The magnetic moments of $2_1^{+}$ states of ${}_{}{}^{102-110}{}_{}{}^{}\mathrm{Pd}$, ${}_{}{}^{106-116}{}_{}{}^{}\mathrm{Cd}$, and ${}_{}{}^{130-136}{}_{}{}^{}\mathrm{Ba}$ have been measured by the dynamic field technique. The resulting magnetic moments are compared to the predictions of the vibrational model and to the interacting boson model.

NUCLEAR REACTIONS ${}_{}{}^{102-110}{}_{}{}^{}\mathrm{Pd}$(${}_{}{}^{32}{}_{}{}^{}\mathrm{S}$, ${}_{}{}^{32}{}_{}{}^{}\mathrm{S}$′) ${}_{}{}^{102-110}{}_{}{}^{}\mathrm{Pd}$ ($2_1^{+}$), ${}_{}{}^{106-116}{}_{}{}^{}\mathrm{Cd}$(${}_{}{}^{32}{}_{}{}^{}\mathrm{S}$, ${}_{}{}^{32}{}_{}{}^{}\mathrm{S}$′) ${}_{}{}^{106-116}{}_{}{}^{}\mathrm{Cd}$ ($2_1^{+}$), ${}_{}{}^{130-136}{}_{}{}^{}\mathrm{Ba}$(${}_{}{}^{32}{}_{}{}^{}\mathrm{S}$,${}_{}{}^{32}{}_{}{}^{}\mathrm{Ś}$)${}_{}{}^{130-136}{}_{}{}^{}\mathrm{Ba}$($2_1^{+}$) $E_S\sim 72-80$ MeV, enriched targets; measured $W(\theta ,H,\infty )$ through polarized iron; deduced $g\left(2_{}^{+}{}_1{}^{}\right)$.

• Received 20 September 1979

DOI:https://doi.org/10.1103/PhysRevC.21.574