Abstract
The structure of parity doublet rotational bands in odd-A actinides is investigated in the di-nuclear system model, in which the cluster-type shape is described by collective oscillations in the mass asymmetry degree of freedom. The odd nucleon is assumed to move in the mean field produced by the even-even di-nuclear core, which is approximated by a Woods-Saxon potential with quadrupole and octupole deformation. The calculated spin dependence of the parity splitting is in good agreement with the experimental data.
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