Table 5
Normalized spectral line emission distribution.
Transition | Obs. | BNF a | F em b | F abs c | L cor d |
(Jy km s-1) | (104 L⊙) | ||||
|
|||||
The 12CO ladder | |||||
|
|||||
J = 1–0 | SEST | 0.53 | 583 ± 87 | 340 | 0.16 ± 0.05 |
J = 2–1 | SEST | 0.99 | 1705 ± 256 | 410 | 0.72 ± 0.20 |
J = 3–2 | JCMT | 2.13 | 3151 ± 473 | 220 | 1.71 ± 0.29 |
J = 4–3 | APEX | 2.13 | 3513 ± 703 | 195 | 2.83 ± 0.61 |
SPIRE | 0.57 | 4208 ± 365 | |||
J = 5–4 | SPIRE | 0.66 | 3441 ± 155 | 170 | 2.87 ± 0.20 |
HIFI | 0.60 | 2803 ± 280 | |||
J = 6–5 | SPIRE | 0.75 | 2066 ± 66 | 145 | 2.30 ± 0.15 |
HIFI | 0.66 | 2291 ± 380 | |||
J = 7–6 | SPIRE | 0.63 | 1267 ± 46 | 140 | 1.58 ± 0.13 |
HIFI | 0.79 | 1229 ± 185 | |||
J = 8–7 | SPIRE | 0.62 | 961 ± 63 | 1.48 ± 0.20 | |
HIFI | 0.89 | 1477 ± 370 | |||
J = 9–8 | SPIRE | 1.25 | 790 ± 89 | 1.44 ± 0.16 | |
HIFI | 0.99 | 1246 ± 210 | |||
J = 10–9 | SPIRE | 1.45 | 494 ± 90 | 0.76 ± 0.15 | |
HIFI | 1.14 | 319 ± 106 | |||
J = 11–10 | SPIRE | 1.39 | 425 ± 120 | 0.79 ± 0.22 | |
J = 12–11 | SPIRE | 1.47 | 269 ± 90 | 0.55 ± 0.18 | |
|
|||||
The 13CO ladder | |||||
|
|||||
J = 1–0 | 0.017 ± 0.007 | ||||
J = 2–1 | 0.065 ± 0.019 | ||||
J = 3–2 | 0.122 ± 0.027 | ||||
J = 4–3 | – | ||||
J = 5–4 | 0.16 ± 0.0.04 | ||||
|
|||||
The carbon C° and C+ lines | |||||
|
|||||
[CI](1–0) | APEX | 2.17 | 6149 ± 922 | 655 | 4.2 ± 0.8 |
SPIRE | 0.63 | 4418 ± 207 | |||
HIFI | 0.58 | 5360 ± 804 | |||
[CI](2–1) | APEX | 7: | – | 1782 | 11.1 ± 2.4 |
SPIRE | 0.68 | 7613 ± 761 | |||
HIFI | 0.81 | 7408 ± 1111 | |||
[CII] | HIFI | 2.8 | 140 773 ± 21 115 | 1436 | 397 ± 60 |
[NII] | SPIRE | 1.47 | 14 832 ± 2000 | – | 31 ± 5 |
Notes.
Beam normalisation factor (BNF) to reduce observed emission line fluxes from Tables 2, 3, 4 to those enclosed by a 22′′ beam; for line fluxes expressed in K km s-1, multiply BNF by (θb/22)2, where θb is the observing FWHM beam-size from Tables 2 and 4.
Beam-independent absorption line flux derived from the estimated difference between integrated and Gaussian-fitted line intensities in Table 2; adopted error: 50%. Note that this is the total amount of absorption over the whole profile, not just the prominently visible deep absorption at systemic velocities.
Final adopted emission line luminosity in a 22′′ beam, corrected for absorption line losses. For 13CO we did not determine line fluxes, but derived corrected luminosities directly from the more accurate 12CO values using the mean of the 12CO/ 13CO ratios in Table 3.
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