The spectroscopy of neutron-rich sdf-shell nuclei using the CLARA-PRISMA setup

被引:0
|
作者
Liang, X. [1 ]
Hodsdon, A. [1 ]
Azaiez, F. [1 ]
Chapman, R. [1 ]
Haas, F. [1 ]
Bazzacco, D.
Beghini, S. [1 ]
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. [1 ]
Montagnoli, G.
Napoli, D. R.
Nowacki, F.
Ollier, J.
Papenberg, A.
Pollarolo, G.
Pucknell, V. F. E.
Salsac, M. -D.
Scarlassara, F.
Smith, J. F.
Spohr, K.
Stanoiu, M.
Stefanini, A. M.
Szilner, S.
Toniolo, N.
Trotta, M.
Verney, D.
Wang, Z.
Wrzesinski, J.
机构
[1] Univ Paisley, Sch Sci & Engn, Paisley PA1 2BE, Renfrew, Scotland
基金
英国工程与自然科学研究理事会;
关键词
gamma-ray spectroscopy; neutron-rich; deep-inelastic;
D O I
暂无
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
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-rich nuclei around N=20 and N=28. New results for the spectroscopy of neutron-rich N=22 Si-36 and P-37 are presented here.
引用
收藏
页码:37 / +
页数:2
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