2020A&A...644A.175V


Query : 2020A&A...644A.175V

2020A&A...644A.175V - Astronomy and Astrophysics, volume 644A175-175 (2020/12-1)

SUPER. III. Broad line region properties of AGNs at z ∼ 2.

VIETRI G., MAINIERI V., KAKKAD D., NETZER H., PERNA M., CIRCOSTA C., HARRISON C.M., ZAPPACOSTA L., HUSEMANN B., PADOVANI P., BISCHETTI M., BONGIORNO A., BRUSA M., CARNIANI S., CICONE C., COMASTRI A., CRESCI G., FERUGLIO C., FIORE F., LANZUISI G., MANNUCCI F., MARCONI A., PICONCELLI E., PUGLISI A., SALVATO M., SCHRAMM M., SCHULZE A., SCHOLTZ J., VIGNALI C. and ZAMORANI G.

Abstract (from CDS):


Aims. The SINFONI survey for Unveiling the Physics and Effect of Radiative feedback (SUPER) was designed to conduct a blind search for AGN-driven outflows on X-ray-selected AGNs at redshift z∼2 with high (∼2kpc) spatial resolution, and to correlate them with the properties of their host galaxy and central black hole. The main aims of this paper are: (a) to derive reliable estimates for the masses of the black holes and accretion rates for the Type-1 AGNs in this survey; and (b) to characterise the properties of the AGN-driven winds in the broad line region (BLR).
Methods. We analysed rest-frame optical and UV spectra of 21 Type-1 AGNs. We used Hα, Hβ, and MgII line profiles to estimate the masses of the black holes. We used the blueshift of the CIV line profile to trace the presence of winds in the BLR.
Results. We find that the Hα and Hβ line widths are strongly correlated, as is the line continuum luminosity at 5100 Å with Hα line luminosity, resulting in a well-defined correlation between black hole masses estimated from Hα and Hβ. Using these lines, we estimate that the black hole masses for our objects are in the range Log (MBH/M☉)=8.4-10.8 and are accreting at λEdd=0.04-1.3. Furthermore, we confirm the well-known finding that the CIV line width does not correlate with the Balmer lines and the peak of the line profile is blueshifted with respect to the [OIII]-based systemic redshift. These findings support the idea that the CIV line is tracing outflowing gas in the BLR for which we estimated velocities up to ∼4700km/s. We confirm the strong dependence of the BLR wind velocity on the UV-to-X-ray continuum slope, the bolometric luminosity, and Eddington ratio. We infer BLR mass outflow rates in the range 0.005-3M☉/yr, revealing a correlation with the bolometric luminosity consistent with that observed for ionised winds in the narrow line region (NLR), and X-ray winds detected in local AGNs, and kinetic power ∼10–7-10–4xLBol. The coupling efficiencies predicted by AGN-feedback models are much higher than the values reported for the BLR winds in the SUPER sample; although it should be noted that only a fraction of the energy injected by the AGN into the surrounding medium is expected to become kinetic power in the outflow. Finally, we find an anti-correlation between the equivalent width of the [OIII] line and the CIV velocity shift, and a positive correlation between this latter parameter and [OIII] outflow velocity. These findings, for the first time in an unbiased sample of AGNs at z∼2, support a scenario where BLR winds are connected to galaxy-scale detected outflows, and are therefore capable of affecting the gas in the NLR located at kiloparsec scale distances.

Abstract Copyright: © ESO 2020

Journal keyword(s): galaxies: active - galaxies: evolution - galaxies: high-redshift - quasars: emission lines - quasars: supermassive black holes

Simbad objects: 21

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Number of rows : 21
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 SDSS J020453.80-060407.8 QSO 02 04 53.8108216680 -06 04 07.728794400           ~ 15 0
2 SDSS J021730.94-041823.6 QSO 02 17 30.9413116800 -04 18 23.637636468           ~ 22 0
3 SDSS J022029.84-025623.4 QSO 02 20 29.8381796976 -02 56 23.397525996           ~ 21 0
4 SDSS J022233.64-054902.7 QSO 02 22 33.6387148008 -05 49 02.720863740           ~ 10 0
5 SDSS J022402.71-051130.8 QSO 02 24 02.717 -05 11 30.81           ~ 15 0
6 SDSS J022550.09-030641.1 QSO 02 25 50.0975224512 -03 06 41.082259716           ~ 18 0
7 SDSS J022701.46-040506.7 QSO 02 27 01.461 -04 05 06.73           ~ 14 0
8 SDSS J022744.63-034205.4 QSO 02 27 44.6365954752 -03 42 05.445261756           ~ 15 0
9 SDSS J022905.93-040242.9 QSO 02 29 05.9387821856 -04 02 42.973458982           ~ 20 1
10 SDSS J023005.65-050814.1 QSO 02 30 05.6629942944 -05 08 14.035728696           ~ 17 0
11 [VV2006] J095858.7+020138 QSO 09 58 58.6825359312 +02 01 39.052405992   19.0139 18.6273   18.713 ~ 75 0
12 SDSS J095919.82+024238.6 QSO 09 59 19.8252374448 +02 42 38.614294800   21.278 21.399   20.935 ~ 42 0
13 SDSS J095943.41+020707.4 QSO 09 59 43.4136711744 +02 07 07.362946992   19.831 19.650   19.472 ~ 44 0
14 ACS-GC 20123811 AGN 10 00 02.57 +02 19 58.8 25.29 25.28 24.83 24.54 24.04 ~ 33 0
15 [VV2006] J100024.5+020619 QSO 10 00 24.4802452008 +02 06 19.669651812   19.43 19.42   19.89 ~ 64 0
16 QSO B1331+170 Bla 13 33 35.7827544072 +16 49 04.013500728   16.84 16.71 16.41   ~ 469 1
17 [VV2006] J144105.5+045454 QSO 14 41 05.5359788928 +04 54 54.963994464   17.77 17.47     ~ 34 0
18 2MASS J15493872+1245092 QSO 15 49 38.7147322320 +12 45 09.161026308   19.21 18.54 17.61   ~ 40 0
19 SDSS J232856.34-003011.7 QSO 23 28 56.3524318488 -00 30 11.773526688   19.81 19.59     ~ 25 0
20 SDSS J232940.28-001751.7 QSO 23 29 40.2903384600 -00 17 51.706312008   21.33 21.18     ~ 15 0
21 SDSS J233158.61-005410.4 QSO 23 31 58.6211300784 -00 54 10.408413888   20.28 20.09     ~ 26 0

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