Nuclear Science References (NSR)

NUCLEAR STRUCTURE ²³⁸U; calculated lambda-hyperonic levels; deduced lambda-attachment probability features, hyperonic fission. Several fission paths, different asymmetries, several mechanisms.

doi: 10.1103/PhysRevC.47.1970
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1992TI03 Phys.Lett. 296B, 296 (1992)

G.-R.Tillack, R.Reif, A.Schulke, P.Frobrich, H.J.Krappe, H.G.Reusch

Light Particle Emission in the Langevin Dynamics of Heavy-Ion Induced Fission

NUCLEAR REACTIONS ¹⁹⁷Au(¹⁸O, F), E=159 MeV; calculated fission fragment total kinetic energy distribution, (fragment)n-coin, prescission particle multiplicities. ²¹⁵Fr deduced light particle emission features. Langevin dynamics.

NUCLEAR STRUCTURE ²¹⁵Fr; calculated prescission fission induced light particle multiplicities; deduced light particle emission features. Langevin dynamics.

doi: 10.1016/0370-2693(92)91323-2
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1989KR14 Nucl.Phys. A505, 417 (1989)

H.J.Krappe

Proximity Friction Reexamined

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), ²⁰⁰Hg(²⁰⁰Hg, X), E not given; calculated radial, tangential friction form factors; deduced inelastic excitation contribution. Perturbation theory.

doi: 10.1016/0375-9474(89)90384-9
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1986KR15 Phys.Lett. 181B, 191 (1986)

H.J.Krappe

Particle-Hole Level Density in Thomas-Fermi Approximation

NUCLEAR STRUCTURE ²⁰⁰Hg; calculated neutron level density. Thomas-Fermi approximation.

doi: 10.1016/0370-2693(86)90029-8
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1983KR16 Z.Phys. A314, 23 (1983)

H.J.Krappe, K.Mohring, M.C.Nemes, H.Rossner

On the Interpretation of Heavy-Ion Sub-Barrier Fusion Data

NUCLEAR REACTIONS, ICPND ¹⁰B(¹⁰B, X), E(cm) ≈ 2-4 MeV; ¹⁴N(¹⁰B, X), E(cm) ≈ 2.75-7 MeV; ¹²C(¹⁶O, X), E(cm)=4-12 MeV; ¹⁴N(¹⁶O, X), E(cm)=5.5-12 MeV; ²⁰Ne(¹²C, X), E(cm)=6-15 MeV; ⁹Be(¹⁶O, X), E(cm)=2.5-5 MeV; ¹²C(¹²C, X), E(cm)=2.5-5.5 MeV; ¹⁴N(¹²C, X), E(cm)=3.5-10 MeV; ¹⁴N(¹⁴N, X), E(cm)=4.5-11 MeV; ¹⁶O(¹⁶O, X), E(cm)=7-14.5 MeV; ¹¹⁰Pd(¹²C, X), E(cm)=30-50 MeV; ^64,58Ni(⁵⁸Ni, X), ⁶⁴Ni(⁶⁴Ni, X), E(cm)=90-110 MeV; ¹²²Sn(⁴⁰Ar, X), E=102.5-130 MeV; calculated fusion σ(E); deduced subbarrier fusion characteristics, neck formation role. Two-dimensional tunneling model.

doi: 10.1007/BF01411825
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1983KR17 Z.Phys. A314, 149 (1983)

H.J.Krappe, H.H.Rossner

Statistical Significance of Phase-Shift Analyses for Heavy-Ion Elastic-Scattering Data

NUCLEAR REACTIONS ⁵⁰Ti(α, α), E=140 MeV; analyzed σ(θ); deduced statistical significance. Phase shift analysis, heavy ion scattering.

doi: 10.1007/BF01879873
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1979KR08 Phys.Rev. C20, 992 (1979)

H.J.Krappe, J.R.Nix, A.J.Sierk

Unified Nuclear Potential for Heavy-Ion Elastic Scattering, Fusion, Fission, and Ground-State Masses and Deformations

NUCLEAR REACTIONS ¹²C(α, X), ²⁸Si(¹⁶O, X), ²⁰⁸Pb(⁸⁴Kr, X), E not given; calculated HI interaction potential. ²⁸Si(¹⁶O, ¹⁶O), E=37.7, 81.0, 215.2 MeV; calculated σ(θ). ²⁷Al(³²S, X), ⁶²Ni(³⁵Cl, X), ²⁰⁸Pb(¹⁶O, X); calculated compound nuclear σ, fission barrier heights, ground-state masses. Unified nuclear potential model.

doi: 10.1103/PhysRevC.20.992
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1978KR07 Z.Phys. A286, 331 (1978)

H.J.Krappe, H.Massmann

On the Theory of Fusion and Elastic Scattering of Deformed Aligned Heavy-Ions

NUCLEAR REACTIONS ⁵⁸Ni(²³Ne, X), E=56-66 MeV; calculated fusion σ(E). ⁵⁸Ni(²³Na, ²³Na), E=56-66 MeV; calculated σ(E).

doi: 10.1007/BF01408267
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1976KR15 Nucl.Phys. A269, 493 (1976)

H.J.Krappe

On the Topography of Potential-Energy Surfaces for Heavy-Ion Reactions

NUCLEAR REACTIONS ⁴⁰Ca(⁴⁰Ca, X), ⁸²Kr(⁸²Kr, X), ⁶⁰Zn(²⁰Ne, X), ¹²³Xe(⁴¹Ar, X), ¹⁴⁴Pr(¹⁴⁴Pr, X), ²¹⁵Ra(⁷³Zn, X); calculated potential energy surfaces.

doi: 10.1016/0375-9474(76)90695-3
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1969KR02 Nucl.Phys. A124, 641 (1969)

H.J.Krappe, U.Wille

Collective Model for Pear-Shaped Nuclei

NUCLEAR STRUCTURE ¹⁹F; calculated levels with collective model.

doi: 10.1016/0375-9474(69)90656-3
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