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Table 8
Line intensity ratios of C33S J = 2−1 hyperfine components.
Source | FWHM (km s−1) | R211 | R212 | R213 |
---|---|---|---|---|
W3OH | 4.41 | 0.29 ± 0.04 | 0.15 ± 0.03 | 0.05 ± 0.03 |
Orion-KL | 4.25 | 0.60 ± 0.02 | 0.30 ± 0.01 | 0.44± 0.02 |
G359.61−00.24 | 3.17 | 0.40 ± 0.05 | 0.62 ± 0.05 | 0.14± 0.04 |
G006.79−00.25 | 2.73 | 0.28 ± 0.02 | 0.17 ± 0.02 | … |
G010.32−00.15 | 2.66 | 0.27 ± 0.04 | 0.23 ± 0.06 | … |
G016.86−02.15 | 3.32 | 0.30 ± 0.05 | 0.18 ± 0.03 | … |
G017.02−02.40 | 3.74 | 0.17 ± 0.03 | 0.17 ± 0.08 | … |
G018.34+01.76 | 2.30 | 0.24± 0.07 | 0.13 ± 0.06 | … |
G019.36−00.03 | 3.02 | 0.29 ± 0.06 | 0.14± 0.04 | … |
G023.43−00.18 | 3.81 | 0.40 ± 0.14 | 1.15 ± 0.34 | … |
G024.78+00.08 | 4.29 | 0.34± 0.03 | 0.21 ± 0.03 | 0.08 ± 0.03 |
G028.39+00.08 | 3.04 | 0.26 ± 0.04 | 0.24± 0.06 | … |
G028.83−00.25 | 2.27 | 0.25 ± 0.04 | 0.18 ± 0.03 | … |
G030.70−00.06 | 4.85 | 0.33 ± 0.02 | 0.23 ± 0.03 | 0.11 ± 0.02 |
G030.74−00.04 | 3.55 | 0.19 ± 0.03 | 0.25 ± 0.06 | … |
G030.81−00.05 | 6.15 | 0.27 ± 0.03 | 0.16 ± 0.02 | 0.14± 0.02 |
G032.74−00.07 | 4.54 | 0.36 ± 0.04 | 0.16 ± 0.03 | … |
G032.79+00.19 | 4.78 | 0.09 ± 0.05 | 1.72 ± 0.28 | … |
G034.41+00.23 | 4.56 | 0.32 ± 0.04 | 0.28 ± 0.04 | 0.12 ± 0.03 |
G034.79−01.38 | 2.40 | 0.44± 0.15 | 0.14± 0.06 | … |
G037.42+01.51 | 3.18 | 0.20 ± 0.05 | 0.10 ± 0.02 | … |
W51-IRS2 | 8.55 | 0.13 ± 0.09 | 3.63 ± 0.36 | 0.71 ± 0.13 |
DR21 | 2.71 | 0.28 ± 0.01 | 0.20 ± 0.01 | 0.14 ± 0.01 |
G097.53+03.18 | 5.22 | 0.30 ± 0.05 | 0.13 ± 0.04 | 0.14± 0.04 |
G109.87+02.11 | 3.19 | 0.23 ± 0.06 | 0.38 ± 0.07 | … |
NGC7538 | 3.71 | 0.22 ± 0.01 | 0.21 ± 0.01 | … |
Notes. Full width at half maximum values of the main component were obtained from measurements of C33S; see Table A.3. The errors provided here are 1σ.
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