Abstract

We show that a wide range of deformed actinides can be described in terms of an interacting boson model hamiltonian with three parameters, two of them [including the coefficient of the only SU(3) symmetry breaking term] remaining almost constant over the whole region. In addition to ground γ 1 and β 1 spectra, B(E2:0 g + → 2 g +) values are well reproduced with no extra adjustable parameters for nuclei with 136⩽ N⩽146, while for nuclei beyond N = 146 an effective boson number has to be considered in order to fit the observed in the B(E2:0 + g → 2 + g) values, which is due to the presensce of a subshell closure at N = 152. The sensitive dependence of the B(E2:0 g +→2 g +) values on the effective boson numbers is emphasized. β 1 → ground and β 1 → ground transitions are fitted by breaking the SU(3) symmetry of the E2 transition operator.

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