QSOFEED: Relationship between star formation and active galactic nuclei feedback

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Table A.3.

Results of the non-parametric analysis of the gas kinematics using the [OIII] emission line.

Name	W80	ΔV	V05	V95	log n_e	log M_of	Ṁ_of	log Ė_of
	(km s⁻¹)	(km s⁻¹)	(km s⁻¹)	(km s⁻¹)	(cm⁻³)	(M_⊙)	(M_⊙ yr⁻¹)	(erg s⁻¹)
J0052-01	767 ± 3	−91 ± 3	−584 ± 5	401 ± 3	( < 2.94)	5.530 ± 0.002	$0 . 7_{- . 5}^{+ 2.3}$ $0.7^{+2.3}_{-.5}$	40.8
J0232-08	854 ± 2	−142 ± 1	−681 ± 2	398 ± 1	$3 . 43_{- 0.12}^{+ 0.03}$ $3.43^{+0.03}_{-0.12}$	5.109 ± 0.001	$0 . 3_{- 0.2}^{+ 0.9}$ $0.3^{+0.9}_{-0.2}$	40.5
J0731+39	699 ± 6	−82 ± 4	−611 ± 6	447 ± 9	$3 . 97_{- 0.05}^{+ 0.06}$ $3.97^{+0.06}_{-0.05}$	4.38 ± 0.01	$0 . 1_{- 0.0}^{+ 0.2}$ $0.1^{+0.2}_{-0.0}$	39.9
J0759+50	1361 ± 4	6 ± 6	−953 ± 7	965 ± 6	$4 . 09_{- 0.03}^{+ 0.03}$ $4.09^{+0.03}_{-0.03}$	4.52 ± 0.02	$0 . 2_{- 0.1}^{+ 0.6}$ $0.2^{+0.6}_{-0.1}$	40.9
J0802+25	1028 ± 6	−255 ± 3	−967 ± 5	456 ± 5	$3 . 56_{- 0.14}^{+ 0.12}$ $3.56^{+0.12}_{-0.14}$	5.04 ± 0.03	$0 . 4_{- 0.3}^{+ 1.3}$ $0.4^{+1.3}_{- 0.3 }$	41.0
J0802+46	893 ± 4	15 ± 3	−615 ± 4	645 ± 3	$3 . 88_{- 0.05}^{+ 0.04}$ $3.88^{+0.04}_{-0.05}$	4.575 ± 0.001	$0 . 1_{- 0.1}^{+ 0.4}$ $0.1^{+ 0.4}_{- 0.1 }$	40.3
J0805+28	938 ± 180	−140 ± 241	−776 ± 121	496 ± 362	$3 . 59_{- 0.16}^{+ 0.08}$ $3.59^{+0.08}_{-0.16}$	4.84 ± 0.71	$0 . 2_{- 0.1}^{+ 0.7}$ $0.2^{+ 0.7}_{- 0.1 }$	40.6
J0818+36	545 ± 2	−53 ± 2	−436 ± 3	329 ± 1	$3 . 67_{- 0.1}^{+ 0.06}$ $3.67^{+0.06}_{-0.1}$	4.749 ± 0.001	$0 . 1_{- 0.1}^{+ 0.3}$ $0.1^{+ 0.3}_{- 0.1 }$	39.7
J0841+01	423 ± 1	−18 ± 1	−297 ± 1	262 ± 1	$2 . 32_{- 0.13}^{+ 0.24}$ $2.32^{+0.24}_{-0.13}$	…	…	…
J0858+31	735 ± 8	−102 ± 6	−636 ± 11	433 ± 10	$(2 . 71_{- 0.12}^{+ 0.1})$ $(2.71^{+0.1}_{-0.12})$	5.54 ± 0.03	$1 . 1_{- 0.7}^{+ 3.3}$ $1.1^{+ 3.3}_{- 0.7 }$	41.2
J0915+30	795 ± 8	74 ± 8	−535 ± 5	683 ± 15	$3 . 41_{- 0.06}^{+ 0.05}$ $3.41^{+0.05}_{-0.06}$	5.10 ± 0.02	$0 . 5_{- 0.3}^{+ 1.5}$ $0.5^{+ 1.5}_{- 0.3 }$	40.9
J0939+35	563 ± 2	−53 ± 1	−426 ± 2	321 ± 2	$3 . 16_{- 0.11}^{+ 0.05}$ $3.16^{+0.05}_{-0.11}$	...	…	...
J0945+17	1079 ± 6	−132 ± 8	−1005 ± 9	742 ± 14	$3 . 39_{- 0.1}^{+ 0.08}$ $3.39^{+0.08}_{-0.1}$	5.46 ± 0.01	$1 . 5_{- 1.0}^{+ 4.9}$ $1.5^{+ 4.9}_{- 1.0 }$	41.8
J1010+06	1490 ± 53	51 ± 31	−1073 ± 87	1176 ± 37	$4 . 58_{- 0.03}^{+ 0.03}$ $4.58^{+0.03}_{-0.03}$	3.75 ± 0.04	$0 . 04_{- 0.03}^{+ 0.12}$ $0.04 ^{ + 0.12}_{- 0.03 }$	40.4
J1015+00	531 ± 3	−38 ± 2	−393 ± 3	318 ± 3	$3 . 16_{- 0.18}^{+ 0.06}$ $3.16^{+0.06}_{-0.18}$	5.396 ± 0.003	$0 . 4_{- 0.3}^{+ 1.3}$ $0.4^{+ 1.3}_{- 0.3 }$	40.2
J1016+00	636 ± 6	−81 ± 3	−515 ± 5	354 ± 4	( < 2.67)	5.813 ± 0.004	$1 . 3_{- 0.9}^{+ 4.1}$ $1.3^{+ 4.1}_{- 0.9 }$	40.9
J1034+60	763 ± 2	8 ± 2	−546 ± 3	562 ± 3	$2 . 99_{- 0.2}^{+ 0.19}$ $2.99^{+0.19}_{-0.2}$	5.586 ± 0.001	$1 . 3_{- 0.9}^{+ 4.2}$ $1.3^{+ 4.2}_{- 0.9 }$	41.3
J1036+01	482 ± 3	−44 ± 2	−362 ± 4	273 ± 3	$3 . 28_{- 0.18}^{+ 0.06}$ $3.28^{+0.06}_{-0.18}$	…	…	…
J1100+08	1162 ± 7	−43 ± 7	−952 ± 13	865 ± 8	$3 . 99_{- 0.08}^{+ 0.07}$ $3.99^{+0.07}_{-0.08}$	4.92 ± 0.01	$0 . 5_{- 0.3}^{+ 1.5}$ $0.5^{+ 1.5}_{- 0.3 }$	41.3
J1137+61	529 ± 64	2 ± 10	−327 ± 31	331 ± 51	$3 . 26_{- 0}^{+ 0.07}$ $3.26^{+0.07}_{-0}$	...	…	...
J1152+10	553 ± 1	−39 ± 1	−382 ± 1	305 ± 1	$3 . 39_{- 0.13}^{+ 0.02}$ $3.39^{+0.02}_{-0.13}$	5.244 ± 0.001	$0 . 2_{- 0.2}^{+ 0.8}$ $0.2^{+ 0.8}_{- 0.2 }$	39.9
J1157+37	660 ± 6	−79 ± 4	−577 ± 8	419 ± 7	$3 . 67_{- 0.07}^{+ 0.06}$ $3.67^{+0.06}_{-0.07}$	4.72 ± 0.01	$0 . 1_{- 0.1}^{+ 0.5}$ $0.1^{+ 0.5}_{- 0.1 }$	40.2
J1200+31	766 ± 4	−146 ± 2	−695 ± 3	402 ± 4	$3 . 42_{- 0.06}^{+ 0.08}$ $3.42^{+0.08}_{-0.06}$	5.564 ± 0.001	$1 . 1_{- 0.7}^{+ 3.4}$ $1.1^{+ 3.4}_{- 0.7 }$	41.2
J1218+47	444 ± 2	−21 ± 1	−319 ± 2	277 ± 2	3.66^a	4.83 ± 0.03	$0 . 1_{- 0.1}^{+ 0.3}$ $0.1^{+ 0.3}_{-0.1 }$	39.3
J1223+08	594 ± 7	−132 ± 4	−580 ± 10	315 ± 6	$3 . 7_{- 0.13}^{+ 0.08}$ $3.7^{+0.08}_{-0.13}$	4.90 ± 0.02	$0 . 2_{- 0.1}^{+ 0.5}$ $0.2^{+ 0.5}_{- 0.1 }$	40.2
J1238+09	641 ± 2	−49 ± 1	−438 ± 2	341 ± 2	$(2 . 68_{- 0.09}^{+ 0.09})$ $(2.68^{+0.09}_{-0.09})$	5.763 ± 0.001	$1 . 0_{- 0.6}^{+ 3.0}$ $1.0^{+ 3.0}_{- 0.6 }$	40.6
J1241+61	616 ± 7	−192 ± 5	−615 ± 9	231 ± 6	$2 . 95_{- 0.46}^{+ 0.12}$ $2.95^{+0.12}_{-0.46}$	5.38 ± 0.02	$0 . 4_{- 0.3}^{+ 1.4}$ $0.4^{+ 1.4}_{- 0.3 }$	40.6
J1244+65	1218 ± 6	−282 ± 6	−1149 ± 9	585 ± 9	$3 . 31_{- 0.22}^{+ 0.05}$ $3.31^{+0.05}_{-0.22}$	4.94 ± 0.02	$0 . 4_{- 0.3}^{+ 1.3}$ $0.4^{+ 1.3}_{- 0.3 }$	41.2
J1300+54	298 ± 1	−27 ± 0	−229 ± 1	175 ± 1	$3 . 33_{- 0.4}^{+ 0.1}$ $3.33^{+0.1}_{-0.4}$	…	…	…
J1316+44	905 ± 15	−220 ± 18	−872 ± 37	432 ± 3	3.66^a	4.84 ± 0.01	$0 . 2_{- 0.1}^{+ 0.6}$ $0.2^{+ 0.6}_{- 0.1 }$	40.6
J1347+12	2519 ± 150	−845 ± 337	−2466 ± 483	775 ± 192	$4 . 27_{- 0.05}^{+ 0.08}$ $4.27^{+0.08}_{-0.05}$	4.21 ± 0.24	$0 . 1_{- 0.1}^{+ 0.4}$ $0.1^{+ 0.4}_{- 0.1 }$	41.4
J1356-02	717 ± 8	−85 ± 7	−654 ± 11	483 ± 13	$3 . 66_{- 0.20}^{+ 0.09}$ $3.66^{+0.09}_{-0.20}$	4.64 ± 0.02	$0 . 1_{- 0.1}^{+ 0.5}$ $0.1^{+ 0.5}_{- 0.1 }$	40.4
J1356+10	861 ± 2	26 ± 1	−535 ± 2	586 ± 2	$3 . 21_{- 0.15}^{+ 0.0}$ $3.21^{+0.0}_{-0.15}$	5.794 ± 0.002	$1 . 9_{- 1.2}^{+ 5.9}$ $1.9^{+5.9}_{- 1.2 }$	41.3
J1405+40	650 ± 5	−124 ± 4	−606 ± 8	358 ± 2	$4 . 1_{- 0.19}^{+ 0.15}$ $4.1^{+0.15}_{-0.19}$	4.476 ± 0.003	$0 . 1_{- 0.0}^{+ 0.2}$ $0.1^{+ 0.2}_{- 0.0 }$	39.8
J1430+13	803 ± 3	−61 ± 2	−630 ± 4	509 ± 2	$3 . 24_{- 0.3}^{+ 0.05}$ $3.24^{+0.05}_{-0.3}$	5.646 ± 0.004	$1 . 3_{- 0.9}^{+ 4.1}$ $1.3^{+ 4.1}_{- 0.9 }$	41.2
J1436+13	627 ± 4	−66 ± 3	−530 ± 4	397 ± 5	$3 . 4_{- 0.17}^{+ 0.08}$ $3.4^{+0.08}_{-0.17}$	5.068 ± 0.001	$0 . 3_{- 0.2}^{+ 0.9}$ $0.3^{+ 0.9}_{- 0.2 }$	40.4
J1437+30	628 ± 2	−24 ± 1	−457 ± 2	409 ± 3	$3 . 3_{- 0.13}^{+ 0.01}$ $3.3^{+0.01}_{-0.13}$	5.301 ± 0.001	$0 . 4_{- 0.3}^{+ 1.4}$ $0.4^{+ 1.4}_{- 0.3 }$	40.5
J1440+53	775 ± 3	−2 ± 3	−667 ± 5	664 ± 2	$3 . 92_{- 0.08}^{+ 0.09}$ $3.92^{+0.09}_{-0.08}$	4.71 ± 0.01	$0 . 2_{- 0.1}^{+ 0.7}$ $0.2^{+ 0.7}_{- 0.1 }$	40.7
J1455+32	845 ± 4	−36 ± 3	−626 ± 4	555 ± 4	$3 . 88_{- 0.06}^{+ 0.05}$ $3.88^{+0.05}_{-0.06}$	4.507 ± 0.002	$0 . 1_{- 0.1}^{+ 0.3}$ $0.1^{+ 0.3}_{- 0.1 }$	40.2
J1509+04	1356 ± 9	−327 ± 7	−1233 ± 10	579 ± 9	$3 . 41_{- 0.21}^{+ 0.11}$ $3.41^{+0.11}_{-0.21}$	4.94 ± 0.03	$0 . 4_{- 0.3}^{+ 1.3}$ $0.4^{+ 1.3}_{- 0.3 }$	41.3
J1517+33	1210 ± 4	−79 ± 2	−823 ± 2	666 ± 3	$2 . 98_{- 0.31}^{+ 0.23}$ $2.98^{+0.23}_{-0.31}$	5.67 ± 0.02	$1 . 8_{- 1.2}^{+ 5.6}$ $1.8^{+ 5.6}_{- 1.2 }$	41.5
J1533+35	538 ± 6	−38 ± 7	−467 ± 15	391 ± 6	$(2 . 44_{- 0.13}^{+ 0.11})$ $(2.44^{+0.11}_{-0.13})$	5.88 ± 0.04	$1 . 6_{- 1.1}^{+ 5.1}$ $1.6^{+ 5.1}_{- 1.1 }$	41.0
J1548-01	497 ± 2	−59 ± 2	−415 ± 4	298 ± 5	$(2 . 74_{- 0.05}^{+ 0.04})$ $(2.74^{+0.04}_{-0.05})$	…	…	…
J1558+35	561 ± 3	−125 ± 2	−533 ± 5	282 ± 3	$3 . 23_{- 0.26}^{+ 0.12}$ $3.23^{+0.12}_{-0.26}$	5.358 ± 0.002	$0 . 5_{- 0.3}^{+ 1.4}$ $0.5^{+ 1.4}_{- 0.3 }$	40.6
J1624+33	490 ± 4	−73 ± 2	−428 ± 4	282 ± 4	$3 . 63_{- 0.09}^{+ 0.12}$ $3.63^{+0.12}_{-0.09}$	4.77 ± 0.01	$0 . 1_{- 0.1}^{+ 0.3}$ $0.1^{+ 0.3}_{- 0.1 }$	39.7
J1653+23	494 ± 2	−57 ± 1	−403 ± 2	289 ± 1	$3 . 26_{- 0.04}^{+ 0.14}$ $3.26^{+0.14}_{-0.04}$	…	…	…
J1713+57	1491 ± 10	−60 ± 10	−1121 ± 18	1001 ± 7	$4 . 06_{- 0.06}^{+ 0.05}$ $4.06^{+0.05}_{-0.06}$	4.64 ± 0.01	$0 . 3_{- 0.2}^{+ 0.9}$ $0.3^{+0.9}_{-0.2}$	41.2
J2154+11	582 ± 206	−50 ± 135	−452 ± 252	353 ± 17	$3 . 27_{- 0.05}^{+ 0.16}$ $3.27^{+0.16}_{-0.05}$	5.06 ± 0.54	$0 . 3_{- 0.2}^{+ 0.8}$ $0.3^{+0.8}_{-0.2}$	40.2

Notes. Column 1 is the abbreviated name of the QSO2, columns 2 and 3 give the derived quantities W80 and ΔV whilst columns 4 and 5 give V05 and V95. All quantities are given in km s⁻¹. Column 6 lists the electron densities measured using either the transauroral technique or the [SII] ratios (between parenthesis). For the two objects where it was not possible to measure the densities, the assumed value of log n_e = 3.66 is given and denoted by an a. Columns 7, 8, and 9 show the total outflow mass, mass outflow rate and the kinetic energy, assuming an outflow radius of 0.62 kpc. The errors given for mass outflow rates are obtained from deriving the outflow rates at the minimum (0.15 kpc) and maximum (1.89 kpc) outflow radii found by Fischer et al. (2018), whilst 0.62 kpc is the mean of the values presented there. Errors for the values of log Ė_of are +0.6, −0.5.

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