Abstract
The renormalized random-phase-approximation equations are solved for a density-dependent particle-hole force emerging from the nucleon-nucleon interaction. Migdal's renormalization constants are determined for and assuming Woods-Saxon states for the quasiparticle and quasihole propagation, and compared with the renormalization constants for a harmonic-oscillator propagation. In both cases the assumption of good isospin is made. Furthermore, we determined the renormalization constants in the , , , and problem in order to test the assumption of a mass-number-independent renormalization constant. For this purpose we used the standard harmonic-oscillator states for the quasi-single-particle (-hole) propagation (no good isospin).
- Received 3 September 1970
DOI:https://doi.org/10.1103/PhysRevC.3.563
©1971 American Physical Society