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

hermitage

The Friction Model for Deep-Inelastic and Fusion Reactions,he region of the strong interaction nearly intact. Moreover, this reaction type exhausts a major part of the total reaction cross section. That is, the bulk of the accessible phase space at these energies is populated by these reactions.

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Supersymmetry Breaking Operators,n the meson-exchange model [2.3,4]. Assuming one of these realistic interactions, one tries to solve the many-body problem of A interacting nucleons and compares the results obtained for observables characterizing the ground-state and low-energy excitations with the experimental data.

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Sebastián Ventura,José María Lunaependent single-particle orbitals; correlations or direct two-body collisions are neglected. The TDHF approximation is expected to be valid for bombarding energies per nucleon that are significantly below the Fermi energy in nuclei, .cm ? ε. ≈ 40 MeV, where the Pauli principle prohibits most of the direct nucleon-nucleon collisions.

Eviction

The G-Matrix in Finite Nuclei,n the meson-exchange model [2.3,4]. Assuming one of these realistic interactions, one tries to solve the many-body problem of A interacting nucleons and compares the results obtained for observables characterizing the ground-state and low-energy excitations with the experimental data.

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The Time-Dependent Hartree-Fock Approximation for Nuclear Slabs,ependent single-particle orbitals; correlations or direct two-body collisions are neglected. The TDHF approximation is expected to be valid for bombarding energies per nucleon that are significantly below the Fermi energy in nuclei, .cm ? ε. ≈ 40 MeV, where the Pauli principle prohibits most of the direct nucleon-nucleon collisions.

Chronological

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修飾

hauteur

Supersymmetry Breaking Operators,, it is an approximation for the calculation of particle transfer reactions. The spin of the projectiles may be any combination of spin 0, spin 1/2, or spin 1. The following physical description uses the notation and formulation of [5.1], which describes nuclear reaction theory in detail.

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