Table 3
SOFIA/GREAT and Herschel/PACS fluxes.
| Pointing | [C II] | [N II] 205μm | ||
|---|---|---|---|---|
| × 10−15 W m−2 | × 10−17 W m−2 | |||
| PACS | GREAT(a) | PACS | GREAT(a) | |
| #1 | 1.4 | 2.1 | ... | 5.4 |
| #2 | 3.3 | 5.8 | <1.3 | <3.6 |
| #3 | 1.1 | 1.7 | <1.0 | <1.8 |
| #4 | 2.2 | 2.7 | <1.7 | <3.1 |
| #5 | 0.4 | 0.11, 0.09(b) | <1.5 | <1.1, <1.9(b) |
| #6 | 2.1 | 2.9 | ... | <3.8 |
| #7 | 1.9 | 1.6 | ... | ... |
| #8 | 2.5 | 4.0 | ... | ... |
| #9 | ≈ 0.7 | 1.0 | ... | ... |
| #10 | 0.9 | 1.4 | ... | ... |
| #11 | 0.5 | 0.9 | ... | ... |
| #12 | ... | 0.6 | ... | ... |
Notes. (a) Velocity-integrated values. For [N II], whose velocity structure is unknown, we calculate upper limits using the [C II] velocity profile. (b) The first value corresponds to the −10.6 km s−1 component, the second value to the 5.7 km s−1 component. PACS fluxes are integrated in a 17.2′′ aperture (see text). The values reported for GREAT (collected over a 17′′ beam) are integrated over the velocities (i.e., not from a fit).
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