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Table 2

Line ratios R74 (I76/I43), R21 (I21/I10) and R14 (I10/I43) for all positions along the two cuts.

Δαδ R 74 R 21 R 14 T ex,43 T ex,74 N C    Tmb(C18O)dv N C18O N tot N(C)/Ntot M LTE M vir
 [″  /″ ]  [K] [K] cm-2 [K km s-1] [1015 cm-2] [1021 cm-2 [M] [M]

10/30 0.62 1.15 0.14 23 62 9.5 × 1016 1.6 2.27 11.35 8.4 × 10-6 236 208
20/10 0.47 1.09 0.08 33 53 1.7 × 1017 1.9 3.57 17.83 9.7 × 10-6 371 751
30/–10 0.47 0.91 0.11 43 53 3.9 × 1017 4.2 9.84 49.19 7.9 × 10-6 1024 1006
40/–30 0.45 1.09 0.10 42 52 4.1 × 1017 4.3 9.87 49.36 8.2 × 10-6 1028 1175
50/–50 0.48 0.79 0.15 34 54 3.7 × 1017 2.1 4.04 20.20 1.9 × 10-5 421 845

–30/60 0.43 8.89 0.01 21 51 1. × 1017 1.3 1.73 8.64 1.2 × 10-5 180 399
–50/50 0.44 0.84 0.12 24 51 1.5 × 1017 2.1 3.07 15.37 1. × 10-5 320 599

Notes. The LTE excitation temperature Tex,43 is derived from the optically thick I43 emission, Tex,74 is derived from R74 The C column densities are derived assuming LTE and optically thin [C i] emission. Values of the integrated intensities of CO 2–1 are given as presented in Nürnberger et al. (2002) along the two cuts, the LTE excitation temperature is derived from I43. The LTE column densities of CO, and the total gas column density assume an isotope ratio of 500 and CO:H2 = 8 × 10-5 (Frerking et al. 1982), i.e. a ratio of C18O/H2 = 2 × 10-7.

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