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Table B.1

Comparison between the results obtained with different implementations of HiFIVe and FilChap (see Sect. B.3) in OMC-1 and OMC-2.

Source Parameter

σnt/cs M/L FWHM Structures
[] [M pc−1] [pc] [#]
Table 2, Hacar et al. (2018)
OMC-1 0.89 ± 0.28 24 ± 22 (*) ~0.02 − 0.05 28
OMC-2 0.65 ± 0.13 31 ± 25 (*) ~0.02 − 0.05 27

this work, [26, 44, 66] Av
OMC-1 0.990.19+0.15${0.99_{ - 0.19}^{ + 0.15}}$ 255+14${25_{ - 5}^{ + 14}}$ 0.0380.010+0.009${0.038_{ - 0.010}^{ + 0.009}}$ 27
OMC-2 0.600.17+0.14${0.60_{ - 0.17}^{ + 0.14}}$ 3514+16${35_{ - 14}^{ + 16}}$ 0.0460.015+0.015${0.046_{ - 0.015}^{ + 0.015}}$ 30

this work, [20, 40, 60, 80, 100, 120] Av
OMC-1 0.990.12+0.12${0.99_{ - 0.12}^{ + 0.12}}$ 278+30${27_{ - 8}^{ + 30}}$ 0.0340.007+0.010${0.034_{ - 0.007}^{ + 0.010}}$ 30
OMC-2 0.660.13+0.11${0.66_{ - 0.13}^{ + 0.11}}$ 4025+37${40_{ - 25}^{ + 37}}$ 0.0430.009+0.018${0.043_{ - 0.009}^{ + 0.018}}$ 46

Notes. The errors for our results have been computed as Inter-Quartile Range (IQR).

(*) The line masses from Hacar et al. (2018) have been multiplied by a factor 2.81/2.33 to account for the different μH2${\mu _{{{\rm{H}}_2}}}$ between the two works.

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