Structure ofIn113studied via the reactionsIn115(p,t)In113,Cd112(He3,d)In113, andCd112(He4,t)In113

${}_{}{}^{115}{}_{}{}^{}\mathrm{In}\mathrm{}(p,t)\mathrm{}{}_{}{}^{113}{}_{}{}^{}\mathrm{In}$, ${}_{}{}^{112}{}_{}{}^{}\mathrm{Cd}({}_{}{}^3{}_{}{}^{}\mathrm{He},d){}_{}{}^{113}{}_{}{}^{}\mathrm{In}$, and ${}_{}{}^{112}{}_{}{}^{}\mathrm{Cd}(\alpha ,t){}_{}{}^{113}{}_{}{}^{}\mathrm{In}$ experiments have been done and distorted-wave Born approximation analysis has been used to obtain $L$ transfers and spectroscopic factors. Several new levels are reported and $J^{\pi }$ assignments are proposed. Two sets of states observed via the two types of reactions are classified as hole-core levels formed by coupling a proton hole to the states of ${}_{}{}^{114}{}_{}{}^{}\mathrm{Sn}$, and particle-core levels formed by coupling a proton to the states of ${}_{}{}^{112}{}_{}{}^{}\mathrm{Cd}$. Results of particle-core and hole-core model calculations are consistent with the observed spectroscopic factors and with the proposed level scheme.