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NSR database version of May 1, 2024.

Search: Author = F.C.Wang

Found 4 matches.

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1989WA12      J.Phys.(London) G15, 829 (1989)

F.-C.Wang, J.-M.Hu

A Study of the Multimode Fission Model

NUCLEAR REACTIONS, ICPND 237Np, 245Cm, 235U, 257Fm(n, F), E=thermal; 233,235,238U, 232Th, 239,240,241,242Pu(n, F), E=fast; 230Th, 233U(α, F), E=25.7 MeV; 226Ra(p, F), E=13 MeV; calculated fission fragment yield vs mass. Multi-mode fission model.

RADIOACTIVITY 258Fm, 252Cf(SF); analyzed fission fragment yield vs mass; deduced minimum potential positions. Multi-mode fission model.

NUCLEAR STRUCTURE 258Fm, 252Cf, 227Ac; calculated potential contours. Multi-mode fission model.

doi: 10.1088/0954-3899/15/6/013
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1980PE07      Nucl.Phys. A341, 440 (1980)

J.C.Peng, H.S.Song, F.C.Wang, J.V.Maher

A Coupled-Channels Born-Approximation Analysis of Rare-Earth (d, t) Transitions

NUCLEAR REACTIONS 160Gd, 162,164Dy, 166Er(d, t), E=17 MeV; 168Er(d, t), E=17, 15, 13, 11 MeV; analyzed σ(θ). CCBA.

doi: 10.1016/0375-9474(80)90376-0
Citations: PlumX Metrics


1978PE05      Phys.Rev.Lett. 41, 225 (1978)

J.C.Peng, H.S.Song, F.C.Wang, J.V.Maher

Inadequacy of the Coupled-Channels Born Approximation for Explaining Anomalous Rare-Earth (d, t) Transitions

NUCLEAR REACTIONS 164Dy, 160Gd, 168Er(d, t), E ≤ 17 MeV; calculated σ(θ), anomalies.

doi: 10.1103/PhysRevLett.41.225
Citations: PlumX Metrics


1978PE15      Phys.Lett. 80B, 35 (1978)

J.C.Peng, J.V.Maher, M.S.Chiou, W.J.Jordan, F.C.Wang, M.W.Wu

Structure in 28Si(16O, 12C)32S Excitation Functions

NUCLEAR REACTIONS 28Si(16O, 12C), E(cm)=22.3-32.5 MeV; measured excitation function, σ(θ).

doi: 10.1016/0370-2693(78)90299-X
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