We show the existence of a stress-induced coupling between upper-condu
ction-band states and valence-band states in bulk zinc-blende semicond
uctors and in their strained-layer low-dimensional systems. This coupl
ing is calculated by an empirical tight-binding method which exactly i
ncludes the full crystal symmetry of the strained semiconductor compou
nds. As an application, we report a study of CdTe-ZnTe superlattices h
aving thin ZnTe layers which exhibit an anomalously high energy for th
e electron to light-hole transition. We show that the large shift of t
his transition is well accounted for via mixing between valence and up
per-conduction bands.