Titlebook: Computational Nuclear Physics 2; Nuclear Reactions K. Langanke,J. A. Maruhn,S. E. Koonin Book 1993 Springer-Verlag New York, Inc. 1993 Pote

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Microscopic Description of Nuclear Collisions,any-body wave functions having well-defined quantum numbers and fulfilling the Pauli principle exactly. While the model is in principle an exact solution to the many-body problem, practical applications are restricted to the consideration of a model space spanned by a few cluster wave functions, acc

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Statistical-Model Calculations with Angular-Momentum Coupling, a nucleus A excited to an excitation energy ... The probability of emitting (“evaporating”) a neutron with a kinetic energy .,transforming the nucleus to .,with an excitation energy ..= .. − .. − . is calculated using the principle of detailed balance. This probability, which he denotes ..(.),can t

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The Time-Dependent Hartree-Fock Approximation for Nuclear Slabs,itations of the numerical methods employed — can be studied exactly. For this reason, it has given important insight into the reaction mechanism of heavy-ion collisions. The basic assumption behind TDHF is that the nucleons can at all times be regarded as independent particles that interact only thr

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The Friction Model for Deep-Inelastic and Fusion Reactions,ected reaction type in the early 1970s, the deep-inelastic collisions [9.1−3]. At bombarding energies below about 10 MeV/nucleon, colliding nuclei convert most of the surplus kinetic energy above their mutual Coulomb barrier into internal heating. Despite this violent excitation, both nuclei leave t

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