Table 3.
Parameters of the detected continuum peaks.
| Band | Source | RA(J2000) | Dec(J2000) | Int. flux (a) | Peak flux(a) | Int. fluxn (b) |
|---|---|---|---|---|---|---|
| (h m s) | (° ′ ″) | (mJy) | (mJy beam−1) | (mJy) | ||
| L | VLA 1-3 | 18:34:20.903±0.002 | −05:59:41.77±0.08 | 1.98±0.26 | 1.40±0.12 | − |
| VLA 4 | 18:34:20.834±0.002 | −05:59:42.69±0.06 | 0.75±0.08 | 0.48±0.03 | – | |
| S | VLA 1-2 | 18:34:20.899±0.001 | −05:59:41.81±0.03 | 2.80±0.18 | 1.58±0.07 | – |
| VLA 3 | 18:34:20.907±0.0001 | −05:59:42.79±0.001 | 0.82±0.04 | 0.69±0.02 | – | |
| VLA 4 | 18:34:20.821±0.0001 | −05:59:43.13±0.002 | 0.47±0.03 | 0.43±0.02 | 0.50±0.05 (*) | |
| C | VLA 1 | 18:34:20.901±0.001 | −05:59:41.74±0.02 | 2.48±0.17 | 1.19±0.06 | – |
| VLA 2 | 18:34:20.909±0.0003 | −05:59:42.21±0.01 | 0.93±0.03 | 0.46±0.01 | – | |
| VLA 3 | 18:34:20.912±0.0002 | −05:59:42.91±0.004 | 0.69±0.02 | 0.48±0.01 | 1.09±0.10 (**) | |
| VLA 4 | 18:34:20.825±0.0003 | −05:59:43.17±0.01 | 0.47±0.02 | 0.33±0.01 | 0.57±0.04 (*) | |
| Ku | VLA 1A | 18:34:20.897±0.0003 | −05:59:41.59±0.004 | 0.58±0.04 | 0.39±0.02 | – |
| VLA 1B | 18:34:20.904±0.0004 | −05:59:41.86±0.01 | 0.96±0.07 | 0.34±0.02 | – | |
| VLA 2 | 18:34:20.914±0.0002 | −05:59:42.28±0.01 | 0.46±0.04 | 0.32±0.02 | – | |
| VLA 3 | 18:34:20.913±0.001 | −05:59:42.96±0.01 | 0.41±0.05 | 0.20±0.02 | 1.13±0.15 (**) | |
| VLA 4 | 18:34:20.825±0.002 | −05:59:43.22±0.02 | 0.31±0.08 | 0.09±0.02 | 0.53±0.08 (**) | |
Notes.
The parameters were obtained from the full UV range images presented in Fig. 1.
The normalised flux densities used for the spectral energy distributions (Fig. 3):
(*) values obtained for VLA 3 using a round beam and 943 kλ UV range (the longest baseline common to the bands at which VLA 3 is resolved), (**)values obtained for VLA 4 using a round beam and 481 kλ UV range (the longest baseline common to the bands at which VLA 4 is resolved).
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