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NSR database version of April 11, 2024.

Search: Author = Z.M.Koenig

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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
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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
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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
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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
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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
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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
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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
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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
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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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