Electron-positron momentum densities in CuCl are calculated along two
different crystallographic directions [001] and [110] with the use of
the empirical pseudopotential method (EPM) coupled with the independen
t particle method (IPM). The results exhibit features that are complet
ely different from those observed in other III-V semiconductors. The d
ip and valley observed in III-V compounds are replaced by peaks. These
differences are attributed to the very shallow ''d'' states in copper
.