2013A&A...549A..43H


Query : 2013A&A...549A..43H

2013A&A...549A..43H - Astronomy and Astrophysics, volume 549A43-43 (2013/1-1)

The properties of the extended warm ionised gas around low-redshift QSOs and the lack of extended high-velocity outflows.

HUSEMANN B., WISOTZKI L., SANCHEZ S.F. and JAHNKE K.

Abstract (from CDS):

We present a detailed analysis of a large sample of 31 low-redshift, mostly radio-quiet type 1 quasi-stellar objects (QSOs) observed with integral field spectroscopy to study their extended emission-line regions (EELRs). We focus on the ionisation state of the gas, size and luminosity of extended narrow line regions (ENLRs), which corresponds to those parts of the EELR dominated by ionisation from the QSO, as well as the kinematics of the ionised gas. We detect EELRs around 19 of our 31 QSOs (61%) after deblending the unresolved QSO emission and the extended host galaxy light in the integral field data with a new dedicated algorithm. Based on standard emission-line diagnostics we identify 13 EELRs to be entirely ionised by the QSO radiation, 3 EELRs are composed of HII regions and 3 EELRs display signatures of both ionisation mechanisms at different locations. The typical size of the ENLR is ∼10kpc at a median nuclear [OIII] luminosity of log(L([OIII])/[erg/s])=42.7±0.15. We show that the ENLR sizes are least a factor of ∼2 larger than determined with the Hubble Space Telescope, but are consistent with those of recently reported type 2 QSOs at matching [OIII] luminosities. The ENLR of type 1 and type 2 QSOs therefore appear to follow the same size-luminosity relation. Furthermore, we show for the first time that the ENLR size is much better correlated with the QSO continuum luminosity than with the total/nuclear [OIII] luminosity. We show that ENLR luminosity and radio luminosity are correlated, and argue that radio jets even in radio-quiet QSOs are important for shaping the properties of the ENLR. Strikingly, the kinematics of the ionised gas is quiescent and likely gravitationally driven in the majority of cases and we find only 3 objects with radial gas velocities exceeding >400km/s in specific regions of the EELR that can be associate with radio jets. In general, these are significantly lower outflow velocities and detection rates compared to starburst galaxies or radio-loud QSOs. This represent a challenge for some theoretical feedback models in which luminous QSOs are expected to radiatively drive an outflow out to scales of the entire host galaxy.

Abstract Copyright: ∼

Journal keyword(s): galaxies: active - quasars: emission lines - galaxies: ISM

Simbad objects: 37

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Number of rows : 37
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 LEDA 1790 Sy1 00 29 13.7012449608 +13 16 03.947778264   15.70 15.41     ~ 474 0
2 Mrk 1502 Sy1 00 53 34.9331107632 +12 41 35.929269132   14.41 14.03     ~ 1242 1
3 LEDA 3237 Sy1 00 54 52.1183662680 +25 25 38.983241532     15.42     ~ 421 0
4 [OKM2018] SWIFT J0056.9+1472 Sy1 00 57 09.9306975096 +14 46 10.142054004   16.56 16.29     ~ 167 0
5 HE 0132-0441 QSO 01 32 00.0 -04 41 00           ~ 5 0
6 2MASS J01352702-0426354 Sy1 01 35 27.0343748784 -04 26 35.477967372   17.37 16.20 16.44   ~ 15 0
7 2MASS J01553002-0857040 Sy1 01 55 30.0252391488 -08 57 04.130375616   17.26 17.02 16.89   ~ 74 0
8 HE 0157-0406 QSO 01 57 00.0 -04 06 00           ~ 4 0
9 Mrk 1014 Sy1 01 59 50.2534701768 +00 23 40.864244784   16.08 15.87     ~ 606 0
10 US 1329 Sy1 08 36 58.9103509968 +44 26 02.269644252   16.04 15.77     ~ 78 1
11 US 995 Sy1 09 48 59.4746090952 +43 35 18.955277736   17.17 16.86     ~ 51 0
12 LB 10235 Sy1 11 31 09.247 +26 32 07.86   17.0 17.0     ~ 33 0
13 QSO B1217+023 BLL 12 20 11.8846520568 +02 03 42.223956876   16.15 15.97 15.6   ~ 338 2
14 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
15 2MASX J12302215+6621551 Sy1 12 30 22.1813597064 +66 21 54.583965828   16.99 16.76     ~ 30 1
16 2MASS J12305003+0115226 Sy1 12 30 50.0331165552 +01 15 22.598028288   14.44 14.42     ~ 102 0
17 RMB 207 Sy1 12 30 54.1170001080 +11 00 11.140418124   17.12 16.94     ~ 81 1
18 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
19 NAME Centaurus A BLL 13 25 27.61521044 -43 01 08.8050291   8.18 6.84 6.66   ~ 4774 3
20 SDSS J135646.10+102609.0 Sy2 13 56 46.106 +10 26 09.09   18.90 18.11     ~ 95 0
21 2MASS J14294306+4747262 Sy1 14 29 43.0739786592 +47 47 26.217623904   17.29 16.97     ~ 195 0
22 2MASS J14441467+0633067 Sy1 14 44 14.6653704312 +06 33 06.705031932   17.26 17.02     ~ 42 1
23 HE 1453-0303 QSO 14 56 -03.3           ~ 2 0
24 ICRF J154743.5+205216 Sy1 15 47 43.5376371336 +20 52 16.612810320   16.80 16.69 15.70   ~ 521 1
25 Ton 256 Sy1 16 14 13.2050129832 +26 04 16.221218880   16.06 16.50     ~ 282 1
26 LEDA 3096518 Sy1 16 55 51.3754270896 +21 46 01.800138324   16.76 16.43     ~ 37 0
27 IRAS 17002+5153 Sy1 17 01 24.8265469104 +51 49 20.447878836   15.49 15.12     ~ 401 0
28 Mrk 1513 Sy1 21 32 27.8162556672 +10 08 19.252365396   14.92 14.64     ~ 651 0
29 HE 2152-0936 QSO 21 55 -09.4           ~ 3 0
30 PHL 1811 Sy1 21 55 01.5124437432 -09 22 24.349496808   13.9 16.8 14.1   ~ 200 1
31 HE 2158-0107 QSO 21 58 00.0 -01 07 00           ~ 7 0
32 HE 2158+0115 QSO 22 01 +01.5           ~ 2 0
33 LEDA 140992 Sy1 22 01 29.6765724840 +01 29 56.440520376   16.4 16.4     ~ 16 0
34 Z 428-65 Sy1 22 17 12.2637639888 +14 14 20.917852980   15.02 14.66     ~ 371 0
35 HE 2307-0254 QSO 23 07 00.0 -02 54 00           ~ 4 0
36 4C -01.61 BLL 23 51 56.1224889360 -01 09 13.315371768   16.83 16.59     ~ 380 1
37 HE 2353-0420 QSO 23 53 00.0 -04 20 00           ~ 4 0

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