Table D.1.
Position angle and hot spot distance of the radio jet.
| HzRG | PAradio† | rapp.* | rrec.* |
|---|---|---|---|
| deg | arcsec | arcsec | |
| MRC 0943-242 | 74 | 1.79 | 1.76 |
| MRC 0316-257 | 53 | 5.56 | 1.15 |
| TN J0205+2242 | 150 | 1.47 | 1.24 |
| TN J0121+1320 | 90 | 0.82a | 0.82a |
| 4C+03.24 | 146 | 2.00b | 1.75b |
| 4C+19.71 | 176 | 3.82 | 4.58 |
| TN J1338-1942 | 150 | 3.78 | 1.18 |
| 4C+04.11 | 158 | 1.15c | 1.70c |
Notes.
Jet position angle. This is measured east from north. We note that we do not quantify the uncertainties which could be ±1 deg.
Distance between the hot spot and the AGN position. rapp. and rrec. are distance for approaching and receding hot spot, respectively.
The radio emission of TN J0121+1320 is spatially unresolved. The ‘hot spot’ distance is represented by the distance from the host galaxy position to the either side of 3σ contour of the radio image along the east-west direction.
Approaching hot spot is A1 and receding hot spot is B1 (named after van Ojik et al. 1996).
Approaching hot spot is knot8 and receding hot spot is knot1 (named after Parijskij et al. 2014).
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