The Spectroscopy of Neutron-Rich sdf-Shell Nuclei Using the CLARA-PRISMA Setup
- Liang, X.
- Hodsdon, A.
- Azaiez, F.
- Chapman, R.
- Haas, F.
- Bazzacco, D.
- Beghini, S.
- Behera, B.R.
- Berti, L.
- Burns, M.
- Caurier, E.
- Corradi, L.
- Curien, D.
- Deacon, A.
- De Angelis, G.
- Dombradi, Zs.
- Farnea, E.
- Fioretto, E.
- Gadea, A.
- Ibrahim, F.
- Jungclaus, A.
- Keyes, K.
- Latina, A.
- Margineau, N.
- Menegazzo, R.
- Montagnoli, G.
- Napoli, D.R.
- Nowacki, F.
- Ollier, J.
- Papenberg, A.
- Pollarolo, G.
- Pucknell, V.F.E.
- Salsac, M.-D.
- Scarlassara, F.
- F. Smith, J.
- Spohr, K.
- Stanoiu, M.
- Stefanini, A.M.
- Szilner, S.
- Toniolo, N.
- Trotta, M.
- Verney, D.
- Wang, Z.
- Wrzesinski, J.
DOIAbstract
Since the discovery of the breakdown of shell effects in very neutron-rich N=20 and 28 nuclei, studies of the properties of nuclei far from stability have been of intense interest since they provide a unique opportunity to increase our understanding of nuclear interactions in extreme conditions and often challenge our theoretical models.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-...
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