States inPt197populated by the (d,p), (d,t) and (n,γ) reactions

States in ${}_{}{}^{197}{}_{}{}^{}\mathrm{Pt}$ have been studied using the ${}_{}{}^{196}{}_{}{}^{}\mathrm{Pt}(d,p){}_{}{}^{197}{}_{}{}^{}\mathrm{Pt}$ and ${}_{}{}^{198}{}_{}{}^{}\mathrm{Pt}(d,t){}_{}{}^{197}{}_{}{}^{}\mathrm{Pt}$ reactions with 13.5 MeV deuterons and the ${}_{}{}^{196}{}_{}{}^{}\mathrm{Pt}(n,\gamma )$ reaction using thermal neutrons. The measured $Q$ values were 3.606 ± 0.020, - 1.221 ± 0.020, and 5.8463 ± 0.0004 MeV for the ($d,p$), ($d,t$), and ($n,\gamma$) reactions, respectively. Transferred $l$ values have been determined from angular distributions and spectroscopic factors determined by comparison with distorted-wave Born-approximation calculations. Some of the states can be tentatively assigned as Nilsson states arising from an oblate deformation. These include the ${5/2}^{-}$[532], decoupled ${1/2}^{+}$[600] and ${9/2}^{+}$[615] states. A number of low lying states with $l=1\mathrm{}$ cannot be explained using the Nilsson model or the shell model.