Extensive experimental studies have been performed on the solid-state formation of the OCS molecule in protonirradiated water-free and water-dominated ices containing CO or CO 2 as the carbon source and H 2 S or SO 2 as the sulfur source. In each case OCS is readily formed. Production efficiency follows the trends CO > CO 2 and H 2 S > SO 2 as C,O-and S-sources, respectively. In water-dominated ices, OCS production appears to be enhanced for CO : H 2 S reactants. The mechanism of formation of OCS appears to be the reaction of CO with free S atoms produced by fragmentation of the sulfur parent species. While OCS is readily formed by irradiation, it is also the most easily destroyed on continued exposure. In H 2 O-dominated ices the half-life of H 2 S, SO 2 , and OCS is $2 eV molecule À1 , corresponding to $7 million years in a cold dense interstellar cloud environment processed by cosmic-ray protons. The spectral profile of the 3 band of OCS is highly dependent on temperature and ice composition, and changes with radiation processing. These effects can be used in theoretical modeling of interstellar infrared (IR) spectra; a laboratory spectrum of irradiated H 2 O : CO : H 2 S, warmed to 50 K, provides a good fit to the 2040 cm À1 feature in the W33A spectrum. The identification of OCS in CO 2-dominated ices provides a further challenge, due to the overlap of the OCS band with that of CO 3 formed from irradiation of the host ice. The two features can be unraveled by a curve-fitting procedure. It is the width of the 2040 cm À1 band that will help observers determine if features identified in CO 2-rich ices are due to OCS or to CO 3 .