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Table 3.

High-ionisation lines.

Line λvac IP Ref log Lline
(μm) (eV) (erg s−1)
(1) (2) (3) (4) (5)
[S VIII] 0.9916 281 L17, C21 < 37.0
Cr VIII 1.0109 160 < 36.9
[Fe XIII] 1.0750 331 L17, C21 < 37.0
[Fe XIII] 1.0801 331 L17, C21 < 37.0
[S IX] 1.2523 329 B23, C21 < 36.9
[Si X] 1.4305 351 C21
[Ti VI] 1.7156 99 < 37.3
[S XI] 1.9201 448 L17, C21 < 37.1
[Si XI] 1.9327 401 L17, C21 < 37.1
[Si VI] 1.9646 167 L17, C21, B23 < 37.1
[Al IX] 2.0450 285 C21 < 37.1
Sc V 2.3118 73 < 37.0
[Ca VIII] 2.3211 127 C21,R06 < 37.0
[Si VII] 2.4810 205 B23 < 37.0
[Si IX] 2.5850 303 S02, L00 < 37.1
Al V 2.9050 120 < 37.0
[Mg VIII] 3.0280 225 S02,B23, L00 < 37.0
[Ca IV] 3.2070 51 L00 < 36.7
[Al VI] 3.6603 154 < 36.9
[Al VIII] 3.6900 242 < 36.9
[Si IX] 3.9290 303 S02, L00 < 37.0
[Ca V] 4.1585 67 < 37.0
[Mg IV] 4.4880 80 S02, B23, L00 38.03 ± 0.01 (W)
37.72 ± 0.02 (E)
[Ar VI] 4.5292 75 B23, L00 < 37.0

Notes. Papers reporting the detection of high-ionisation lines: Sturm et al. (2002, S02), Lamperti et al. (2017, L17), Bianchin et al. (2024, B23), Cerqueira-Campos et al. (2021, C21), Lutz et al. (2000, L00). [Mg IV] luminosities are reported for both E and W nuclei; for all other high-ionisation lines, we report 3σ upper limits for the luminosities, assuming FWHM = 250 km s−1. [Si X] is not covered by NIRSpec observations (it falls in detector gap).

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