Table C.1
Best-fit discminer model parameters.
| Tracer | M* | υLSRK | i0 | PA | xc | yc} | z0 | p | Rt | q |
|---|---|---|---|---|---|---|---|---|---|---|
| (M⊙) | (km s−1) | (deg) | (deg) | (mas) | (mas) | (au) | (au) | |||
| 12CO | ![]() |
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| 13CO | ![]() |
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| C18O | ![]() |
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The total stellar mass of the binary M*, systemic velocity υLSRK, geometrical parameters (xc,yc offset from the central binary, PA position angle measured from the North to the redshifted major axis, and negative inclination i0 indicates anti-clockwise disk rotation), and emission surface parameters (z0, p, Rt, q describe an exponentially tapered power law) were inferred from the high-resolution cubes for 12CO and 13CO and the fiducial cube for C18O . The reported MCMC uncertainties are represented by the 16th and 84th percentiles drawn from the posterior distribution of the final 10% walkers of each model. These discminer-model uncertainties can increase by a factor of ∼10 due to spatially correlated noise, as shown by Hilder et al. (2025). The strongest correlation between model parameters is observed between the stellar mass and the disk inclination, which are known to be degenerate (e.g. Teague et al. 2018). This M* ∙ sin i0 degeneracy is evident through the varying best-fit parameters among CO isotopologs. Note that the inferred inclinations i0 and position angles PA between the CO tracers are significantly different, which we interpret as a sign of disk warping.
†Stellar masses for 12CO and C18O models with geometrical parameters fixed to the best-fit 13CO ones are 3.58 M⊙ and 5.01 M⊙, respectively.
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