Table 5
Line fluxes and ratios for one position in the globule head.
| Instrument | Species | I(Θ = 20″) | I(Θ = 20″) | Ratio |
|---|---|---|---|---|
| [K km s−1] | [erg s−1 cm−2 sr−1] | |||
| HIFI | [C II] 158 μm | 153.5 | 1.08E-03 | − |
| PACS | [O I] 145 μm | 25.5 | 2.29E-04 | − |
| upGREAT | [O I] 63 μm | 6.3 | 6.85E-04 | − |
| SPIRE | [C I] 2–1 | 7.4 | 4.04E-06 | − |
| SPIRE | [C I] 1–0 | 10.2 | 1.25E-06 | − |
| upGREAT | 12CO 16→15 | 1.1 | 7.03E-06 | − |
| SPIRE | 12CO 13→12 | 9.3 | 3.19E-05 | − |
| SPIRE | 12CO 12→11 | 14.9 | 4.02E-05 | − |
| SPIRE | 12CO 11→10 | 20.5 | 4.27E-05 | − |
| SPIRE | 12CO 10→9 | 26.4 | 4.13E-05 | − |
| SPIRE | 12CO 9→8 | 31.7 | 3.62E-05 | − |
| SPIRE | 12CO 8→7 | 45.1 | 3.62E-05 | − |
| SPIRE | 12CO 7→6 | 51.3 | 2.76E-05 | − |
| SPIRE | 12CO 6→5 | 68.2 | 2.31E-05 | − |
| SPIRE | 12CO 5→4 | 91.8 | 1.80E-05 | − |
| SPIRE | 12CO 4→3 | 104.6 | 1.05E-05 | − |
| SPIRE | 13CO 9→8 | 2.6 | 2.61E-06 | − |
| SPIRE | 13CO 8→7 | 5.5 | 3.86E-06 | − |
| SPIRE | 13CO 7→6 | 9.0 | 4.24E-06 | − |
| SPIRE | 13CO 6→5 | 11.1 | 3.30E-06 | − |
| SPIRE | 13CO 5→4 | 19.9 | 3.41E-06 | − |
| SPIRE | [C I] 2–1/1–0 | − | − | 3.23 |
| SPIRE | 12CO 8–7/7–6 | − | − | 1.19 |
| SPIRE | 12CO 6–5/5–4 | − | − | 1.71 |
| SPIRE | 12CO 5–4/4–3 | − | − | 1.94 |
| SPIRE | 13CO 8–7/7–6 | − | − | 0.91 |
| SPIRE | 13CO 6–5/5–4 | − | − | 0.97 |
Notes. The fluxes are given in erg s−1 cm−2 sr−1, the ratios are determined from these fluxes for the SPIRE central pixel in the globule head (RA(2000) = 20h33m50s, Dec(2000) = 40°08′36″). All data points have the same angular resolution of 20″. The absolute error for the SPIRE data for the [C I] lines and CO J ≤ 8 is 2.5–3.1E07 erg s−1 cm−2 sr−1 and for J > 8 ~9E07 erg s−1 cm−2. The low- and mid-J CO data have a resolution of ~30–40″ so that we only use line ratios.
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