX), (40Ar, dX), (40Ar, tX), (40Ar, 3HeX), (40Ar, αX), E=92 MeV/nucleon; measured inclusive σ(θp, Ep), σ(θd, Ed), σ(θt, Et), σ(θ(3He), E(3He)), σ(θα, Eα). Moving source model.
doi: 10.1103/PhysRevC.32.145
1985ST20 Phys.Lett. 161B, 60 (1985) G.S.F.Stephans, D.G.Kovar, R.V.F.Janssens, G.Rosner, H.Ikezoe, B.Wilkins, D.Henderson, K.T.Lesko, J.J.Kolata, C.K.Gelbke, B.V.Jacak, Z.M.Koenig, G.D.Westfall, A.Szanto De Toledo, E.M.Szanto, P.L.Gonthier Influence of Nucleon Fermi Motion on Incomplete Fusion NUCLEAR REACTIONS 24Mg, 27Al, 28Si, 40Ca, 48Ti(14N, X), E=5-35 MeV/nucleon; measured evaporation residue velocity spectra; deduced Fermi motion role in inelastic fusion. Other data input.
doi: 10.1016/0370-2693(85)90609-4
1985WE14 Nucl.Instrum.Methods 238, 347 (1985) G.D.Westfall, J.E.Yurkon, J.Van Der Plicht, Z.M.Koenig, B.V.Jacak, R.Fox, G.M.Crawley, M.R.Maier, B.E.Hasselquist, R.S.Tickle, D.Horn A Logarithmic Detection System Suitable for a 4π Array NUCLEAR REACTIONS 197Au(14N, X), E=35 MeV/nucleon; 58Ni(35Cl, X), E=230 MeV; 12C(12C, X), E=30 MeV/nucleon; measured fragment, charge spectra.
doi: 10.1016/0168-9002(85)90472-3
1984WE03 Phys.Rev. C29, 861 (1984) G.D.Westfall, Z.M.Koenig, B.V.Jacak, L.H.Harwood, G.M.Crawley, M.W.Curtin, C.K.Gelbke, B.Hasselquist, W.G.Lynch, A.D.Panagiotou, D.K.Scott, H.Stocker, M.B.Tsang Light Particle Spectra from 35 MeV/Nucleon 12C-Induced Reactions on 197Au NUCLEAR REACTIONS 197Au(12C, pX), (12C, dX), (12C, tX), (12C, 3HeX), (12C, αX), (12C, 6HeX), E=35 MeV/nucleon; measured inclusive σ(Ep, θ), σ(Ed, θ), σ(Et, θ), σ(E(3He), θ), σ(Eα, θ), σ(E(6He, θ)); deduced moving source parameters, composite particle to proton yield ratio. Quantum statistical, hydrodynamic, thermal models.
doi: 10.1103/PhysRevC.29.861
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