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Table 6.

Properties of the ionised gas wind derived from [O III] emission.

L[O III] AV ne Mof rof vof of Ėkin
[1042 erg s−1] [cm−3] [106M] [kpc] [km s−1] [M yr−1] [1040 erg s−1]
(a) (b) (c) (d) (e) (f) (g) (h)
Nucleus (N) 22.9 ± 3 3.89 2325 0.39 ± 0.05 0.3 –895 ± 5 3.6 ± 0.5 91 ± 13
West cone 1 (W1) 6.2 ± 1 1.38 259 10 ± 2 1.5 217 ± 5 4.2 ± 0.7 7 ± 1
West cone 2 (W2) 1.1 ± 0.2 54 8 ± 1 6.7 217 ± 5 0.8 ± 0.2 1.3 ± 0.4
East cone 1 (E1) 2.2 ± 0.3 1.49 176 5.0 ± 0.7 1.5 –375 ± 5 3.8 ± 0.5 16.8 ± 3
East cone 2 (E2) 0.5 ± 0.1 22 9 ± 2 5.6 –227 ± 5 1.1 ± 0.2 1.8 ± 0.6

Notes. The table reports the main properties of the outflowing ionised gas detected through the [O III] emission line in different regions: N = nuclear region, W1 (W2) = west cone at r < 1.5 kpc (r > 1.5 kpc), E1 (E2) = east cone at r < 1.5 kpc (r > 1.5 kpc). (a) Extinction-corrected [O III] luminosity, (b) extinction, assumed negligible in W2 and E2, (c) electron density with a typical uncertainty of 0.6 dex (Baron & Netzer 2019), (d) wind mass, (e) wind radius, (f) wind velocity defined as v98, (g) outflow rate at radius rof, (h) outflow kinetic power.

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