Gas-phase photolysis of metal-containing molecules readily causes photofragmentation to produce metal atoms and ions. [1][2][3][4] More recently it has been shown by luminescence spectroscopy that photolysis of these molecules also readily produces diatomic metal-containing molecules in the gas phase. [5][6][7][8][9][10][11] These discoveries have assisted in the elucidation of the photolytic decomposition pathways relevant to laser-assisted chemical vapor deposition (LCVD). Both desired fragments (e.g., TiN in the LCVD of TiN films) 11 and undesirable fragments containing heteroatoms that contaminate the final films (e.g., CuF, CrF, NiF, and PtC in the laser CVD of the respective metal films) 6-10 have been identified. The fluorinated acetylacetonate ligands (1,1,1,5,5,5-hexafluoro-2-4-pentanedionate ) hfac) that were used in the latter studies provide good precursor volatility and allow for facile transport in the gas phase, but they may also result in fluorine and/or carbon contamination of the final deposit. [12][13][14] The formation of diatomic metal fluorides can be easily eliminated by removing the fluorine substituents from the precursor, but the carbon that leads to metal carbide molecules cannot be so easily eliminated. A least-motion mechanism that was proposed to explain PtC formation is based on a change in the excited state from M-O bonding to η 1 bonding of the hfac ligand to the metal by its central carbon. 6,10 This type of bonding is known for some similar compounds in the ground state. 15 MF formation obviously must follow a different mechanism.During the course of our studies of the gas-phase photolysis of Pd(hfac) 2 , we discovered that PdC + is a common photoproduct over a wide range of irradiation wavelengths, but that the ratio of Pd + to PdC + is very sensitive to the wavelength. In the detailed studies reported in this communication, we show that changing the wavelength by a few angstroms can cause the formation of PdC + to disappear below the detection limit. The photoproducts are monitored by using time-of-flight mass spectroscopy. We demonstrate the selectivity over the 21 700-23 800cm -1 excitation region and explain the phenomenon in terms of the electronic excited states.The TOF mass spectrometer was constructed on the basis of a design in the literature. 16 Pd(hfac) 2 is admitted to the high-vacuum