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Table 2

Emission lines used to constrain the physical conditions and observed by the Herschel SPIRE FTS.

Transition Frequency Eup gup FWHM ϵ
(GHz) (K) (″) (10−9 W m-2 sr-1)
CO J = 4−3 461.041 55.32 9 41.7 1.40
[CI]3P0 -3P1 492.161 23.62 3 38.1 0.84
CO J = 5−4 576.268 82.97 11 33.5 1.27
CO J = 6−5 691.473 116.16 13 29.3 1.02
CO J = 7−6 806.652 154.87 15 33.0 1.02
[CI]3P1 -3P2 809.342 62.46 5 33.0 1.01
CO J = 8−7 921.800 199.11 17 33.2 1.88
CO J = 9−8 1036.912 248.88 19 19.1 2.22
CO J = 10−9 1151.985 304.16 21 17.6 2.53
CO J = 11−10 1267.015 364.97 23 17.3 2.65
CO J = 12−11 1381.995 431.29 25 16.9 2.52
CO J = 13−12 1496.923 503.13 27 16.6 4.37

Notes. The two last columns correspond to the instrument FWHM and to the mean 1σ uncertainty of the integrated line intensity.

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