The positive parity levels in ${}_{}{}^{44}{}_{}{}^{}\mathrm{Ti}$ below 4.2 MeV and many of the $E2\mathrm{}$ transitions between them are fairly successfully explained using a soft asymmetric rotor model. A brief discussion of suggested negative parity states is also given.

NUCLEAR STRUCTURE ${}_{}{}^{44}{}_{}{}^{}\mathrm{Ti}$; calculated levels, $B\left(E2\mathrm{}\right)\text{'}\mathrm{s}$. Asymmetric rotor model with vibrations.

• Received 22 July 1974

DOI:https://doi.org/10.1103/PhysRevC.11.1828