Table 4
Centimeter continuum properties of VLA1 and VLA2.
| λ | Beam | PA | Iν | Sν |
| (cm) | ( ) |
(°) | (mJy beam-1) | (mJy) |
|
|
||||
| VLA1 | 22:15:09.23 | +58:49:08.9 | (J2000) | |
|
|
||||
| 20.0 | 45 × 45 | 0 | 1.3 ± 0.47 | 2.9 ± 0.70 |
| 6.0 | 14.3 × 10.0 | + 33 | 4.2 ± 0.03 | 4.6 ± 0.08 |
| 6.0 | 0.41 × 0.36 | –17 | 1.6 ± 0.03 | 3.5 ± 0.11 |
| 3.6 | 8.3 × 5.9 | + 44 | 3.6 ± 0.02 | 4.1 ± 0.08 |
| 3.6 | 0.24 × 0.19 | +25 | 0.8 ± 0.02 | 3.5 ± 0.09 |
| 1.3 | 0.30 × 0.22 | + 31 | 0.8 ± 0.06 | 2.1 ± 0.20 |
| 0.7 | 0.63 × 0.39 | + 68 | 1.5 ± 0.18 | 2.1 ± 0.36 |
|
|
||||
| VLA2 | 22:15:07.26 | +58:49:17.9 | (J2000) | |
|
|
||||
| 6.0 | 14.3 × 10.0 | + 33 | 0.7 ± 0.1 | 0.8 ± 0.05 |
| 3.6 | 8.3 × 5.9 | + 44 | 0.4 ± 0.1 | 0.6 ± 0.06 |
Notes.
Error in intensity is the rms noise level of the map. Error in flux density is estimated as 
, where θsource is the size of the source which we used to calculate the flux density (outlined by the lowest contour in Fig. 1), θbeam is the size of the synthesized beam, σflux−scale is the error in the flux scale which takes into account the uncertainty of the calibration and is estimated as Sν × %uncertainty (%uncertainty is listed in Table 1).
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