Table A.2
Parameters of the 6.7-GHz CH3OH maser features detected in G30.76-0.05.
| (1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | (10) | (11) | (12) | (13) | (14) |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Maser | RAa | Deca | Peak flux | Vlsr | ΔvL |  |
χb |  |
TbΔΩc | PV | ΔVZ | |B||| | θd |
| offset | offset | Density(I) | |||||||||||
| (mas) | (mas) | (Jy/beam) | (km/s) | (km/s) | (%) | (°) | (km/s) | (log K sr) | (%) | (m/s) | (mG) | (°) | |
| G308.E01 | -168.187 | -21.082 | 0.215 ± 0.005 | 89.28 | 0.50 | − | − | − | − | − | − | − | − |
| G308.E02 | -163.384 | -23.605 | 0.274 ± 0.012 | 88.22 | 0.29 | − | − | − | − | − | − | − | − |
| G308.E03 | -81.835 | 116.776 | 0.113 ± 0.004 | 92.61 | 0.27 | − | − | − | − | − | − | − | − |
| G308.E04 | -72.856 | 103.867 | 0.159 ± 0.006 | 89.54 | 0.44 | − | − | − | − | − | − | − | − |
| G308.E05 | -41.918 | -19.604 | 0.578 ± 0.007 | 89.89 | 0.45 | − | − | − | − | − | − | − | − |
| G308.E06 | -31.682 | -239.437 | 0.239 ± 0.029 | 91.08 | 0.99 | − | − | − | − | − | − | − | − |
| G308.E07 | -30.824 | 61.823 | 0.436 ± 0.048 | 91.21 | 0.33 | − | − | − | − | − | − | − | − |
| G308.E08 | -30.709 | -0.284 | 13.831 ± 0.067 | 91.38 | 0.41 | 0.4 ± 0.1 | − 81 ± 19 |  |
 |
− | − | − |  |
| G308.E09 | -29.165 | 62.798 | 0.222 ± 0.018 | 90.90 | 0.57 | − | − | − | − | − | − | − | − |
| G308.E10 | -27.850 | 111.902 | 0.287 ± 0.019 | 90.94 | 0.15 | − | − | − | − | − | − | − | − |
| G308.E11 | -19.386 | 10.185 | 0.077 ± 0.008 | 91.78 | 1.87 | − | − | − | − | − | − | − | − |
| G308.E12 | -17.213 | -3.788 | 0.183 ± 0.006 | 90.24 | 0.33 | − | − | − | − | − | − | − | − |
| G308.E13 | -16.813 | 2.300 | 0.076 ± 0.008 | 90.59 | 2.74 | − | − | − | − | − | − | − | − |
| G308.E14 | -14.526 | -66.776 | 0.081 ± 0.006 | 90.46 | 0.97 | − | − | − | − | − | − | − | − |
| G308.E15 | -11.437 | -16.159 | 1.070 ± 0.029 | 91.12 | 0.41 | − | − | − | − | − | − | − | − |
| G308.E16 | -10.694 | 19.527 | 0.829 ± 0.006 | 93.71 | 0.24 | − | − | − | − | − | − | − | − |
| G308.E17 | -2.173 | -175.463 | 0.093 ± 0.018 | 92.17 | 0.87 | − | − | − | − | − | − | − | − |
| G308.E18 | -1.601 | 13.784 | 1.531 ± 0.009 | 93.32 | 0.34 | − | − | − | − | − | − | − | − |
| G308.E19 | -0.515 | 64.768 | 0.303 ± 0.040 | 91.82 | 0.48 | − | − | − | − | − | − | − | − |
| G308.E20 | 0 | 0 | 14.074 ± 0.085 | 91.82 | 0.38 | 1.9 ± 0.4 | 8 ± 3 |  |
 |
− | − | − |  |
| G308.E21 | 5.947 | 18.745 | 0.088 ± 0.005 | 92.53 | 0.27 | − | − | − | − | − | − | − | − |
| G308.E22 | 11.495 | -400.833 | 0.519 ± 0.074 | 91.87 | 0.38 | − | − | − | − | − | − | − | − |
| G308.E23 | 31.396 | -26.608 | 0.166 ± 0.023 | 92.13 | 0.19 | − | − | − | − | − | − | − | − |
| G308.E24 | 45.807 | -77.103 | 0.098 ± 0.007 | 93.93 | 0.23 | − | − | − | − | − | − | − | − |
Notes. (a)The reference position is α2000 = 18h47m39s.732 and δ2000 = −01°57′21″.975 (see Sec. 3). (b)Pl and χ are the mean values of the linear polarization fraction and the linear polarization angle measured across the spectrum, respectively. (c)The best-fitting results obtained using a model based on the radiative transfer theory of methanol masers for Γ + Γν = 1 s-1 (Vlemmings et al. 2010; Surcis et al. 2011b). The errors were determined by analyzing the full PDFprobability distribution function. (d)The angle between the magnetic field and the maser propagation direction is determined using the observed Pl and the fitted emerging brightness temperature. The errors were determined by analyzing the full PDF. The boldface indicates that |θ+ − 55°| < |θ−− 55°|, i.e., the magnetic field is parallel to the linear polarization vector (see Sect. 4).
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.