Phys.Lett. B 633, 696 (2006)

N.Marginean, S.M.Lenzi, A.Gadea, E.Farnea, S.J.Freeman, D.R.Napoli, D.Bazzacco, S.Beghini, B.R.Behera, P.G.Bizzeti, A.Bizzeti-Sona, D.Bucurescu, R.Chapman, L.Corradi, A.N.Deacon, G.de Angelis, F.Della Vedova, E.Fioretto, M.Ionescu-Bujor, A.Iordachescu, Th.Kroll, A.Latina, X.Liang, S.Lunardi, G.Montagnoli, R.Marginean, M.Nespolo, G.Pollarolo, C.Rusu, F.Scarlassara, J.F.Smith, K.Spohr, A.M.Stefanini, S.Szilner, M.Trotta, C.A.Ur, B.J.Varley, W.Zhimin

Shape transitions far from stability: The nucleus ⁵⁸Cr

NUCLEAR REACTIONS ²³⁸U(⁶⁴Ni, X)⁵⁴Cr/⁵⁸Cr/⁶⁰Cr, E=400 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. ^54,58,60Cr deduced levels, J, π; calculated B(E2). Interacting boson model, Clara and Prisma arrays.

doi: 10.1016/j.physletb.2005.12.047