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Table 3

Derived outflow energetics for different models.

log Mion log (Ekin/ [erg]) log (Ėkin(D)/ [erg s-1])a log (Ṁout(D)/ [M⊙ yr-1])b
Name Pixel-by-pixel Spherical Biconical Spherical Biconical
tot tot ENLR tot ENLR tot ENLR NLR tot ENLR tot ENLR NLR
SDSS J0233-0743 8.3 55.3 55.3 43.9 43.0 42.5 41.8 42.6 2.3 1.7 1.7 1.1 1.6
SDSS J0304+0022 8.1 56.8 55.3 45.4 43.0 43.8 41.7 43.8 2.8 1.6 2.0 0.9 1.9
SDSS J0311-0707 8.1 55.5 55.5 44.9 43.8 43.3 42.3 43.3 2.6 1.9 1.8 1.1 1.8
SDSS J0412-0511 8.9 55.9 56.4 45.8 44.1 44.4 42.7 44.5 3.3 2.2 2.7 1.4 2.7
SDSS J0753+3153 7.8 54.4 54.9 42.7 41.7 41.2 40.4 41.2 1.6 0.9 0.9 0.2 0.8
SDSS J0809+0743 8.5 56.2 55.5 45.2 43.7 43.5 42.2 43.5 2.9 1.9 2.0 1.0 2.1
SDSS J0847+2940 7.9 54.2 54.8 43.2 42.9 41.7 41.4 42.6 1.9 1.7 1.1 0.9 1.1
SDSS J0909+3459 8.3 54.7 54.8 44.2 43.7 42.6 42.2 43.1 2.5 2.2 1.6 1.3 1.6
SDSS J0924+0642 8.1 55.6 55.6 44.7 43.2 43.2 41.9 43.5 2.5 1.4 1.8 0.7 1.9
SDSS J0935+5348 8.4 55.6 56.0 44.5 43.6 42.8 42.0 43.0 2.7 2.1 1.7 1.2 1.8
SDSS J1144+1043 8.6 55.9 56.0 44.6 44.0 42.9 42.5 43.3 2.7 2.4 1.8 1.5 1.8
SDSS J2214+2115 7.9 54.9 55.6 43.6 43.7 42.2 42.3 42.4 2.0 1.8 1.3 1.0 1.3

Notes.

(a)

Kinetic power dreived from the total light and ENLR distribution for distance D = 5 kpc from the QSO for the spherical and conical model. For the conical model we also estimate the kinetic power for the unresolved NLR adopting a distance of D = 1 kpc.

(b)

Mass outflow rate from the total light and ENLR distribution for distance D = 5 kpc from the QSO for the spherical and conical model. For the conical model we also estimate the kinetic power for the unresolved NLR adopting a distance of D = 1 kpc.

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