Table A.3
Line intensities from Odin and IRAM observations in 2015
| Date(a) (yyyy/mm/dd.dd) | Molecule | Transition | Frequency(b) (MHz) | offset(c) (″) | Intensity (K km s−1) | Doppler shift (km s−1) |
|---|---|---|---|---|---|---|
| 2015/11/10.8 | H2O | 110−102 | 556935.988 | 10 | < 0.057 | |
| 2015/09/19.3 | HCN | 3-2 | 265886.434 | 1.5 | 0.060 ± 0.012 | -0.29 ± 0.13 |
| 2015/09/21.30 | HCN | 1-0 | 88631.848 | 0.9 | < 0.066 | |
| 2015/09/21.30 | CH3CN | 8-7 | 147174.588-147149.068 | 0.9 | sum(4lines)< 0.123 | |
| 2015/09/22.30 | CH3CN | 9-8 | 165569.082-165540.377 | 1.5 | sum(4lines)< 0.051 | |
| 2015/09/19.3 | CS | 5-4 | 244935.557 | 2.3 | < 0.043 | |
| 2015/09/21.30 | 3-2 | 146969.029 | 0.9 | < 0.064 | ||
| 2015/09/22.30 | H2S | 110−101 | 168762.762 | 1.5 | < 0.029 | |
| 2015/09/21.30 | CH3OH | 3K−2K | 143865.801-146368.342 | 0.9 | sum(7lines)< 0.153 | |
| 2015/09/22.30 | CH3OH | J1−J0E | 165050.175-165678.649 | 1.5 | sum(6lines)< 0.069 | |
| 2015/09/19.3 | CH3OH | 5K−4K | 241700.168-241904.401 | 2.3 | sum(4lines)=0.037 ± 0.021 | |
| 2015/09/19.4 | CH3OH | 52−4−1E | 266838.123 | 1.5 | < 0.033 | |
| 2015/09/22.30 | CH3OH | 11−10A−+ | 303366.893 | 1.3 | 0.057 ± 0.030 | −0.16 ± 0.32 |
| 21−20A−+ | 304208.324 | 0.022 ± 0.026 | −0.07 ± 0.37 | |||
| 31−30A−+ | 305473.472 | 0.050 ± 0.031 | −0.49 ± 0.51 | |||
| 41−40A−+ | 307165.911 | 0.061 ± 0.035 | −0.24 ± 0.36 | |||
| 51−50A−+ | 309290.354 | 0.001 ± 0.039 | ||||
| 2015/09/21.30 | H2CO | 212−111 | 140839.518 | 0.9 | < 0.060 | |
| 2015/09/19.3 | 312−211 | 225697.772 | 2.3 | < 0.033 | ||
| 2015/09/19.3 | CO | 2-1 | 230538.000 | 2.1 | < 0.041 | |
Notes. (a)Dates are rounded to the nearest tenth of a day for averages over several days. (b)From Müller et al. (2005) and Pickett et al. (1998). For HCN the strongest hyperfine components are in the integration window and the integrated intensity takes into account the weaker ones according to their statistical weight. (c)Average radial pointing offset.
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