The two stretching vibrations associated with the CCO ligand in (PPN)/sub 2/(Ru/sub 3/(CO)/sub 6/(/mu/-CO)/sub 3/(/mu//sub 3/-CCO)) (1) have been identified by isotopic substitution and fit to an approximate normal-coordinate analysis. The high-frequency CCO stretching component occurs in the carbonyl stretching region (1977 cm/sup /minus/1/), and significant mixing occurs between this CCO stretch and a terminal carbonyl stretch of the same symmetry. The low-frequency CCO stretching vibration has been identified in the Raman spectrum of 1 and in the IR or Raman spectra of the ketenylidene clusters H/sub 2/Ru/sub 3/(CO)/sub 9/(/mu//sub 3/-CCO), (PPN)/sub 2/(Fe/sub 3/(CO)/sub 9/(/mu//sub 3/-CCO)), and (Co/sub 3/(CO)/sub 9/(/mu//sub 3/-CCO))(PF/sub 6/). This mode was found in the 1200-1350-cm/sup /minus/1/ range, with the more positively charged clusters having lower frequencies. The position of the high-frequency CCO stretch of (PPN)/sub 2/(Ru/sub 3/(CO)/sub 6/(/mu/-CO)/sub 3/(/mu//sub 3/-CCO)) is sensitive to isotopic substitution at the central carbon atom of the CCO but relatively unaffected by /sup 13/C substitution at the basal carbon. The converse is true for the low-frequency CCO stretch. This pattern of isotope shifts has a simple explanation in the form of the normal modes, and it should prove useful in the search for CCO on metal surfaces. Several of the framework more » vibrations associated with the M/sub 3/C core of the above ketenylidene clusters are reported. Assignments were made with the aid of Raman depolarization ratio measurements on samples in CH/sub 2/Cl/sub 2/ solution and in some cases on polycrystalline solids. 36 refs., 8 figs., 6 tabs. « less