NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Karp Found 9 matches. 1987VI02 Phys.Rev. C35, 2333 (1987) F.Videbaek, S.G.Steadman, G.G.Batrouni, J.Karp Anisotropies in Transfer-Induced Fission of 16O + 232Th NUCLEAR REACTIONS 232Th(16O, 15N), (16O, 16N), (16O, 17N), (16O, 16C), (16O, 15C), (16O, 14C), (16O, 13C), (16O, 12C), (16O, 13B), (16O, 12B), (16O, 11B), (16O, 10Be), E=105 MeV; measured transfer induced fission yields, probabilities, in-plane, out-of-plane fission anisotropies. ΔE-E telescope.
doi: 10.1103/PhysRevC.35.2333
1983BE26 Phys.Rev. C28, 667 (1983) G.M.Berkowitz, P.Braun-Munzinger, J.S.Karp, R.H.Freifelder, T.R.Renner, H.W.Wilschut Fusion near and below the Barrier for the Systems 32,34S + 24,25,26Mg and 32S + 27Al NUCLEAR REACTIONS, ICPND 27Al, 24,25,26Mg(32S, X), (34S, X), E(cm)=24-36 MeV; measured fusion σ(θ), σ vs E; deduced static deformation, zero point motion effects. 59,61Cu, 56,57,58,59,60Ni deduced fusion barrier parameters.
doi: 10.1103/PhysRevC.28.667
1983KA10 Phys.Rev. C27, 2649 (1983) J.S.Karp, D.Abriola, R.L.McGrath, W.A.Watson III Search for Transfer-Induced 12C + 12C Resonances in the 12C(16O, α)24Mg Reaction NUCLEAR REACTIONS 12C(16O, α), E=130 MeV; measured (12C)(12C)-coin. 24Mg deduced resonant state transfer production σ upper limit. Monte Carlo simulation.
doi: 10.1103/PhysRevC.27.2649
1982KA08 Phys.Rev. C25, 1838 (1982) J.S.Karp, S.G.Steadman, S.B.Gazes, R.Ledoux, F.Videbaek Statistical Behavior of Nucleon Transfer to Highly Excited States in Heavy-Ion Collisions NUCLEAR REACTIONS, ICPND 232Th(16O, X)10Be/11B/12C/13C/14C/15N, E=97, 105, 115, 125 MeV; deduced total σ, reaction σ. 181Ta, 232Th(15N, X), E=86, 95, 103 MeV; 181Ta(35Cl, X), E=205 MeV; measured σ(fragment θ, E) for X=9,10,11Be, 11,12,13B, 12,13,14,15,16C, 15,16,17N, 16,17,18,19O, 30,31,32Si, 31,32,33,34P, 33,34,35,36S, 36,37Cl; deduced reaction mechanism, dependence on transferred nucleon number, (Q)-dependence. Surprisal analysis.
doi: 10.1103/PhysRevC.25.1838
1982WI04 Phys.Lett. 113B, 141 (1982) H.W.Wilschut, P.Braun-Munzinger, G.M.Berkowitz, R.H.Freifelder, J.S.Karp, T.R.Renner The 19.7 MeV Resonance in the System 16O + 12C NUCLEAR REACTIONS, ICPND 12C(16O, 16O), E=45.5-49 MeV; measured σ(θ), σ(E). 28Si deduced resonance, Γ, Γp/Γ, J, π. S-matrix analysis.
doi: 10.1016/0370-2693(82)90411-7
1981MC13 Phys.Rev. C24, 2374 (1981) R.L.McGrath, D.Abriola, J.Karp, T.Renner, S.Y.Zhu Direct γ Transitions in 12C + 12C NUCLEAR REACTIONS 12C(12C, 12C'), E=25.8 MeV; measured (12C)(12C)-coin, σ vs (Q); deduced Γγ/Γ upper limit.
doi: 10.1103/PhysRevC.24.2374
1979AL22 Phys.Rev. C20, 1789 (1979) Y.Alhassid, R.D.Levine, J.S.Karp, S.G.Steadman Information-Theoretic Analysis of Energy Disposal in Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 232Th(16O, X), E=105 MeV; Mo(14N, X), E=97 MeV; 53Cr(15N, X), E=90 MeV; 232Th(15N, X), E=145 MeV; 232Th(22Ne, X), E=174 MeV; 197Au(16O, X), E=218, 250 MeV; Ni(16O, 12C), E=96 MeV; calculated energy spectra, Q-dependence for X from 7Li to 15O. Constrained statistical approach to multinucleon transfer.
doi: 10.1103/PhysRevC.20.1789
1978LE15 Phys.Rev.Lett. 41, 1537 (1978) R.D.Levine, S.G.Steadman, J.S.Karp, Y.Alhassid Heavy-Ion Transfer Reactions to the Continuum: Surprisal Analysis and The Condition of Maximal Entropy NUCLEAR REACTIONS 232Th(16O, 16N), (16O, 15N), (16O, 14C), (16O, 13C), (16O, 12C), 232Th(16O, 11B), E=105 MeV; measured σ.
doi: 10.1103/PhysRevLett.41.1537
1975HO11 Phys.Rev. A11, 916 (1975) F.Hopkins, R.Brenn, A.R.Whittemore, J.Karp, S.K.Bhattacherjee K- and L-Shell Ionization by Energetic Lithium Beams ATOMIC PHYSICS Al, Sc, Cu, Sn(Li, X), E=4=34 MeV; measured K X-ray yields.
doi: 10.1103/PhysRevA.11.916
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