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This article has an erratum: [https://doi.org/10.1051/0004-6361/200912350e]


   

Table 4:

Line intensity ratios between the peak antenna temperatures, assuming a source size of 1.5''.

Molecule
Transitions Ratioa

CN
$\frac{2_{5/2}-1_{3/2}}{1_{3/2}-0_{1/2}}$ 0.61 $\pm$ 0.39

CN
$\frac{3_{5/2}-2_{5/2}}{2_{5/2}-1_{3/2}}$ 0.13 $\pm$ 0.04

HCN
$\frac{3-2}{1-0}$ 1.01 $\pm$ 0.53

HCN
$\frac{4-3}{3-2}$ 0.49 $\pm$ 0.14

HNC
$\frac{3-2}{1-0}$ 0.38 $\pm$ 0.18

HNC
$\frac{4-3}{3-2}$ 0.30 $\pm$ 0.10

HCO+
$\frac{3-2}{1-0}$    0.12 $\pm$ 0.04b

HCO+
$\frac{4-3}{3-2}$ 1.37 $\pm$ 0.46
a See Pérez-Beaupuits et al. (2007) for the J=1-0 and J=3-2 transitions. The low-J lines of HCO+ were obtained from Krips et al. (2008).
b This ratio slightly differs from that found by Krips et al. (2008) because we use the ratio between the peak main beam temperatures and we corrected the HCO+ J=1-0 line for the starburst contribution factor.

Source LaTeX | All tables | In the text

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