Table 2
Properties of identified emission lines detected toward the continuum peak emission of IRAS2A around 219 GHz.
Rest frequency | Moleculea | Eupb | Size (FWHM)c | PAd | Fluxe | ncrit,100 Kf |
(MHz) | (K) | (arcsec) | (°) | (Jy/beam) | (cm-3) | |
|
||||||
216 945.60 | CH3OH (+?) | 56 | 0.7 × 0.4 (±0.03) | 30 | 0.51 | 7.1e6 |
216 966.65 | CH3OCHO | 111 | 0.47 × 0.40 (±0.05)⋆ | 41 | 0.25 | |
217 104.98 | SiO | 31 | – | – | – | 4.7e6 |
217 193.17 | CH3OCH3 | 253 | 0.48 × 0.15 (±0.1) | 33 | 0.04 | |
217 238.53 | DCN | 21 | 1.13 × 0.56 (±0.07)⋆ | 34 | 0.37 | |
217 299.20 | CH3OH, νt = 1 | 374 | 0.5 × 0.3 (±0.03)⋆ | 41 | 0.40 | |
217 359.28 | CH2DOH | 277 | 0.9 × 0.3 (±0.3) | −45 | 0.04 | |
217 447.90 | CH2DOH (+aGg′-(CH2OH)2) | 265 | point | 0.043 | ||
217 642.86 | CH3OH, νt = 1 | 746 | 0.46 × 0.23 (±0.05) | 62 | 0.14 | |
217 886.39 | CH3OH | 508 | 0.51 × 0.33 (±0.04)⋆ | 48 | 0.30 | |
218 222.19 | H2CO | 20 | 1.4 × 0.8 (±0.05)⋆⋆ | 25 | 0.83 | 5.0e6 |
218 280.90 | CH3OCHO | 100 | 0.45 × 0.35 (±0.1) | −31 | 0.07 | |
218 297.89 | CH3OCHO | 100 | 0.41 × 0.20 (±0.09) | 21 | 0.09 | |
218 316.39 | CH2DOH | 33 | 0.64 × 0.29 (±0.1) | −36 | 0.09 | |
218 324.71 | HC3N | 131 | 0.75 × 0.45 (±0.05)⋆ | 21 | 0.19 | |
218 440.05 | CH3OH | 45 | 0.79 × 0.50 (±0.03)⋆ | 27 | 0.81 | 7.8e7 |
218 459.65 | NH2CHO | 61 | 0.34 × 0.20 (±0.07)⋆⋆ | 72 | 0.1 | |
218 475.63 | H2CO | 68 | 1.0 × 0.60 (±0.03)⋆⋆ | 22 | 1.0 | 5.6e6 |
218 574.68 | aGg′-(CH2OH)2 | 207 | 0.88 × 0.25 (±0.3) | 40 | 0.05 | |
218 705.81 | (?+) aGg′-(CH2OH)2 | 195 | point | 0.04 | ||
218 760.07 | H2CO | 68 | 1.0 × 0.70 (±0.03)⋆⋆ | 21 | 0.96 | 6.1e6 |
218 903.35 | OCS | 100 | 0.9 × 0.6 (±0.02)⋆ | 25 | 0.89 | 4.0e5 |
218 981.17 | HNCO | 101 | 0.45 × 0.26 (±0.05)⋆ | 35 | 0.21 | 8.2e7 |
219 089.73 | aGg′-(CH2OH)2 | 173 | point | 0.04 | ||
219 173.75 | HC3N, ν7 = 1 | 452 | point | 0.03 | ||
219 385.18 | aGg′-(CH2OH)2 | 164 | point | 0.03 | ||
219 540.33 | HNCO, ν5 = 1 (+aGg′-(CH2OH)2) | 902 | point | 0.04 | ||
219 547.09 | HNCO (+ CH2DOH) | 709 | point | 0.03 | ||
219 551.48 | CH2DOH (+ HNCO) | 26 | 0.57 × 0.26 (±0.09) | 61 | 0.12 | |
219 560.35 | C18O | 16 | 5.0 × 4.0 (±0.15) | −80 | 3.0 | 9.6e3 |
219 580.67 | aGg′-(CH2OH)2 | 122 | point | 0.03 | ||
219 656.71 | HNCO | 448 | 0.38 × 0.10 (±0.09)⋆ | 23 | 0.08 | |
219 733.85 | HNCO | 228 | 0.59 × 0.14 (±0.07) | 39 | 0.15 | |
219 764.92 | aGg′-(CH2OH)2 | 113 | point | 0.03 | ||
219 798.32 | HNCO | 58 | 0.60 × 0.27 (±0.05)⋆ | 37 | 0.24 | 7.6e6 |
219 803.67 | (?+) aGg′-(CH2OH)2 | 156 | point | 0.05 | ||
219 908.48 | H213CO | 33 | 0.93 × 0.57(±0.05) | 19 | 0.34 | |
219 949.44 | SO | 35 | – | – | – | 3.7e6 |
219 983.99 | CH3OH | 802 | 0.31 × 0.18 (±0.1) | 53 | 0.08 | |
219 993.94 | CH3OH | 776 | 0.31 × 0.11 (±0.1) | 63 | 0.07 | |
220 038.07 | t-HCOOH | 58 | 0.39 × 0.07 (±0.11)⋆ | 33 | 0.10 | |
220 071.80 | CH2DOH | 17 | 0.65 × 0.44 (±0.05) | 42 | 0.31 | |
220 078.49 | CH3OH | 97 | 0.63 × 0.43 (±0.03)⋆ | 25 | 0.65 | 2.9e7 |
220 166.88 | CH3OCHO (+ HNCO, ν5 = 1) | 103 | 0.71 × 0.20 (±0.08) | 55 | 0.08 | |
220 178.19 | CH2CO | 46 | 0.60 × 0.53 (±0.07) | 85 | 0.16 | |
220 190.28 | CH3OCHO | 103 | 0.72 × 0.27 (±0.11) | 55 | 0.08 | |
220 193.86 | (?+) HNCO, ν5 = 1 | 967 | 0.60 × 0.39 (±0.16) | −5 | 0.07 | |
220 398.68 | 13CO (+CH3OH) | 16 | 9.5 × 5.4 (±0.30) | 47 | 3.6 | 9.7e3 |
220 401.37 | CH3OH (+13CO) | 252 | 0.45 × 0.25 (±0.04) | 48 | 0.28 | 9.3e6 |
Notes.
Molecule identified to be the source of the line emission. When two lines are too close in frequencies to be separated with the WideX channel width, the secondary spectral line is indicated in parentheses.
Size of the best fit of an elliptical Gaussian to the visibilities, see text for further details. Gaussian fits were performed on the channel showing the maximum emission (our data has a spectral resolution of 3.9 MHz ~ 2.7 km s-1). Most lines are detected at the systemic velocity Vsys ~ 7( ± 0.5) km s-1. Two notable lines show several blue-shifted velocity components: SiO shows emission at 7, 3, − 14.5, and − 32.5 km s-1, while SO is detected at velocities 6.5, − 0.5, and − 14.0 km s-1. No FWHM is indicated when the molecular emission is dominated by an outflow- or jet-like structure, as determined by a preliminary inspection of the emission maps line per line. The ⋆ symbol indicates the presence of a secondary component to be fitted at a different position in the map. The ⋆⋆ symbol indicates that, in addition to the component towards IRAS2A the line also traces outflow and/or complex structures at other locations in our maps.
Position angle of the elliptical Gaussian, when an elliptical Gaussian fit could be performed successfully.
Flux attributed to the best fit with a Gaussian component located at the center of the protostellar envelope.
Critical density of the transition, computed at 100 K, using the collision rates compiled in the LAMDA database when available. http://home.strw.leidenuniv.nl/~moldata/
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