Abstract

The boson expansion technique, extensively used in the past to describe anharmonic effects in spherical nuclei, is used to derive a boson formalism in a deformed basis (Nilsson model). The new formalism is then used to describe anharmonic gamma vibrations in $^{168}\mathrm{Er}$. The Hamiltonian adopted for practical calculations includes monopole and quadrupole pairing, and quadrupole particle-hole interactions. Some effects due to the coupling of the collective-noncollective modes and a three-body interaction are also taken into account in a perturbative fashion.

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