“…In the employed model, by selecting suitable separable, effective isoscalar and isovector forces, the rotational invariance (RI-) was restored to describe the magnetic dipole (M1) excitations [17,[37][38][39], as well as the translational and Galilean invariance (TGI-) [9,19] for calculating the E1 excitations. This model also satisfactorily described the fragmentation of electric and magnetic dipole strength in well-deformed [40][41][42][43][44][45][46][47][48][49][50][51], transitional, and γ-soft [9,10,13,19] nuclei, as well as the giant dipole resonance and pygmy dipole resonance [40, 42-44, 46, 49, 50] in deformed nuclei [17, 37, 40-48, 52, 53].…”