Abstract
The angular distribution of photodisintegration products, previously resolved into contributions with different angular momentum transfers jt=jγ1, is analyzed further according to the parity of jt. Odd values of jt+jγ+l correspond to parity-unfavored transitions which result from effectively pseudotensor interactions with the unobserved fragments. In electric dipole processes, these transitions yield an angular distribution with the fixed asymmetry parameter βunf=1 while the distribution of parity-favored transitions consists of three standard functions weighted by dynamical factors.