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Table 3
Result of HFS line-fitting of the PdBI H13CN line.
| Source | ∫I dv | vlsr | σH13CN | τ | |
| [Jy/beam] | [km s-1] | [km s-1] | |||
|
|
|||||
| CygX-N3 | 0.113 ± 0.002 | 14.96 ± 0.12 | 0.69 ± 0.03 | 0.1 | |
| CygX-N12 | 0.076 ± 0.002 | 16.16 ± 0.29 | 0.98 ± 0.07 | 0.1 | |
| CygX-N48-1 | 0.05 ± 0.01 | −2.39 ± 0.04 | 0.53 ± 0.1 | 0.15 | |
| CygX-N48-2 | 0.127 ± 0.002 | −4.77 ± 0.02 | 0.86 ± 0.05 | 0.1 | |
| CygX-N53 | 0.063 ± 0.001 | −4.87 ± 0.03 | 1.1 ± 0.06 | 0.1 | |
| CygX-N63 | 0.063 ± 0.006 | −4.64 ± 0.1 | 2.05 ± 0.22 | 0.271 | |
Notes. The H13CN is taken from an average within the contour of 50% of the peak emission: peak intensity, local rest velocity, velocity dispersion and opacity. The same excitation temperature is assumed for all components.
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