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NSR database version of April 27, 2024.

Search: Author = J.S.Karp

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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, ^{56,57,58,59,60}Ni deduced fusion barrier parameters.

doi: 10.1103/PhysRevC.28.667
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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
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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, ^{12,13,14,15,16}C, ^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
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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
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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
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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
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