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Table 3
Results of fitting Gaussian profiles with single velocity components to observed spectra at selected positions.
| (Δα, Δδ) | Transition | I | υLSR | Δυ | N(C+) |
|---|---|---|---|---|---|
| (K km s−1) | (km s−1) | (km s−1) | (cm−2) | ||
| (− 61,45) | [13C II] | 3.99 ± 0.38 | 2.97 ± 0.1 | 1.74 ± 0.2 | 2.8(18) |
| [O I]145 | 70.77 ± 0.33 | 2.67 ± 0.1 | 1.79 ± 0.1 | ||
| 13CO(6–5) | 36.63 ± 0.22 | 2.71 ± 0.1 | 1.65 ± 0.1 | ||
| C18O(3–2) | 19.25 ± 0.09 | 3.08 ± 0.1 | 1.09 ± 0.1 | ||
| H2 S(2) | 1.5 × 10−4 | ||||
| H2 S(3) | 1.0 × 10−4 | ||||
| (− 33,6) | [13C II] | 5.33 ± 0.42 | 2.55 ± 0.1 | 3.08 ± 0.3 | 3.8(18) |
| [O I]145 | 50.77 ± 0.47 | 2.45 ± 0.1 | 2.55 ± 0.1 | ||
| 13CO(6–5) | 12.62 ± 0.68 | 3.41 ± 0.1 | 1.03 ± 0.1 | ||
| C18O(3–2) | 6.73 ± 0.11 | 3.06 ± 0.1 | 0.90 ± 0.1 | ||
| H2 S(2)(a) | 1.0 × 10−4 | ||||
| H2 S(3)(a) | 2.0 × 10−5 | ||||
| (− 31, − 31) | [13C II] | 4.34 ± 0.29 | 4.02 ± 0.1 | 2.28 ± 0.2 | 3.4(18) |
| [O I]145 | 48.21 ± 0.47 | 3.80 ± 0.1 | 3.02 ± 0.1 | ||
| 13CO(6–5) | 11.48 ± 0.60 | 3.50 ± 0.1 | 0.97 ± 0.1 | ||
| C18O(3–2) | 10.83 ± 0.10 | 3.10 ± 0.1 | 0.90 ± 0.1 | ||
| H2 S(2)(a) | 1.2 × 10−4 | ||||
| H2 S(3)(a) | 3.5 × 10−5 | ||||
| (32, − 23) | [13C II] | 3.34 ± 0.35 | 4.25 ± 0.2 | 2.74 ± 0.3 | 3.0(18) |
| [O I]145 | 19.17 ± 0.50 | 4.35 ± 0.1 | 2.93 ± 0.1 | ||
| C18O(3–2) | 4.77 ± 0.09 | 3.20 ± 0.1 | 1.09 ± 0.1 | ||
| H2 S(2)(a) | 3.0 × 10−5 | ||||
| H2 S(3)(a) | 1.1 × 10−5 | ||||
| (60, − 45) | [13C II] | 1.95 ± 0.24 | 3.91 ± 0.2 | 2.20 ± 0.3 | 1.3(18) |
| [O I]145 | 24.27 ± 0.67 | 3.58 ± 0.1 | 2.42 ± 0.1 | ||
| C18O(3–2) | 6.50 ± 0.10 | 3.23 ± 0.1 | 0.81 ± 0.1 | ||
| H2 S(2)(a) | 8.8 × 10−5 | ||||
| H2 S(3)(a) | 1.4 × 10−5 | ||||
Notes.
N(C+) is calculated assuming the lower limits of the kinetic temperature,
from Table 2.
(a) H2
data are taken from Larsson & Liseau (2017) and intensities are expressed in units of erg s−1 cm−2 sr−1.
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