Time-odd components in the mean field of rotating superdeformed nuclei

Rotation-induced time-odd components in the nuclear mean field are analyzed using the Hartree-Fock cranking approach with effective interactions SIII, SkM*, and SkP. Identical dynamical moments ${\mathcal{J}}^{\mathrm{}\left(2\right)\mathrm{}}$ are obtained for pairs of superdeformed bands ${}_{}{}^{151}{}_{}{}^{}\mathrm{Tb}$(2)${\mathrm{-}}^{152}$Dy(1) and ${}_{}{}^{150}{}_{}{}^{}\mathrm{Gd}$(2)${\mathrm{-}}^{151}$Tb(1). The corresponding relative alignments strongly depend on which time-odd mean-field terms are taken into account in the Hartree-Fock equations.