Measurements of the $^{49}\mathrm{Ti}(d,t) ^{48}\mathrm{Ti}$ reaction have been carried out at 18 MeV with an energy resolution of about 10 keV. Single-particle strength distributions for $l=0,2,\mathrm{and} 3$ have been obtained up to excitation energy of 7 MeV in $^{48}\mathrm{Ti}$. About 85% of the $l=3$ strength is found in states below 3.6 MeV, and the total $l=3$ strength is consistent with the sum rule limit for $1{f}_{\frac{7}{2}}$ transfer to $T=2$ states. About three quarters of the sum rule limit for the $l=2$ strength (assumed be $1{d}_{\frac{3}{2}}$) and half the limit for the $l=0,2{s}_{\frac{1}{2}}$ strength is observed, with lower limits for the centroid energies of 5.36 and 5.17 MeV for the $1{d}_{\frac{3}{2}}$ and $2{s}_{\frac{1}{2}}$ hole, respectively. Measurements of inelastic $\ensuremath{\alpha}$ scattering on $^{48}\mathrm{Ti}$ have also been carried out at an incident energy of 28.5 MeV with a resolution of 18 keV. These measurements provide many new spin-parity assignments for natural parity states in $^{48}\mathrm{Ti}$. In combination with the pickup measurements, they provide identification for the centroids of the ${J}^{\ensuremath{\pi}}={(2,3,4,5)}^{\ensuremath{-}}$ states of the (${{f}_{\frac{7}{2}}}^{9}\ifmmode\times\else\texttimes\fi{}{{d}_{\frac{3}{2}}}^{\ensuremath{-}1}$) multiplet.