2018A&A...617A..81V


Query : 2018A&A...617A..81V

2018A&A...617A..81V - Astronomy and Astrophysics, volume 617A81-81 (2018/9-1)

The WISSH quasars project. IV. Broad line region versus kiloparsec-scale winds.

VIETRI G., PICONCELLI E., BISCHETTI M., DURAS F., MARTOCCHIA S., BONGIORNO A., MARCONI A., ZAPPACOSTA L., BISOGNI S., BRUNI G., BRUSA M., COMASTRI A., CRESCI G., FERUGLIO C., GIALLONGO E., LA FRANCA F., MAINIERI V., MANNUCCI F., RICCI F., SANI E., TESTA V., TOMBESI F., VIGNALI C. and FIORE F.

Abstract (from CDS):

Winds accelerated by active galactic nuclei (AGNs) are invoked in the most successful models of galaxy evolution to explain the observed physical and evolutionary properties of massive galaxies. Winds are expected to deposit energy and momentum into the interstellar medium (ISM), thus regulating both star formation and supermassive black hole (SMBH) growth. We undertook a multiband observing program aimed at obtaining a complete census of winds in a sample of WISE/SDSS selected hyper-luminous (WISSH) quasars (QSOs) at z~=2-4. We analyzed the rest-frame optical (i.e. LBT/LUCI and VLT/SINFONI) and UV (i.e. SDSS) spectra of 18 randomly selected WISSH QSOs to measure the SMBH mass and study the properties of winds both in the narrow line region (NLR) and broad line region (BLR) traced by blueshifted or skewed [OIII] and CIV emission lines, respectively. These WISSH QSOs are powered by SMBH with masses ≥109M☉ accreting at 0.4<λEdd<3.1. We found the existence of two subpopulations of hyper-luminous QSOs characterized by the presence of outflows at different distances from the SMBH. One population (i.e. [OIII] sources) exhibits powerful [OIII] outflows, a rest-frame equivalent width (REW) of the CIV emission REWCIV~=20-40Å, and modest CIV velocity shift (vCIVpeak) with respect to the systemic redshift (vCIVpeak≲2000km/s). The second population (i.e. Weak [OIII] sources), representing ∼70% of the analyzed WISSH QSOs, shows weak or absent [OIII] emission and an extremely large blueshifted CIV emission (vCIVpeak up to ∼8000km/s and REWCIV≲20Å). We propose two explanations for the observed behavior of the strength of the [OIII] emission in terms of the orientation effects of the line of sight and ionization cone. The dichotomy in the presence of BLR and NLR winds could be likely due to inclination effects considering a polar geometry scenario for the BLR winds. In a few cases these winds are remarkably as powerful as those revealed in the NLR in the [OIII] QSOs (Ekin∼1044–45erg/s). We also investigated the dependence of these CIV winds on fundamental AGN parameters such as bolometric luminosity (LBol), Eddington ratio (λEdd), and UV-to-X-ray continuum slope (αOX). We found a strong correlation with LBol and an anti-correlation with αOX whereby the higher the luminosity, the steeper the ionizing continuum described by means of αOX and the larger the blueshift of the CIV emission line. Finally, the observed dependence vCIVpeak∝LBol0.28±0.04 is consistent with a radiatively-driven-winds scenario, where a strong UV continuum is necessary to launch the wind and a weakness of the X-rayemission is fundamental to prevent overionization of the wind itself.

Abstract Copyright: © ESO 2018

Journal keyword(s): galaxies: active - galaxies: nuclei - quasars: emission lines - quasars: general - quasars: supermassive black holes - ISM: jets and outflows

Simbad objects: 22

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Number of rows : 22
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 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
2 QSO J0745+4734 QSO 07 45 21.7878198936 +47 34 36.191801820   16.76 16.44     ~ 103 0
3 QSO J0801+5210 QSO 08 01 17.7968016048 +52 10 34.598421012   17.41 17.04     ~ 67 0
4 QSO B0900+42 QSO 09 00 33.5091652824 +42 15 47.031009948   17.63 17.18     ~ 85 0
5 2MASS J09584122+2827291 QSO 09 58 41.2178328792 +28 27 29.568196188   19.02 18.44     ~ 24 0
6 QSO B1103+6416 QSO 11 06 10.7339248800 +64 00 09.644901192   16.36 16.16     ~ 76 0
7 QSO J1111+1336 QSO 11 11 19.1031731280 +13 36 03.822328512   18.59 17.96     ~ 47 0
8 IRAS 11119+3257 Sy1 11 14 38.8902542640 +32 41 33.483258276   19.22 17.96     ~ 165 0
9 2MASS J11574799+2724595 QSO 11 57 47.9892554664 +27 24 59.656490100   19.70 18.99     ~ 21 0
10 QSO J1201+0116 QSO 12 01 44.3649782736 +01 16 11.740001304   18.09 17.74 17.4   ~ 66 2
11 QSO B1159+123 QSO 12 01 47.9118521640 +12 06 30.253926276   18.85 18.16     ~ 108 0
12 [VV2006] J123641.5+655441 QSO 12 36 41.4592914600 +65 54 42.183138852   18.21 17.72     ~ 39 0
13 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
14 [VV2006] J132655.0-000531 QSO 13 26 54.9527826240 -00 05 30.134926968   21.22 20.81     ~ 37 0
15 [VV2006] J142124.0+463318 QSO 14 21 23.9850678432 +46 33 17.955577764   18.53 17.99     ~ 47 0
16 [VV2006] J142243.0+441721 QSO 14 22 43.0262924160 +44 17 21.323456196   19.96 19.08     ~ 39 0
17 QSO J1521+5202 QSO 15 21 56.4821480376 +52 02 38.598049752   16.02 15.70     ~ 64 0
18 QSO J1538+0855 QSO 15 38 30.5596599072 +08 55 17.150004552   18.77 17.98     ~ 39 0
19 2MASS J15493872+1245092 QSO 15 49 38.7147322320 +12 45 09.161026308   19.21 18.54 17.61   ~ 40 0
20 SDSS J212329.46-005052.9 QSO 21 23 29.4639412848 -00 50 52.916363736   16.91 16.62     ~ 131 0
21 PHL 1811 Sy1 21 55 01.5124437432 -09 22 24.349496808   13.9 16.8 14.1   ~ 200 1
22 QSO J2346-0016 QSO 23 46 25.6709113344 -00 16 00.427438668   19.44 18.73     ~ 63 0

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