Abstract
The wobbling motion in even-even nuclei is investigated by means of a collective Hamiltonian constructed from a semiclassical treatment applied to a triaxial rotor with a rigidly aligned pair of quasiparticles. The limits of distinct wobbling regimes are discussed in connection to the dynamic evolution of the wobbling excitations and corresponding electromagnetic properties. Model calculations are performed for the description of transverse wobbling bands in $^{130}\mathrm{Ba}, ^{134}\mathrm{Ce}$, and $^{136,138}\mathrm{Nd}$ nuclei.
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