An empirical bond-order potential for semiconductors is developed. The
total energy is expressed as the sum of contributions of individual b
onds weighted by a bond-order term. For the bond-order term the tight
binding second moment approximation is used. The application to silico
n in its diamond structure gives results comparable to those obtained
with the Tersoff potential. A parameter set for GaAs is proposed yield
ing elastic constants and surface and defect properties in good agreem
ent with experimental and quantum mechanical results. Because of its g
enerality and small number of fitting parameters, the potential is eas
y to apply to a wide range of semiconducting materials.