Table 3.
Same as Table 2: Analysis results obtained using the method described in Sect. 4.2.2.
| Gaussian | S | ν | Δν | B// |  |
 |
Heliocentric velocity |
|---|---|---|---|---|---|---|---|
| (mJy) | (MHz) | (MHz) | (mG) | (mG) | (mG) | (km s−1) | |
| (1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) |
| 1 | 1.65 ± 0.07 | 1408.3387 ± 0.0014 | 0.0298 ± 0.0014 | 54720.91 ± 0.35† | |||
| 2 | 4.35 ± 0.11 | 1409.9958 ± 0.0007 | 0.0388 ± 0.0010 | 54304.28 ± 0.17† | |||
| 3 | 3.68 ± 0.10 | 1410.0460 ± 0.0046 | 0.1406 ± 0.0042 | 54291.67 ± 1.16† | |||
| 4 | 4.99 ± 0.20 | 1410.4444 ± 0.0027 | 0.1361 ± 0.0046 | 4.0 ± 0.8* | 2.8 ± 1.0* | 5.7 ± 1.1* | 54191.66 ± 0.67† |
| 5 | 1.04 ± 0.09 | 1410.6005 ± 0.0020 | 0.0264 ± 0.0025 | 7.3 ± 1.7* | 7.8 ± 2.4* | 7.0 ± 1.9* | 54152.48 ± 0.50† |
| 6 | 1.90 ± 0.04 | 1410.8472 ± 0.0280 | 0.3175 ± 0.0217 | 54090.58 ± 7.03† | |||
| 7 | 3.94 ± 0.17 | 1411.5624 ± 0.0002 | 0.0051 ± 0.0003 | 54326.96 ± 0.06 | |||
| 8 | 2.93 ± 0.17 | 1411.6410 ± 0.0009 | 0.0290 ± 0.0015 | 54307.25 ± 0.24 | |||
| 9 | 4.85 ± 0.16 | 1411.6553 ± 0.0028 | 0.1068 ± 0.0038 | 54303.65 ± 0.69 | |||
| 10 | 3.22 ± 0.16 | 1411.8640 ± 0.0026 | 0.0495 ± 0.0027 | 54251.30 ± 0.65 | |||
| 11 | 4.23 ± 0.39 | 1412.0049 ± 0.0010 | 0.0266 ± 0.0017 | 54215.97 ± 0.25 | |||
| 12 | 3.40 ± 0.21 | 1412.0550 ± 0.0009 | 0.0144 ± 0.0009 | 11.7 ± 1.0 | 14.6 ± 1.5 | 11.0 ± 1.2 | 54203.43 ± 0.23 |
| 13 | 3.62 ± 0.26 | 1412.0870 ± 0.0006 | 0.0130 ± 0.0005 | 17.1 ± 1.2 | 14.9 ± 1.2 | 20.0 ± 2.0 | 54195.39 ± 0.15 |
| 14 | 22.56 ± 0.29 | 1412.1406 ± 0.0027 | 0.1008 ± 0.0026 | 54181.96 ± 0.69 | |||
| 15 | 2.43 ± 0.15 | 1412.2011 ± 0.0008 | 0.0165 ± 0.0010 | −4.4 ± 0.9 | −6.1 ± 1.4 | −3.5 ± 1.1 | 54166.80 ± 0.20 |
| 16 | 6.89 ± 0.54 | 1412.3052 ± 0.0006 | 0.0134 ± 0.0006 | 54140.70 ± 0.15 | |||
| 17 | 12.18 ± 0.84 | 1412.3370 ± 0.0010 | 0.0292 ± 0.0006 | 18.4 ± 2.1 | 19.5 ± 4.6 | 17.0 ± 1.5 | 54132.74 ± 0.25 |
| 18 | 1.83 ± 0.71 | 1412.3473 ± 0.0010 | 0.0155 ± 0.0013 | 54130.16 ± 0.24 | |||
| 19 | 8.63 ± 0.83 | 1412.3662 ± 0.0058 | 0.1116 ± 0.0024 | −24.5 ± 3.8 | −21.1 ± 3.3 | −32.8 ± 9.1 | 54125.42 ± 1.45 |
| 20 | 0.39 ± 0.51 | 1412.3964 ± 0.0020 | 0.0329 ± 0.0023 | 54117.85 ± 0.49 | |||
| 21 | 2.20 ± 0.21 | 1412.5148 ± 0.0031 | 0.0398 ± 0.0030 | 20.6 ± 3.2 | 16.5 ± 3.0 | 29.8 ± 6.3 | 54088.20 ± 0.77 |
| 22 | 0.87 ± 0.11 | 1412.7501 ± 0.0014 | 0.0119 ± 0.0014 | 8.4 ± 2.4 | 11.9 ± 3.7 | 5.8 ± 2.5 | 54029.24 ± 0.34 |
| 23 | 8.02 ± 0.07 | 1412.9356 ± 0.0003 | 0.0362 ± 0.0004 | 2.0 ± 0.4 | 1.9 ± 0.5 | 2.2 ± 0.5 | 53982.81 ± 0.09 |
| 24 | 3.64 ± 0.04 | 1413.0112 ± 0.0022 | 0.1838 ± 0.0021 | 53963.86 ± 0.56 | |||
| 25 | 0.98 ± 0.07 | 1414.5674 ± 0.0023 | 0.0277 ± 0.0023 | 53574.70 ± 0.57 |
Notes. Same as the notes of Table 2. In Column (5), the values annotated with an asterisk designate components attributed to the 1665 MHz OH transition. When these emissions are instead assumed to be dominated by the 1667 MHz OH transition, the derived values are 6.6 ± 1.3 mG and 12.1 ± 2.8 mG.
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