Motivation : Several theoretical comparisons with experimental data have
recently pointed out that the mass tensor of the collective Bohr Hamiltonian
cannot be considered as a constant and should be taken as a function of the
collective coordinates. Method : The Davydov-Chaban Hamiltonian, describing the
collective motion of {\gamma}-rigid atomic nuclei, is modified by allowing the
mass to depend on the nuclear deformation. Moreover, the eigenvalue problem for
this Hamiltonian is solved for Davidson potential and {\gamma} = 30{\deg}
involving an Asymptotic Iteration Method (AIM). The present model is
conventionally called Z(4)-DDM-D (Deformation Dependent Mass with Davidson
potential), in respect to the so called Z(4) model. Results : Exact analytical
expressions are derived for energy spectra and normalized wave functions, for
the present model. The obtained results show an overall agreement with the
experimental data for 108-116Pd, 128-132Xe, 136;138Ce and 190-198Pt and an
important improvement in respect to other models. Prediction of a new candidate
nucleus for triaxial symmetry is made. Conclusion : The dependence of the mass
on the deformation reduces the increase rate of the moment of inertia with
deformation, removing a main drawback of the model and leading to an improved
agreement with the corresponding experimental data.Comment: 20p, 8 figs, 3 Tabs (accepted for publication in nucl. Phys. A