By A A Raduta; et al
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Additional info for Collective motion and phase transitions in nuclear systems : proceedings of the Predeal International Summer School in Nuclear Physics, Predeal, Romania, 28 August-9 September 2006
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The most advanced asymmetric two center shell model  was improved [32,33] and applied to calculate potential energy surfaces (PES) for cluster emitters (222Ra,232U,236Pu,242Cm) as well as for 228Th and for light (loSTeand 212Po)and superheavy (294118)alpha emitters . Other applications concerns the sub-barrier synthesis of 2 = 118 isotopes  and the study of input channels to produce 286~290~298114 [38,39]. The dynamical calculations have been performed in a multidimensional hyperspace of deformation coordinates followed by minimization of the action integral for all possible charge and mass asymmetries.
Due to this feature the study of the rotational bands in octupole deformed nuclei is of a paramount importance. However, it is difficult to identify the nuclei with a static octupole deformation The reason is that there is no measurable observable which may quantitatively describe the octupole deformation. Therefore, information about it should be indirectly obtained from energy levels. In the framework of microscopic theories the onset of octupole deformation is caused by the octupole interaction of orbits lying close to the Fermi sea and characterized by A j = A1 = 3.
Collective motion and phase transitions in nuclear systems : proceedings of the Predeal International Summer School in Nuclear Physics, Predeal, Romania, 28 August-9 September 2006 by A A Raduta; et al