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Table E.1

CH3OH and SO line fluxes for the disks with methanol detections.

Name CH3OH Transition vCH3OH [GHz] Obs. flux [mJy km s−1] Resc. flux(a) [mJy km s−1] SO Transition vSO [GHz] Obs. flux [mJy km s−1] Resc. flux(a) [mJy km s−1] Refs.(b)
HD 100546 7(0,7)−6(0,6) A 338.4087 137 ± 19 149 ± 21 78 − 67 340.7142 343 ± 26 124 + 9 (1,2)
HD 169142 4(2,2)−3(1,2) E 218.4401 65 ± 7 379 ± 41 88 − 77 344.3106 120 ± 16 45 ± 6 (3,4)
HD 100453 6(1,5)−6(0,6) A 311.8526 141 ± 8 78 ± 5 77 − 66 301.2861 258 ± 5 99 ± 2 (5,6)
IRS 48 7(1,7)−6(1,6) E 338.3446 67 ± 4 441 ± 21 78 − 67 340.7142 1063 ± 23 569 ± 12 (7,8)
CQ Tau 6(1,5)−6(0,6) A 311.8526 54 ± 17 61 ± 19 65 − 54 219.9494 72 ± 15 82 ± 17 (9,10)
V883 Ori(c) 5(4,2)−6(3,3) A 364.2027 800 ± 180 (2.0±0.4)×105 65 − 54 219.9494 1100 ± 100 8449 ± 768 (11,12)
HL Tau 6(1,5)−6(0,6) A 311.8526 < 10 < 10 1515 − 1414 645.2549 591 ± 90 855 ± 130 (13,14)

Notes. All the observed line fluxes are disk-integrated, with the exception for those taken from the following references: Ruíz-Rodríguez et al. (2022); van't Hoff et al. (2018); Zagaria et al. (2025). (a)The observed CH3OH and SO line fluxes have been rescaled to a common distance of 140 pc and to the same transition (the 6(1,5)−6(0,6) A one for CH3OH and the JN = 65 − 54 transition for SO). (b)In the column, the first entry points to the reference where the CH3OH line flux values are presented, while the second entry does the same for SO. (c)The high rescaled CH3OH and SO fluxes inside the V883 Ori disk suggest that the emission could be optically thick. To be consistent with the other sources, we still rescale the fluxes using Eq. E.1 under the assumption of optically thin emission.

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