Table 2
Properties of methanol maser spots from D-conflguration maps for a selection of sources.
| Name (1) | a/Δa (h:m:s/″) (2) | δ/Δδ (d:m:s/″) (3) | Vlsr (km s−1) (4) | Sυ, Peak (Jy beam−1) (5) | Sυ, Int (Jy) (6) | Notes (7) |
|---|---|---|---|---|---|---|
| G35.2260–0.3544 | 18:56:53.2332 | +01:52:47.068 | 59.49 | 0.38 ± 0.02 | 0.39 ± 0.04 | YANG 19 |
| G35.2260–0.3544 | –0.17 | –0.34 | 59.13 | 0.12 ± 0.02 | 0.16 ± 0.04 | |
| G35.2260–0.3544 | 0.27 | 0.03 | 59.31 | 0.20 ± 0.02 | 0.19 ± 0.03 | |
| G35.2260–0.3544 | 1.32 | 0.84 | 59.67 | 0.14 ± 0.02 | 0.23 ± 0.04 | |
| G35.2476–0.2365 | 18:56:30.3917 | +01:57:08.664 | 72.25 | 1.40 ± 0.02 | 1.47 ± 0.03 | MMB |
| G35.2476–0.2365 | –1.30 | 1.68 | 71.53 | 0.12 ± 0.02 | 0.14 ± 0.03 | |
| G35.2476–0.2365 | –0.91 | –0.42 | 71.89 | 0.08 ± 0.02 | 0.10 ± 0.03 | |
| G35.2476–0.2365 | 0.12 | 0.16 | 72.43 | 1.34 ± 0.02 | 1.33 ± 0.04 | |
| G35.2476–0.2365 | 2.08 | 1.03 | 72.79 | 0.10 ± 0.02 | 0.22 ± 0.05 | |
| G35.3974+0.0252 | 18:55:50.7873 | +02:12:18.699 | 89.07 | 0.36 + 0.01 | 0.36 ± 0.02 | MMB |
| G35.3974+0.0252 | –2.04 | –2.05 | 88.89 | 0.12 + 0.01 | 0.15 ±0.03 | |
| G35.3974+0.0252 | –0.29 | 0.39 | 89.25 | 0.27 ± 0.02 | 0.32 ± 0.03 | |
| G35.3974+0.0252 | 0.76 | –0.28 | 89.43 | 0.19 ± 0.02 | 0.25 ± 0.04 | |
| G35.3974+0.0252 | 0.76 | –0.50 | 89.61 | 0.11 ±0.02 | 0.14 ± 0.04 | |
| G35.4166–0.2839 | 18:56:59.0536 | +02:04:54.463 | 56.11 | 1.67 ± 0.02 | 1.69 ± 0.03 | NEW |
| G35.4166–0.2839 | –0.05 | –0.49 | 55.75 | 0.21 ± 0.01 | 0.23 ± 0.02 | |
| G35.4166–0.2839 | 0.00 | –0.02 | 55.93 | 0.73 ± 0.01 | 0.72 ± 0.03 | |
| G35.4166–0.2839 | 0.17 | –0.07 | 56.29 | 1.35 ±0.02 | 1.35 ±0.03 | |
| G35.4166–0.2839 | –0.04 | –0.20 | 56.47 | 0.48 ± 0.02 | 0.55 ± 0.04 | |
| G35.4571–0.1782 | 18:56:41.0152 | +02:09:57.411 | 56.11 | 0.26 ± 0.02 | 0.31 ± 0.05 | NEW |
| G35.4571–0.1782 | –1.16 | 0.92 | 54.67 | 0.12 ± 0.02 | 0.21 ± 0.04 | |
| G35.4571–0.1782 | –0.08 | –0.11 | 54.85 | 0.19 ± 0.02 | 0.30 ± 0.05 | |
| G35.4571–0.1782 | –1.41 | –2.16 | 55.21 | 0.09 ± 0.01 | 0.17 ± 0.04 | |
| G35.4571–0.1782 | 1.16 | 0.48 | 55.39 | 0.11 ±0.01 | 0.09 ± 0.02 | |
| G35.4571–0.1782 | –0.66 | 0.20 | 55.57 | 0.24 ± 0.02 | 0.32 ±0.04 | |
| G35.4571–0.1782 | –1.01 | 0.30 | 55.75 | 0.20 ± 0.02 | 0.21 ± 0.04 | |
| G35.4571–0.1782 | –2.15 | –0.36 | 55.93 | 0.23 ± 0.02 | 0.27 ± 0.04 | |
| G35.4571–0.1782 | –0.45 | –0.46 | 56.29 | 0.17 ± 0.02 | 0.21 ± 0.04 | |
| G35.4571–0.1782 | –2.15 | –2.03 | 56.65 | 0.12 ± 0.02 | 0.18 ± 0.04 |
Notes. Column (1) gives the GLOSTAR source name based on the GLOSTAR Galactic coordinates. Columns (2) and (3) are the GLOSTAR equatorial coordinates of the position of the maser velocity component with the highest intensity. For sources with multiple components, we list their position offsets with respect to the component with the highest intensity. The position uncertainties are ~l.l″ (see Sect. 4.5). Column (4) gives the LSR radial velocity of the peak of the component. Columns (5) and (6) give the peak and integrated fluxes at the peak velocity, given by Col. (4). Column (7): Source references.
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