TY - JOUR
T1 - Lifetime measurements of strongly deformed rotational bands in 133Pm
AU - Galindo-Uribarri, A.
AU - Ward, D.
AU - Andrews, H. R.
AU - Ball, G. C.
AU - Radford, D. C.
AU - Janzen, V. P.
AU - Mullins, S. M.
AU - Waddington, J. C.
AU - Afanasjev, A. V.
AU - Ragnarsson, I.
PY - 1996/9
Y1 - 1996/9
N2 - We have measured lifetimes and deduced deformation parameters for rotational bands in 133Pm by the Doppler-shift attenuation method. A strongly coupled band based on the configuration with a hole in the g9/2 orbital has deformation parameter β2 = 0.40 (5), which is comparable to or larger than typical superdeformed bands in the A ∼130 region. We observe this band in 133Pm down to its I=K=9/2 bandhead. Calculations with a configuration-dependent shell correction to the cranked Nilsson potential can explain the existence of such low-spin superdeformed structures in the A ∼ 130 region. These shapes, which also occur in 129,131Pr, can be observed experimentally because of relatively low-lying shell gaps for β2=0.4 near Z=58, N=72. No high-spin intruder orbitals (vi 13/2) are occupied (over the spin range observed), however the strongly deformation-driving properties of a hole in the extruder πg9/2 orbital appear to be an essential ingredient in lowering the energy of the superdeformed shape.
AB - We have measured lifetimes and deduced deformation parameters for rotational bands in 133Pm by the Doppler-shift attenuation method. A strongly coupled band based on the configuration with a hole in the g9/2 orbital has deformation parameter β2 = 0.40 (5), which is comparable to or larger than typical superdeformed bands in the A ∼130 region. We observe this band in 133Pm down to its I=K=9/2 bandhead. Calculations with a configuration-dependent shell correction to the cranked Nilsson potential can explain the existence of such low-spin superdeformed structures in the A ∼ 130 region. These shapes, which also occur in 129,131Pr, can be observed experimentally because of relatively low-lying shell gaps for β2=0.4 near Z=58, N=72. No high-spin intruder orbitals (vi 13/2) are occupied (over the spin range observed), however the strongly deformation-driving properties of a hole in the extruder πg9/2 orbital appear to be an essential ingredient in lowering the energy of the superdeformed shape.
UR - http://www.scopus.com/inward/record.url?scp=0030492252&partnerID=8YFLogxK
U2 - 10.1103/PhysRevC.54.1057
DO - 10.1103/PhysRevC.54.1057
M3 - Article
AN - SCOPUS:0030492252
SN - 0556-2813
VL - 54
SP - 1057
EP - 1069
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 3
ER -