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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.

(a)

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.

(b)

Upper-level energy of the transition.

(c)

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.

(d)

Position angle of the elliptical Gaussian, when an elliptical Gaussian fit could be performed successfully.

(e)

Flux attributed to the best fit with a Gaussian component located at the center of the protostellar envelope.

(f)

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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