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Table 2

Molecular line and continuum observations used in this work.

Disk Transition Int. flux(1) (Jy km s−1) Channel width (km s−1) Channel rms (mJybeam−1) Beam MRS(2) Robust Project code PI
LkCa15 12CO J = 2–1 16 ± 2 0.04 8.9 0″.34 × 0″.25 (−9.7°) 3″.7 −2.0 2018.1.01255.S M. Benisty
13CO J = 2–1 1.4 ± 0.2 0.17 4.4 0″,17 × 0″.13 (−13.7°) 0″.5 nat.(4) 2018.1.00945.S C. Qi
13CO J = 2–1 5.8 ± 0.6 0.33 3.1 0″.35 × 0″.25 (26.6°) 4″.0 −2.0 2018.1.00945.S C. Qi
13CO J = 6–5 7.5 ± 0.8 0.5 2.8 0″.08 × 0″.05 (−18.6°) 1″.2 0.5(5) 2017.1.00727.S J. Szulágyi
13CO J = 6–5 8.2 ± 0.9 0.44 25 0″.32 × 0″.30 (−31.2°) 2″.1 0.5 2017.1.00727.S J. Szulágyi
C18O J = 2–1 1.0 ± 0.1 0.33 3.9 0″.36 × 0″.27 (26.6°) 4″.0 −2.0 2018.1.00945.S C. Qi
0.45 mm cont. 0.16 0″.071 × 0″.048 (−23.5°) 1″.2 0.5 2017.1.00727.S J. Szulágyi
HD 169142 12CO J = 2–1 9.3 ± 0.9 0.17 1.7 0″.05 × 0″.029 (78.8°) 0″.6 0.5 2016.1.00344.S S. Pérez(3)
13CO J = 2–1 4.3 ± 0.4 0.17 2.3 0″.054 × 0″.035 (78.4°) 0″.6 0.5 2016.1.00344.S S. Pérez(3)
13CO J = 6–5 6.1 ± 0.7 0.44 12 0″.055 × 0″.054 (86.2°) 0″.6 0.0 2017.1.00727.S J. Szulágyi
C18O J = 2–1 2.0 ± 0.2 0.17 1.4 0″.052 × 0″.031 (78.6°) 0″.6 0.5 2016.1.00344.S S. Pérez(3)
0.45 mm cont. 0.52 0″.038 × 0″.037 (−72.0°) 0″.6 0.5(6) 2017.1.00727.S J. Szulágyi
1.3 mm cont. 0.022 0″.036 × 0″.018(73.0°) 0″.6 −0.5 2016.1.00344.S S. Pérez(3)

Notes. (1)Disk integrated flux calculated from the region within the Keplerian mask. The error includes the 10% absolute flux calibration error but not any uncertainty due to resolved-out large-scale emission. (2)The maximum recoverable scale (MRS) is estimated as ~0.983λ/L5, with λ the wavelength and L5 the fifth percentile baseline of the configuration. (3)Data first presented by Pérez et al. (2019).(4)Natural weighting with a 0″.15 uv taper.(5) ALMA image for which high and intermediate spatial resolution ALMA data are combined. (6)Product data.

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