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Table B.1.

Ionized gas kinematics from the 1D spectra extracted at the positions of the radio core and [O III] companions.

component redshift Δv σv
z km s−1 km s−1
TN J0121-radio core

0 3.5191±0.0003 9±17 191±11
1 3.5243±0.0002 352±10 132±7
2 3.5246±0.0002 373±12 628±10

J0121-[O III]

0 3.5236±0.0003 305±20 248±13
1( † ) 3.5255±0.0001 434±2 95±3

TN J0205-radio core

0 3.5015±0.0001 -302±4 158±5
1 3.5059±0.0001 -4±7 508±9
2 3.5091±0.0001 204±2 106±2

J0205-[O III]

0( † ) 3.4846±0.0001 -1426±8 309±7
1 3.5066±0.0003 42±18 618±21
2 3.5085±0.0001 167±4 174±6

4C03-radio core

0 3.5533±0.0002 -817±16 1092±12
1 3.5639±0.0007 -115±46 294±21
2 3.5691±0.0002 222±15 204±14

4C03-[O III]

0 3.5748±0.0001 595±4 158±6
1( † ) 3.5852±0.0002 1280±11 55±16
2( † ) 3.5872±0.0001 1410±9 574±5

4C19-radio core

0 3.5822±0.0021 -455±134 712±54
1 3.5933±0.0001 265±3 207±4
2 3.5947±0.0012 361±75 444±49

4C19-[O III]

0( † ) 3.5803±0.0001 -584±9 210±9
1 3.5874±0.0001 -121±7 98±8
2 3.5970±0.0001 512±3 213±3

Notes. Kinematic components of each sources are ordered based on their redshifts. Δv is calculated with respect to the systemic redshift listed in Table 1. The quoted uncertainties are 1σ errors from q3dfit. ( † ) Kinematic emission from of the potential [O III] companion.

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