Table 3.
Source parameters of AT2019wey.
Epoch | ν [GHz] | Sν [mJy] | θ [mas] | θmin [mas] | Tb [107 K] | Lν [1011 W Hz−1] | Figs. |
---|---|---|---|---|---|---|---|
1 | 6.7 | 1.2 ± 0.2 | 0.7 ± 0.1 | 0.14 | 6.4 ± 1.8 | > 1.4 | 2b |
2 | 1.6 | 1.2 ± 0.6 | 16.6 ± 7.6 | 3.19 | 0.21![]() |
> 1.5 | 2c1 |
4.5 | 1.5 ± 0.4 | 2.0 ± 0.4 | 0.50 | 2.2 ± 1.0 | > 1.8 | 2c2 | |
6.7 | 1.2 ± 0.3 | 1.0 ± 0.2 | 0.34 | 2.9 ± 1.4 | > 1.4 | 2c3 | |
3 | 1.6 | 0.8 ± 0.3 | 13.8 ± 5.9 | 3.07 | 0.18![]() |
> 0.9 | 2d1 |
4.5 | 0.8 ± 0.2 | 1.4 ± 0.3 | 0.59 | 2.5 ± 1.3 | > 1.0 | 2d2 | |
6.7 | 0.8 ± 0.2 | 0.9 ± 0.2 | 0.41 | 2.4 ± 1.3 | > 0.9 | 2d3 |
Notes. The model parameters corresponding to the source images in Fig. 2. Col. 2 – observing frequency; Col. 3 – flux density; Col. 4 – angular size, i.e. the FWHM of the circular Gaussian component; Col. 5 – minimum resolvable angular size of the VLBI array; Col. 6 – brightness temperature; Col. 7 – lower limit of the monochromatic luminosity, calculated by assuming that the source is located 1 kpc away from the Earth; Col. 8 – figure number. The errors of brightness temperatures at 1.6 GHz were likely overestimated and thus determined with the lower and upper bounds of the flux densities and source sizes.
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