Deep‐inelastic processes can be used to populated high spin states of neutron‐rich nuclei. In the deep‐inelastic processes, an equilibration in N/Z between the target and projectile nuclei is achieved. For most heavy neutron‐rich target nuclei, the N/Z ratio is 1.5 – 1.6, while for the possible neutron‐rich sdf‐shell projectile it is about 1.2. Thus by using deep‐inelastic processes one can populate neutron‐rich nuclei around N=20 and N=28.
New results for the spectroscopy of neutron‐rich N=22 36Si and 37P are presented here.
- neutron spectroscopy
- shell model
- properties of nuclei
- nuclear interactions