Table 1
Targeted lines(a) of SO and SO2.
| Mol. | Trans.(b) | Freq. | Sijμ2 | Eup | ALMA Projects and targets(c) | Peak S/N(d) | Total flux(e) |
|---|---|---|---|---|---|---|---|
NJ ![]() |
GHz | D2 | K | mJy km s–1 | |||
| SO | 55 – 44 | 215.22065 | 11.5 | 44.1 | 2023.1.00592.S (L1527) | 20 | 1030±16 |
| 12 – 21 | 236.45229 | 0.03 | 15.8 | 2022.1.01411.S (IRS 63, DK Cha) | – | – | |
| 56 – 45 | 251.82577 | 11.6 | 50.6 | 2022.1.01411.S (IRS 63, DK Cha) | 27, 26 | 6200±50, 6300±80 | |
| SO2 | 163,13 – 162,14 | 214.68938 | 28.4 | 148 | 2023.1.00592.S (L1527) | 3 | 87±10 |
| 161,15 – 152,14 | 236.21668 | 16.1 | 131 | 2022.1.01411.S (IRS 63, DK Cha) | 3, 3 | 105±11, 480±30 | |
| 123,9 – 122,10 | 237.06887 | 18.4 | 93.9 | 2022.1.01411.S (IRS 63, DK Cha) | 3.5, 4 | 290±25, 590±35 | |
| 152,14 – 151,15 | 248.05740 | 14.1 | 119 | 2022.1.01411.S (IRS 63, DK Cha) | 2.5, 3 | 42±6, 510±32 | |
| 131,13 – 120,12 | 251.19967 | 25.7 | 82.2 | 2022.1.01411.S (IRS 63, DK Cha) | 7, 7 | 640±25, 1020±30 | |
| 83,5 – 82,6 | 251.21058 | 11.0 | 55.2 | 2022.1.01411.S (IRS 63, DK Cha) | 5, 4 | 600±23, 750±30 |
Notes.(a) The transition parameters are quoted from the JPL (Pickett et al. 1998) and CDMS (Endres et al. 2016) database through Splatalogue2. The columns from the left to right list the names of molecules (Mol.), transition quantum numbers (Trans.), rest frequency (Freq.), line strengths (Sijμ2), upper-level energies (Eup), and some notes (Note). The unit of Sijμ2 is Debye2 (denoted as D2). Note that transitions of molecules that have been covered by the observations but were not used in this work are not listed. (b) For both the upper and lower levels, the transition labels for SO and SO2 are NJ and
, respectively.(c) Only the targets relevant to this work are listed. IRS 63 represents Oph IRS 63.(d) The S/Ns are measured from spectra extracted at the emission peaks for the corresponding targets listed in the sixth column, under the native angular and spectral resolution, when cleaned with a “robust” parameter of 0.5. The S/Ns can be improved through smoothing. The symbol “–” indicates non-detection. (e) The total fluxes and their uncertainties for the corresponding targets listed in the sixth column, obtained by applying Gaussian fitting to the integrated spectrum over the whole emission region.
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