Phys.Rev. C59, 1324 (1999)

D.Sohler, J.Cederkall, M.Lipoglavsek, Zs.Dombradi, M.Gorska, J.Persson, D.Seweryniak, I.Ahmad, A.Atac, R.A.Bark, J.Blomqvist, M.P.Carpenter, B.Cederwall, C.N.Davids, C.Fahlander, S.M.Fischer, H.Grawe, G.Hackman, R.V.F.Janssens, A.Johnson, A.Kerek, W.Klamra, J.Kownacki, C.J.Lister, S.Mitarai, D.Nisius, L.-O.Norlin, J.Nyberg, G.Poli, P.Reiter, J.J.Ressler, H.A.Roth, J.Schwartz, G.Sletten, J.Uusitalo, W.B.Walters, M.Weiszflog

Yrast States of the Proton Drip Line Nucleus ¹⁰⁶Sb

NUCLEAR REACTIONS ⁵⁴Fe(⁵⁸Ni, npα), E=261 MeV; measured Eγ, Iγ, (charged particle)γ-, (neutron)γ-, γγ-coin. ¹⁰⁶Sb deduced levels, J, π. Cluster detectors, Si-ball. Shell model analysis.

RADIOACTIVITY ¹⁰⁶Sb(IT) [from ⁵⁰Cr(⁵⁸Ni, np), E=220 MeV]; measured Eγ, Iγ(t). ¹⁰⁶Sb deduced isomeric state T_1/2, ICC. Fragment mass analyzer.

doi: 10.1103/PhysRevC.59.1324