NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = P.Nagel Found 10 matches. 1995NA35 Nucl.Sci.Eng. 119, 97 (1995) P.Nagel, J.Rodens, M.Blann, H.Gruppelaar Intermediate Energy Nuclear Reaction Code Intercomparison: Applications to Transmutation of Long-Lived Reactor Wastes NUCLEAR REACTIONS 208Pb, 90Zr(p, xn), E=25-800 MeV; 90Zr(p, xp), E=80, 160 MeV; analyzed σ(θ, θ(nucleon)). Zr, Pb(p, xn), (p, xp), E < 1 GeV; analyzed nucleon multiplicities. Intercomparison of codes.
doi: 10.13182/NSE95-A24074
1986HO28 Radiat.Eff. 95, 27 (1986) P.E.Hodgson, G.M.Field, H.Gruppelaar, P.Nagel Pre-Equilibrium Processes in Nuclear Reactions NUCLEAR REACTIONS 93Nb(n, xn), E=10, 14.6, 20, 25.7 MeV; calculated angle integrated σ(En). 59Co(n, xn), (n, xp), E=14 MeV; 65Cu(p, xn), E=26.7 MeV; calculated σ(θ), σ(θn, En), σ(θp, Ep). Semi-classical models, quantum mechanical theory.
doi: 10.1080/00337578608208667
1981MA02 Nucl.Phys. A351, 509 (1981) J.F.Mateja, D.P.Stanley, L.V.Theisen, A.D.Frawley, P.L.Pepmiller, L.R.Medsker, P.B.Nagel A Woods-Saxon and Double-Folding Optical-Model Description of 14N Elastic and Inelastic Scattering from 24Mg, 27Al and 28Si NUCLEAR REACTIONS 27Al(14N, 14N), E=52.3 MeV; 24Mg, 28Si(14N, 14N), (14N, 14N'), E=53, 53.4 MeV; measured σ(θ); deduced Woods-Saxon and double-folding optical model parameters. 24Mg, 28Si deduced deformation lengths.
doi: 10.1016/0375-9474(81)90185-8
1980GO08 Nucl.Phys. A341, 494 (1980) Effects of Local Density Dependence on the Scattering of Heavy Ions and Alpha Particles NUCLEAR REACTIONS 40Ca(α, α), E=29 MeV; 58Ni(α, α), E=50.2 MeV; 60Ni(16O, 16O), E=61.4 MeV; 28Si(16O, 16O), E=53 MeV; 40Ca, 208Pb(16O, 16O), 208Pb(α, α), E not given; calculated σ(θ); deduced local density dependence. Double-folding calculations.
doi: 10.1016/0375-9474(80)90380-2
1979MA21 Phys.Rev. C20, 176 (1979) J.F.Mateja, A.D.Frawley, P.B.Nagel, L.A.Parks 12C(9Be, 9Be)12C (g.s., 4.43 MeV) Reaction NUCLEAR REACTIONS 12C(9Be, 9Be), E=40-45 MeV; measured σ(E, θ); deduced reaction mechanism. Enriched target. Hauser-Feshbach, coupled-channel, exchange analysis.
doi: 10.1103/PhysRevC.20.176
1978NA15 Phys.Rev. C18, 2617 (1978) Exact-Finite-Range Coupled-Channels Born Approximation Analysis of the Reaction 12C(14N, 13N)13C at 100 MeV NUCLEAR REACTIONS 12C(14N, 13N), E=100 MeV; calculated σ(θ). DWBA, CCBA, finite range.
doi: 10.1103/PhysRevC.18.2617
1977PA25 Phys.Lett. 70B, 27 (1977) L.A.Parks, K.W.Kemper, A.H.Lumpkin, R.I.Cutler, L.H.Harwood, D.Stanley, P.Nagel, F.Petrovich Quadrupole Effects in the Elastic Scattering of 10B, 11B, and 12C by 27Al NUCLEAR REACTIONS 27Al(10B, 10B), (11B, 11B), E=50 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1016/0370-2693(77)90336-7
1976NA05 Phys.Rev. C13, 907 (1976) Finite-Range Coupled-Channels Born Approximation NUCLEAR REACTIONS 12C(6Li, d), E=18 MeV; 24Mg(p, d), E=28 MeV; 12C(d, 6Li), E=35 MeV; calculated σ(θ).
doi: 10.1103/PhysRevC.13.907
1976NA14 Phys.Lett. 63B, 11 (1976) Exact Finite Range CCBA Results for the Reaction 24Mg(d, p)25Mg at 14 and 15 MeV NUCLEAR REACTIONS 24Mg(d, p), E=15, 14 MeV; calculated σ(Ep, θ). CCBA analysis.
doi: 10.1016/0370-2693(76)90455-X
1976NA19 Phys.Rev. C14, 1667 (1976) Exact Finite-Range CCBA Calculations for the Reaction 16O(d, 6Li)12C At E = 35 MeV NUCLEAR REACTIONS 16O(d, 6Li), E=35 MeV; calculated σ(θ). CCBA, DWBA analysis.
doi: 10.1103/PhysRevC.14.1667
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