Abstract
The possible chiral interpretation of twin bands in odd‐odd nuclei was investigated in the Interacting Boson Fermion‐Fermion Model. The analysis of the wave functions has shown that the possibility for angular momenta of the valence proton, neutron and core to find themselves in the favorable, almost orthogonal geometry is present, but not dominant. Such behaviour is found to be similar in nuclei where both the level energies and the electromagnetic decay properties display the chiral pattern, as well as in those where only the energies of the corresponding levels in the twin bands are close together. The difference in the structure of the two types of chiral candidates nuclei can be attributed to different β and γ fluctuations, induced by the exchange boson‐fermion interaction of the Interacting Boson Fermion‐Fermion Model. In both cases the chirality is weak and dynamic. The existence of doublets of bands in 134Pr can be attributed to dynamic chirality dominated by shape fluctuations.
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