NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = S.P.Kwan Found 9 matches. 1987CA15 Nucl.Phys. A467, 205 (1987) J.R.Campbell, O.A.Abou-Zeid, W.R.Falk, R.Abegg, S.K.Datta, S.P.Kwan The 18O(p, α)15N Reaction at 40.9 MeV NUCLEAR REACTIONS 18O(p, α), E=40.9 MeV; measured σ(θ); deduced model parameters. 15N deduced levels, J-transfer, J, spectroscopic strengths, π. DWBA analysis, cluster from form factors. Shell model.
doi: 10.1016/0375-9474(87)90526-4
1987PA07 Phys.Rev. C35, 1119 (1987) S.A.Page, H.C.Evans, G.T.Ewan, S.-P.Kwan, J.R.Leslie, J.D.MacArthur, W.McLatchie, P.Skensved, S.-S.Wang, H.-B.Mak, A.B.McDonald, C.A.Barnes, T.K.Alexander, E.T.H.Clifford Weak Pion-Nucleon Coupling Strength: New constraint from parity mixing in 18F NUCLEAR REACTIONS 16O(3He, p), E=4.05 MeV; measured γ CP; deduced weak pion-nucleon coupling strength. 19F levels deduced parity mixing.
doi: 10.1103/PhysRevC.35.1119
1985EV03 Phys.Rev.Lett. 55, 791 (1985) H.C.Evans, G.T.Ewan, S.-P.Kwan, J.R.Leslie, J.D.MacArthur, H.-B.Mak, W.McLatchie, S.A.Page, P.Skensved, S.-S.Wang, A.B.McDonald, C.A.Barnes, T.K.Alexander, E.T.H.Clifford Parity Mixing of 0+ and 0- Levels in 18F NUCLEAR REACTIONS 16O(3He, p), E=4.05 MeV; measured Eγ, Iγ, γ CP; deduced weak pion-nucleon coupling constant. 18F transition deduced parity nonconserving matrix element.
doi: 10.1103/PhysRevLett.55.791
1985KW01 Phys.Rev. C31, 271 (1985) S.P.Kwan, S.T.Lam, G.C.Neilson, H.S.Sherif Isospin Dependence in the Central Real Part of the Optical Model Potential NUCLEAR STRUCTURE A=12-208; analyzed nucleon elastic scattering data; deduced potential isospin dependent term behavior. Empirical optical models.
doi: 10.1103/PhysRevC.31.271
1985LA13 Phys.Rev. C32, 76 (1985) S.T.Lam, W.K.Dawson, S.A.Elbakr, H.W.Fielding, P.W.Green, R.L.Helmer, I.J.van Heerden, A.H.Hussein, S.P.Kwan, G.C.Neilson, T.Otsubo, D.M.Sheppard, H.S.Sherif, J.Soukup Elastic Scattering of Polarized Neutrons on 16O, 59Co, and Pb at 23 MeV NUCLEAR REACTIONS 16O, 59Co, Pb(polarized n, n), E=23 MeV; measured σ(θ), A(θ). Optical model potential analysis.
doi: 10.1103/PhysRevC.32.76
1985MA32 Phys.Rev. C32, 314 (1985) J.D.MacArthur, S.-P.Kwan, H.-B.Mak, W.McLatchie, S.A.Page, S.-S.Wang, T.K.Alexander Experimental Evidence Against the Proposed Band Based on a Shape Isomer in 32S NUCLEAR REACTIONS 28Si(α, γ), E=1.76-3.82 MeV; σ(Eγ, E), γ yield, γ(θ). 32S level deduced J, π, B(λ).
doi: 10.1103/PhysRevC.32.314
1982AB03 Nucl.Phys. A382, 185 (1982) O.A.Abou-zeid, W.R.Falk, S.K.Datta, S.P.Kwan, J.Campbell The 46,48,50Ti(p, α)43,45,47Sc Reactions at 40.35 MeV NUCLEAR REACTIONS 46,48,50Ti(p, α), E=40.35 MeV; measured σ(θ). 43,45,47Sc deduced levels, j-transfer, π. DWBA analysis, microscopic form factors.
doi: 10.1016/0375-9474(82)90131-2
1980DA07 Phys.Rev. C21, 1687 (1980) S.K.Datta, W.R.Falk, S.P.Kwan, R.Abegg, O.A.Abou-Zeid 12C(p, α*)9B Reaction in the Finite Range Microscopic Distorted-Wave Born-Approximation Formalism NUCLEAR REACTIONS 12C(p, α), (p, pt), E=45.2 MeV; measured σ(Ep, Et, θ), σ(Eα, θ). Finite range DWBA, microscopic, cluster form factors, final-state interactions.
doi: 10.1103/PhysRevC.21.1687
1979VO08 Nucl.Phys. A332, 157 (1979) F.K.Vosniakos, N.E.Davison, W.R.Falk, O.Abou-Zeid, S.P.Kwan Exchange Terms in the Optical Model NUCLEAR REACTIONS 16O, 40Ca, 66,68Zn, 208Pb(p, p), E=20-50 MeV; analyzed σ(θ), P(θ). Optical model.
doi: 10.1016/0375-9474(79)90101-5
Back to query form |