Table 4.
Outflow properties measured from the [O III]λ5007 Å emission line.
ID | log ne ( * ) | Mout × 106 | Rout | PA | vout | Ṁout | log Ėkin | ξ |
---|---|---|---|---|---|---|---|---|
[cm−3] | [M⊙] | [kpc] | [ ° ] | [km s−1] | [M⊙ yr−1] | [erg s−1] | [%] | |
(1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) |
J1100 | 63 | 42.02 | 0.0148 | |||||
J1356 | 197 | 200 | −631 | 41.32 | 0.0060 | ||||
J1430 | 65 | 198 | −760529 | 41.13 | 0.0020 | ||||
J1509 | 320 | −1289 | 41.18 | 0.0012 | ||||
ID | log ne ( * *) | Mout × 106 | Rout | PA | vout | Ṁout | log Ėkin | ξ |
[cm−3] | [M⊙] | [kpc] | [ ° ] | [km s−1] | [M⊙ yr−1] | [erg s−1] | [%] | |
J1100 | 63 | 41.03 | 0.0015 | |||||
J1356 | 197 | 200 | −631 | 40.58 | 0.0011 | ||||
J1430 | 65 | 198 | −760529 | 40.90 | 0.0011 | ||||
J1509 | 320 | −1289 | 40.61 | 0.0003 |
Notes. (1) Object ID; (2) electron density; (3) mass of the outflowing gas; (4) maximum outflow radius; (5) position angle of the outflow; (6) outflow velocity measured from the velocity maps (negative velocities correspond to vel05 and positive to vel95); (7) mass outflow rate computed as 3 × vout × Mout/Rout; (8) outflow kinetic energy calculated as , with σ being the velocity dispersion, measured as FWHM = 2.355/σ, with FHWM = W80/1.09; (9) coupling efficiency (ξ = Ėkin/Lbol).
( * )Electron densities computed from the [S II]λλ6716, 6731 doublet ([S II]).
( * *)Electron densities computed using the trans-auroral lines (TA). Two values of Rout, PA, and vout are reported for J1356 and J1430 because the redshifted side of the outflow is also detected. For them, the outflow mass rates, kinetic powers, and coupling efficiencies are calculated independently for the blueshifted and redshifted sides of the outflow, and then added.
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