Interactions between catalytically active metal particles and reactant gases depend strongly on the particle size, particularly in the subnanometer regime where the addition of just one atom can induce substantial changes in stability, morphology, and reactivity. Here, time-lapse scanning tunneling microscopy (STM) and density functional theory (DFT)-based calculations are used to study how CO exposure affects the stability of Pt adatoms and subnano clusters at the Fe 3 O 4 (001) surface, a model CO oxidation catalyst. The results reveal that CO plays a dual role: first, it induces mobility among otherwise stable Pt adatoms through the formation of Pt carbonyls (Pt 1 -CO), leading to agglomeration into subnano clusters. Second, the presence of the CO stabilizes the smallest clusters against decay at room temperature, significantly modifying the growth kinetics. At elevated temperatures, CO desorption results in a partial redispersion and recovery of the Pt adatom phase. S ubnanometer metal particles exhibit a range of interesting electronic or catalytic properties that can vary substantially with the removal or addition of a single atom (1-6). Understanding the mechanistic details underlying the rearrangement of the active phase is important because changes in cluster size and shape are known to be commonplace under the conditions used in heterogeneous catalysis (7,8), and because such processes are associated with deactivation phenomena such as sintering. Although sintering is usually regarded as a thermally activated process, there is increasing evidence that adsorbates influence sintering rates in a reactive environment by formation of mobile metal-molecule intermediates (2,. Indeed, in a previous study we demonstrated that the formation of highly mobile Pd 1 -CO species led to enhanced sintering in the Pd/Fe 3 O 4 (001) system (31). Here, we turn our attention to Pt. Mobility is induced in the form of Pt 1 -CO. In addition, CO stabilizes the smallest clusters. When it desorbs, Pt dimers break up into single atoms; thus, the CO is necessary for preserving nuclei that act as seeds for further growth. Using roomtemperature scanning tunneling microscopy (STM), complemented by X-ray photoelectron spectroscopy (XPS) and density functional theory with an on-site Hubbard U (DFT+U), we follow the COinduced diffusion and coalescence of Pt atom-by-atom, creating catalytically active (32) subnano clusters with a well-defined size distribution. On heating, desorption of CO leads to significant redispersion of Pt into the adatom phase. Fig. 1B), the configuration commonly observed for other metal adatoms at this surface (31,35,36,39,40). DFT+U calculations find an adsorption energy ΔE ads (Pt 1 ) of 3.89 eV compared with free Pt atoms in vacuum and little charge transfer to the surface (<0.5 e − ). A second configuration, labeled Pt 1 *, not previously observed for other metals, appears offset to one side in STM images. Our DFT+ U calculations find a stable adsorption site [ΔE ads (Pt 1 *) = 3.01 eV, charge transfer <0.3...