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Table 7.

Properties of the emission lines in the nucleus of Mrk 1044.

v (km s−1) σ (km s−1) F (10−16 erg s−1 cm−2)
Fe II] λ4713
−820 ± 30 667 ± 17 240 ± 40

Fe II] λ4720
−820 ± 30 667 ± 17 10 ± 20

Fe II] λ4731
−51.4 ± 1.4 252 ± 2 42.3 ± 1.2

[Fe II] λ4775
−51.4 ± 1.4 252 ± 2 8.8 ± 1.1

Fe II] λ4803
−51.4 ± 1.4 252 ± 2 31.0 ± 1.1

[Fe II] λ4815
−51.4 ± 1.4 252 ± 2 53.1 ± 1.1

Cr IIλ4824
−51.4 ± 1.4 252 ± 2 79.0 ± 1.7

Hβ
−218 ± 10 973 ± 5 1970 ± 20
−81.0 ± 1.0 285.1 ± 1.4 1523 ± 13

Cr IIλ4876
−51.4 ± 1.4 252 ± 2 30 ± 5

[Fe II] λ4890
−51.4 ± 1.4 252 ± 2 42 ± 3

[Fe II] λ4899
−51.4 ± 1.4 252 ± 2 10.2 ± 1.6

Ti IIλ4911
−51.4 ± 1.4 252 ± 2 5 ± 2

Fe IIλ4924
−820 ± 30 667 ± 17 184 ± 8
−51.4 ± 1.4 252 ± 2 207 ± 4

Fe II] λ4928
−51.4 ± 1.4 252 ± 2 12.0 ± 1.3

N Iλ4935
−51.4 ± 1.4 252 ± 2 34.5 ± 1.3

Fe IIλ4947
−51.4 ± 1.4 252 ± 2 12.2 ± 1.0

Fe IIλ4993
−51.4 ± 1.4 252 ± 2 2.4 ± 1.6

[O III] λ5007
−153.1 ± 0.5 141.6 ± 0.9 273 ± 2

Fe IIλ5018
−820 ± 30 667 ± 17 232 ± 7
−51.4 ± 1.4 252 ± 2 158 ± 4

[Fe II] λ5020
−51.4 ± 1.4 252 ± 2 25 ± 6

[Fe II] λ5031
−820 ± 30 667 ± 17 126 ± 4

Si IIλ5056
−820 ± 30 667 ± 17 141.3 ± 1.9

[Fe II] λ5060
−51.4 ± 1.4 252 ± 2 8.0 ± 1.9

Ti IIλ5072
−51.4 ± 1.4 252 ± 2 9.9 ± 0.9

Fe IIλ5102
−51.4 ± 1.4 252 ± 2 14.4 ± 0.8

[Fe VII] λ6087
−366 ± 2 241.3 ± 1.8 67.5 ± 0.6

Fe IIλ6149
−70 ± 3 212.0 ± 3 41.4 ± 0.7

Notes. The errors denote one-sigma uncertainties from a hundred Montecarlo realisations. For the lines at λ < 5110 Å, the broad and narrow components not belonging to either Hβ or [O III] also share the kinematics, as done in Park et al. (2022). The following narrow lines from Park et al. (2022) have a zero weight according to the fit: [Fe II] λ4775, [Fe II] λ4905, Ti IIλ4911, [Fe II] λ4973, Fe IIλ4993, [Fe II] λ5006, and [Fe II] λ5044. The same occurs for the following broad lines: Fe II] λ4713 and Fe IIλ4924. The errors in the kinematics of Fe IIλ4924 and the lines tied with it come from a preliminary fit where only the former line was characterised (see text).

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