Magnetic rotational bands in108Sb

High-spin states in ${}^{108}\mathrm{Sb}$ were populated using the ${}^{54}\mathrm{Fe}{(}^{58}\mathrm{Ni},3pn)$ reaction at a beam energy of 243 MeV and the subsequent γ decay was studied using the Gammasphere array. A new sequence of magnetic dipole transitions has been observed in addition to a previously known $M1\mathrm{}$ band in ${}^{108}\mathrm{Sb}.$ These bands may be interpreted, within the tilted axis cranking model as magnetic rotational bands with $\pi [g_{7/2}^2\otimes {(g}_{9/2}{)}^{-1}]$ $\otimes \nu \left[h_{11/2}\right]$ and $\pi [h_{11/2}{g}_{7/2}\otimes {(g}_{9/2}{)}^{-1}]\otimes \nu \left[{(g}_{7/2}{d}_{5/2}\right)]$ configurations.