Answers are grounded in this paper and cite their sources.
CO isotopolog emission is widely used to infer gas masses and volatile carbon abundances in protoplanetary disks, but converting line emission into a CO column depends on optical depth, temperature structure, line width, and isotope ratios. Inferring CO/H 2 additionally requires an independent constraint on the local hydrogen column. We use high-resolution 13 C 18 O 2–1 observations of HD 163296 to derive a spatially localized empirical constraint on the CO column at the resolved CO snowline edge. We focus on the 70–75 au annulus, on the inner, high-column side of the observed profile steepening near 75 au. Using RADEX slab calculations conditioned on a two-dimensional temperature structure, we infer an effective beam-averaged CO column from the absolute integrated intensity. Across representative temperatures, isotope-ratio pairs, and effective local line widths of 0.30 and 0.50 km s −1 , we find N CO beam = ( 1.6 –2.4) × 10 20 cm −2 and 13 C 18 O line-center optical depths τ = 0.39–0.97. Thus, even this rare isotopolog is not safely optically thin at the snowline edge. Adopting N H2 = 2.5 × 10 24 cm −2 from a published parametric gas surface density profile gives the conditional abundance CO/H 2 = (6.4–9.5) × 10 −5 . A beam-forward radial-profile analysis gives consistent columns, and a physical disk model with a near-canonical warm-layer CO abundance supplies a comparable CO column. The measurement is consistent with the higher C 17 O-based MAPS estimate. For the adopted hydrogen column, the inferred CO/H 2 ratio is consistent with a near-canonical abundance on the warm side of the snowline.
No takes yet. Share an insight, caveat, or question.
Qi et al. (2026) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: