A possibility of intermediately bound excitons in semiconductors doped
with transition metal impurities is considered. These sorts of excito
n can appear in hexagonal (wurzite-type) semiconductors due to strong
hybridization of the conduction band states and the impurity d states.
In tetrahedral (zinc blende) semiconductors this hybridization is str
ongly suppressed due to a symmetry consideration. It is shown that the
exciton hole in ZnS:Ni (zinc blende type) is bound by the Coulomb fie
ld of the exciton electron and may be considered within the framework
of the hydrogen-like model. As for CdS:Ni (wurzite type) the orthogona
lization central cell pseudopotential appears to be the leading attrac
ting potential for the hole. These differences in the binding mechanis
ms account for striking differences measured experimentally in the str
ucture of the exciton spectra and values of the g-factors of these two
presumably similar systems.