Fig. 2
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Schematic showing how a gap-opening planet triggers the C2H ring associated with the continuum gap. (a) Before runaway growth, a small planet is embedded inside the gaseous disk and carbon-rich ice is frozen out on pebbles. (b) During runaway gas accretion, the planet grows rapidly, consumes the pebbles in its vicinity, and opens a gas gap in the disk. Since the accreting planet is hot, carbon-rich volatile ice (e.g., methane) with lower sublimation temperature is readily liberated from the ice. On the other hand, the sublimation of H2O or CO2, which are the major oxygen carriers, can only be reached in the immediate vicinity of the planet (<RHill), at which point the material is lost to the planet. The discrepancy in sublimation temperature renders the gas C/O>1. In addition, stellar UV photons penetrate the gas gap. The combination of C/O>1 and high UV fluxes trigger photochemistry reactions to form the C2H ring. (c) After the gap opens, the supply of sublimated pebbles terminates due to the gap opening. The C/O ratio is smoothed out across the disk through radial mixing by diffusion.
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