Table 8.
Properties of the CIV outflows derived from the total profile of the CIV emission line.
| ID |  |
R |  |
Mout | Ṁout | Log(Ėkin/erg s−1) | Log(Ṗout/g cm s−2) |
|---|---|---|---|---|---|---|---|
| (1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) |
| km s−1 | pc | km s−1 | M⊙ | M⊙ yr−1 | |||
| X_N_160_22 | −30 | 0.06 | 250 | 68.46 | 0.10 | 39.31 | 32.21 |
| X_N_81_44 | 700 | 0.04 | 700 | 37.37 | 0.26 | 40.60 | 33.06 |
| X_N_53_3 | 540 | 0.03 | 470 | 29.40 | 0.17 | 40.07 | 32.69 |
| X_N_66_23 | 110 | 0.02 | 240 | 14.14 | 0.06 | 39.02 | 31.93 |
| X_N_35_20 | 950 | 0.01 | 950 | 2.31 | 0.06 | 40.23 | 32.55 |
| X_N_12_26 | 430 | 0.04 | 920 | 19.43 | 0.17 | 40.66 | 33.00 |
| X_N_4_48 | 260 | 0.03 | 50 | 16.28 | 0.01 | 36.87 | 30.47 |
| X_N_102_35 | 400 | 0.06 | 190 | 87.51 | 0.11 | 39.09 | 32.11 |
| X_N_115_23 | 70 | 0.04 | 140 | 38.84 | 0.05 | 38.51 | 31.66 |
| cid_166 | 780 | 0.06 | 850 | 109.30 | 0.52 | 41.07 | 33.45 |
| cid_1605 | −120 | 0.02 | −120 | 12.64 | 0.03 | 38.07 | 31.29 |
| cid_346 | 2230 | 0.05 | 2230 | 28.72 | 0.50 | 41.89 | 33.85 |
| cid_1205 | −250 | 0.002 | −250 | 0.14 | 0.005 | 37.98 | 30.88 |
| cid_467 | 210 | 0.05 | 280 | 51.23 | 0.11 | 39.42 | 32.28 |
| J1333+1649 | 2160 | 0.15 | 2300 | 285.46 | 1.56 | 42.42 | 34.36 |
| J1441+0454 | 3320 | 0.11 | 4690 | 189.15 | 2.85 | 43.29 | 34.93 |
| S82X1905 | 1070 | 0.04 | 1070 | 27.36 | 0.30 | 41.03 | 33.30 |
| S82X1940 | 430 | 0.02 | 430 | 16.40 | 0.11 | 39.81 | 32.47 |
| S82X2058 | 680 | 0.05 | 740 | 25.86 | 0.16 | 40.44 | 32.87 |
Notes. Columns give the following information: (1) target identification, (2) the velocity at the peak of the CIV total profile, (3) CIV BLR radius derived from the CIV radius-luminosity relation from Lira et al. (2018), (4) velocity of the CIV at 50% of the cumulative line flux, (5) mass of the outflow (M⊙), (6) mass outflow rate assuming a thin-shell geometry as described in Sect. 5.2, (7) kinetic power of the outflow and (8) outflow momentum load.
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