Structure of collective states built on the isomer in : Quasiparticle-plus-triaxial-rotor model and interpretation as tilted-precession bands

Background: The shape of most nuclei is described by its quadrupole deformation (showing the deviation from spherical shape) and its triaxiality (showing the deviation from axial symmetry). Nuclei affected by triaxiality show additional collective rotational bands, called bands, that appear at low excitation energy. The bands can be caused by the precession of a nucleus with triaxial shape, but can also arise from small vibrations around an axially symmetric shape. Purpose: The aim of this work is to search for new collective excitations in in particular related with the degree of freedom.Methods: The rotational structures of were populated by the reaction at a beam energy of 37 MeV. The measurements of - coincidences, angular distribution ratios and -ray intensities were performed using eleven Compton-suppressed Ge clover detectors.Results: The previously known positive-parity band built on the isomer has been extended up and a new excited positive-parity band built above a state has been observed. The band was assigned a configuration while the new band was associated with a coupling of the valence neutron with the band of the even-even core. The quasiparticle-plus-triaxial-rotor model calculations provide a good agreement with the experimental data for both bands. They describe the band as a collective excitation with respect to the band that corresponds to a precession of the intermediate nuclear axis similarly to the precession of a rotating top.Conclusions: As shown by the calculations, the new rotational band can be understood as resulting from the three-dimensional rotation of a triaxially-deformed nucleus. However, a description based on the vibrations of a -soft nuclear shape should also be investigated in order to firmly establish the nature of the excited positive-parity band. Further studies able to distinguish between these alternative descriptions will be beneficial.