2013MNRAS.432..138R


Query : 2013MNRAS.432..138R

2013MNRAS.432..138R - Mon. Not. R. Astron. Soc., 432, 138-166 (2013/June-2)

The importance of warm, AGN-driven outflows in the nuclear regions of nearby ULIRGs.

RODRIGUEZ ZAURIN J., TADHUNTER C.N., ROSE M. and HOLT J.

Abstract (from CDS):

We present an optical spectroscopic study of a 90percent complete sample of nearby ULIRGs (z < 0.175) with optical Seyfert nuclei, with the aim of investigating the nature of the near-nuclear (r ≲ 3.5 kpc) warm gas outflows. A high proportion (94percent) of our sample show disturbed emission line kinematics in the form of broad (FWHM > 500 km s-1) and/or strongly blueshifted (ΔV < -150 km s-1) emission line components. This proportion is significantly higher than found in a comparison sample of nearby ultraluminous infrared galaxies (ULIRGs) that lack optical Seyfert nuclei (19percent). We also find evidence that the emission line kinematics of the Sy-ULIRGs are more highly disturbed than those of samples of non-ULIRG Seyferts and Palomar-Green quasars in the sense that, on average, their [Oiii] λλ5007, 4959 emission lines are broader and more asymmetric.

The Sy-ULIRG sample encompasses a wide diversity of emission line profiles. In most individual objects, we are able to fit the profiles of all the emission lines of different ionization with a kinematic model derived from the strong [Oiii] λλ4959, 5007 lines, using between two and five Gaussian components. From these fits, we derive diagnostic line ratios that are used to investigate the ionization mechanisms for the different kinematic components. We show that, in general, the line ratios are consistent with gas of supersolar abundance photoionized by a combination of AGN and starburst activity, with an increasing contribution from the AGN with increasing FWHM of the individual kinematic components, and the AGN contribution dominating for the broadest components. However, shock ionization cannot be ruled out in some cases. Our derived upper limits on the mass outflows rates and kinetic powers of the emission line outflows show that they can be as energetically significant as the neutral and molecular outflows in ULIRGs - consistent with the requirements of the hydrodynamic simulations that include AGN feedback. However, the uncertainties are large, and more accurate estimates of the radii, densities and reddening of the outflows are required to put these results on a firmer footing.


Abstract Copyright: © 2013 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2013)

Journal keyword(s): ISM: jets and outflows - ISM: kinematics and dynamics - galaxies: active - galaxies: evolution - galaxies: interactions - galaxies: Seyfert

Simbad objects: 25

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Number of rows : 25
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 2MASX J00212652-0839261 LIN 00 21 26.5135306416 -08 39 25.967117268   18.37       ~ 124 1
2 IRAS 01003-2238 Sy2 01 02 49.9920152640 -22 21 57.262136544   18.62 18.9 17.83   ~ 192 0
3 LEDA 90164 Sy2 12 09 45.1187842872 -05 01 13.431047484   17.52 17.8 16.56   ~ 114 1
4 IRAS 12112+0305 PaG 12 13 45.98880 +02 48 39.9600           ~ 373 0
5 [CGM90] IRAS 12112+0305 NE rG 12 13 46.10735 +02 48 41.4959           ~ 369 0
6 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
7 Z 294-4 Sy1 12 56 14.2341182928 +56 52 25.238373852   14.68 13.84     ~ 2096 3
8 IRAS 13305-1739 Sy1 13 33 16.5631735944 -17 55 10.612057080   20.0 18.6     ~ 47 1
9 Z 271-60 Sy2 13 44 42.1883001099 +55 53 13.596220922   15.68 14.91     ~ 958 3
10 IRAS 13443+0802 PaG 13 46 51.07533 +07 47 18.4520           ~ 39 0
11 2MASS J13465108+0747190 GiP 13 46 51.08906 +07 47 19.0032           ~ 37 0
12 PKS 1345+12 Sy2 13 47 33.36161873 +12 17 24.2398927   19.28 18.44 15.718   ~ 652 2
13 IRAS 14121-0126 LIN 14 14 45.5286962688 -01 40 54.809983452   18.006   17.772   ~ 40 0
14 SBSG 1439+535 Sy2 14 41 04.3772323224 +53 20 08.658129120   18.29 17.77     ~ 81 0
15 2MASX J15155520-2009172 Sy2 15 15 55.1783451792 -20 09 16.916691024   18.34 17.1 17.16   ~ 55 0
16 LEDA 90222 Sy1 15 48 56.8020209304 -04 59 33.598051584   16.4 16.40 16.85   ~ 106 0
17 QSO B1549-790 Bla 15 56 58.86979525 -79 14 04.2817241   18.80 18.800 17.84   ~ 221 1
18 2MASS J16180935+0139216 AGN 16 18 09.35520 +01 39 21.6828           ~ 10 0
19 LEDA 165716 LIN 17 04 28.4433405168 +67 16 28.258598748     17.0     ~ 59 0
20 2MASX J17185436+5441486 Sy2 17 18 54.4002 +54 41 48.289           ~ 84 1
21 LEDA 66703 Sy1 21 24 41.6403183696 -17 44 45.886080696   17.18 16.50 15.95   ~ 96 0
22 IRAS 23060+0505 Sy1 23 08 33.9537309816 +05 21 29.751752412           ~ 160 0
23 IRAS 23233+2817 Sy2 23 25 49.4068081702 +28 34 21.273807553           ~ 41 1
24 2MASS J23351192+2930002 LIN 23 35 11.92032 +29 30 00.2124           ~ 56 0
25 [KVS2002] IRAS 23389+0300 N GiP 23 41 30.30 +03 17 26.2           ~ 5 0

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