The electronic structure of hydrogenated amorphous silicon layers is c
alculated within the empirical tight binding approximation. We predict
an important blueshift due to the confinement for layer thickness bel
ow 3 nm, and we compare with crystalline silicon layers. The radiative
recombination rate is enhanced by the disorder and the confinement bu
t remains much weaker than that in direct band gap semiconductors. The
comparison of our results with experimental data shows that the densi
ty of defects and localized states in the studied samples is quite sma
ll. (C) 1997 American Institute of Physics.