NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = W.K.Wells Found 10 matches. 1986CH41 Phys.Rev. C34, 2358 (1986) T.Chapuran, D.P.Balamuth, W.K.Wells, C.M.Laymon, D.P.Bybell Angular Momenta of Intermediate Width Structures in 12C + 16O NUCLEAR REACTIONS 12C(16O, 16O), (16O, 16O'), E(cm)=14.9-27.6 MeV; measured σ(E, θ), yield vs E. 28Si deduced intermediate structure, possible J, π. Legendre polynomial analysis.
doi: 10.1103/PhysRevC.34.2358
1985BA60 Phys.Rev.Lett. 55, 2842 (1985) D.P.Balamuth, T.Chapuran, C.M.Laymon, W.K.Wells, D.P.Bybell Characterization of Gross-Structure Resonances in Angular-Momentum-Mismatched Channels in Heavy-Ion Collisions NUCLEAR REACTIONS 16O(16O, 16O'), E(cm)=17-41 MeV; measured σ(θ), mutual, single excitations. 32S deduced resonances, L, J.
doi: 10.1103/PhysRevLett.55.2842
1985BY01 Phys.Rev. C32, 452 (1985) D.P.Bybell, W.K.Wells, D.P.Balamuth Mechanism of Spin-Dependent Inelastic Scattering in the 13C + 12C System NUCLEAR REACTIONS 12C(13C, 13C), E(cm)=17.28, 26.88 MeV; measured (particle)γ(θ), (particle)γ-coin; deduced spin-flip probability. 12C level deduced density matrix.
doi: 10.1103/PhysRevC.32.452
1984BA31 Phys.Lett. 140B, 295 (1984) D.P.Balamuth, W.K.Wells, T.Chapuran, D.P.Bybell, C.M.Laymon Failure of the Molecular Core-Particle Coupling Model in 13C + 13C Inelastic Scattering NUCLEAR REACTIONS 13C(13C, 13C'), E(cm)=8-25 MeV; measured σ(θ); deduced intermediate states role, molecular particle-core coupling model inadequacy. Single, mutual inelastic excitation.
doi: 10.1016/0370-2693(84)90756-1
1984WE10 Nucl.Instrum.Methods 219, 284 (1984) C.R.Westerfeldt, E.G.Bilpuch, M.E.Bleck, D.A.Outlaw, W.K.Wells, J.F.Wilkerson, T.B.Clegg A System for Producing High-Resolution Polarized and Unpolarized Beams with a Tandem Accelerator NUCLEAR REACTIONS 54Fe(p, p), E=4.341-4.345 MeV; measured σ(θ) vs E. 55Co deduced resonance, J, π, Γp. R-matrix analysis. 32S(p, p), E=3.374-3.376 MeV; measured T=3/2 resonance yield; deduced optimum resolution conditions. Polarized, unpolarized beams, foil, gas strippers.
doi: 10.1016/0167-5087(84)90334-X
1982DA10 Phys.Rev. C25, 1388 (1982) K.Daneshvar, W.K.Wells, D.P.Bybell, L.Mulligan, D.P.Balamuth 24Mg(12C, α)32S Reaction from E(12C) = 24-36 MeV NUCLEAR REACTIONS 24Mg(12C, α), E=24-36 MeV; measured σ(Eα), σ(θ) vs E.
doi: 10.1103/PhysRevC.25.1388
1982WE03 Nucl.Instrum.Methods 192, 273 (1982) C.R.Westerfeldt, S.A.Wender, E.G.Bilpuch, G.E.Mitchell, W.K.Wells Measurement of Nuclear E0 Transitions NUCLEAR REACTIONS 72Ge(p, p'e), E=3-4.34 MeV; measured p'e-coin, I(ce)(t), σ(E). 72Ge level deduced T1/2. 73As deduced IAR. Pulsed beam, large solid angle electron detector.
doi: 10.1016/0029-554X(82)90832-1
1982WE07 Phys.Rev. C25, 2512 (1982) W.K.Wells, D.P.Bybell, D.P.Balamuth Mutual Inelastic Scattering in the 16O + 16O System NUCLEAR REACTIONS, ICPND 16O(16O, 16O'), E(cm)=24-41 MeV; measured γγ-coin; deduced σ(E) for single, mutual excitation, reaction mechanism.
doi: 10.1103/PhysRevC.25.2512
1980WE09 Z.Phys. A297, 215 (1980) W.K.Wells, E.G.Bilpuch, G.E.Mitchell Non-Statistical Effects for Inelastic Proton Amplitudes in 49V NUCLEAR REACTIONS 48Ti(p, p'γ), E=1.9-3.09 MeV; measured γ(θ), relative sign of inelastic amplitudes; deduced nonstatistical effects. 49V resonances deduced reduced width channel correlation, Γp, Γp'.
doi: 10.1007/BF01892801
1979WE09 Phys.Lett. 86B, 18 (1979) W.K.Wells, E.G.Bilpuch, G.E.Mitchell Observation of Intermediate Structure in Inelastic Proton Amplitudes in 49V NUCLEAR REACTIONS 48Ti(p, p'), E=1.90-3.09 MeV; measured σ(E). 49V resonances deduced magnitude, relative signs localized nonstatistical behavior of inelastic channel amplitudes.
doi: 10.1016/0370-2693(79)90610-5
Back to query form |