Table B.1.
Measurements of the W80, v50, and v98 parameters of the ionised gas emission lines in the integrated nuclear spectra (R∼0.5″).
| Line | λ | v50AGN | v50NE | v50SW | W80AGN | W80NE | W80SW | v98AGN | v98NE | v98SW |
|---|---|---|---|---|---|---|---|---|---|---|
| (μm) | (km s−1) | (km s−1) | (km s−1) | (km s−1) | (km s−1) | (km s−1) | (km s−1) | (km s−1) | (km s−1) | |
| [Fe II] | 5.34 | 9.3 | −168.8 | – | 267.1 | 89.1 | – | 168.8 | 213.3 | – |
| [Fe VIII] | 5.45 | 27.5 | – | – | 305.6 | – | – | 289.4 | – | – |
| [Mg V] | 5.61 | −69.4 | −196.6 | – | 339.1 | 296.7 | – | 366.1 | 493.2 | – |
| [Ar II] | 6.98 | −47.9 | −150.1 | 21.0 | 272.3 | 340.4 | 204.2 | 252.2 | 354.3 | 217.3 |
| [Ne VI] | 7.65 | −58.1 | −159.1 | −6.7 | 302.9 | 252.5 | 252.5 | 411.5 | 310.5 | 259.2 |
| [Ar V] | 7.90 | −24.0 | – | – | 342.3 | – | – | 219.6 | – | – |
| [Ar III] | 8.99 | −33.1 | −250.0 | −32.2 | 300.8 | 214.9 | 257.8 | 248.0 | 376.9 | 248.0 |
| [S IV] | 10.51 | −62.3 | −172.6 | 12.1 | 294.1 | 257.3 | 257.3 | 429.9 | 319.6 | 318.7 |
| [Ne II] | 12.81 | −24.5 | −140.5 | 34.3 | 289.9 | 289.9 | 231.9 | 314.5 | 488.4 | 313.6 |
| [Ar V] | 13.10 | −50.0 | – | – | 226.8 | – | – | 163.5 | – | – |
| [Ne V] | 14.32 | −47.4 | −151.2 | −46.5 | 259.4 | 363.2 | 311.3 | 306.8 | 358.7 | 305.9 |
| [Ne III] | 15.55 | −26.1 | −169.4 | 22.6 | 334.4 | 334.4 | 286.6 | 312.7 | 408.2 | 261.4 |
| [S III] | 18.71 | −33.1 | −230.5 | 56.3 | 285.9 | 285.9 | 190.6 | 325.8 | 421.1 | 246.8 |
| [Ne V]† | 24.32 | 4.3 | −142.4 | 5.2 | 366.7 | 366.7 | 440.0 | 362.4 | 362.4 | 434.8 |
| [O IV] | 25.89 | 44.7 | −93.1 | 45.6 | 344.4 | 344.4 | 344.4 | 299.7 | 344.4 | 321.1 |
Notes. † indicates that the continuum near the line for the NE and SW regions contained strong wiggles and thus the measurements are not well constrained (see Fig. A.1). The v98 parameter is the maximum in absolute value between the v02 and v98 measurements. The different integrated regions nuclear-AGN, NE, and SW, are defined in see Sect. 3.
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