Table 8
Integrated line fluxes for the transitions observed by PACS, and additional CO and H2 lines, as predicted by the models listed in Table 6.
| Species | λ [μm] | ν [GHz] | “low UV” model | “high UV” model | Fully mixed model | Power-law | Observed flux |
| Oi | 63.18 | 4745.05 | 200.6 | 222.0 | 191.4 | 170.3 | 193.1 (58.2) |
| Oi | 145.52 | 2060.15 | 6.29 | 7.33 | 5.39 | 4.59 | <8.5 |
| Cii | 157.74 | 1900.55 | 8.32 | 8.40 | 11.2 | 9.98 | – |
| p-H2O 322 → 211 | 89.99 | 3331.40 | 1.22 | 1.68 | 1.20 | 0.353 | <9.4 |
| o-H2O 212 → 101 | 179.52 | 1669.97 | 4.40 | 4.19 | 2.43 | 3.94 | <14.5 |
| o-H2O 221 → 212 | 180.49 | 1661.64 | 0.847 | 0.993 | 0.618 | 0.243 | <16.2 |
| o-H2O 432 → 312 | 78.74 | 3810.01 | 2.33 | 2.94 | 2.20 | 0.840 | <15.0 |
| o-H2 S(1) | 17.03 | 17603.78 | 1.15 | 1.59 | 1.15 | 0.572 | <28 |
| OH | 79.11 | 3792.19 | 4.59 | 6.31 | 5.40 | 2.71 | <17.0 |
| OH | 79.18 | 3788.84 | 4.78 | 6.54 | 5.59 | 2.82 | <17.0 |
| CO J = 36–35 | 72.85 | 4115.20 | 0.335 | 0.489 | 0.423 | 0.132 | <11.6 |
| CO J = 33–32 | 79.36 | 3777.63 | 0.497 | 0.704 | 0.578 | 0.197 | <22.8 |
| CO J = 29–28 | 90.16 | 3325.12 | 0.763 | 1.03 | 0.732 | 0.311 | <11.1 |
| CO J = 18–17 | 144.78 | 2070.68 | 1.91 | 2.31 | 1.49 | 0.851 | <13.1 |
|
|
|||||||
| CO J = 3–2 | 866.96 | 345.80 | 1.26 | 1.27 | 1.22 | 1.49 | 1.65 (0.39) |
| CO J = 2–1 | 1300.40 | 230.54 | 0.401 | 0.401 | 0.397 | 0.464 | 0.379 (0.118) |
| 13CO J = 1–0 | 2720.41 | 110.20 | 0.0122 | 0.0115 | 0.0120 | 0.0127 | 0.0124 (0.007) |
Notes. Observed fluxes for comparison. Fluxes in [10-18 W/m2] . Errors are a quadratic sum of the calibration error (20% for the interferometric CO observations and 30% for the PACS observations) and the rms continuum noise.
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