2011ApJ...735...48S


Query : 2011ApJ...735...48S

2011ApJ...735...48S - Astrophys. J., 735, 48 (2011/July-1)

Type 2 active galactic nuclei with double-peaked [O III] lines. II. Single AGNs with complex narrow-line region kinematics are more common than binary AGNs.

SHEN Y., LIU X., GREENE J.E. and STRAUSS M.A.

Abstract (from CDS):

Approximately 1% of low-redshift (z ≲ 0.3) optically selected type 2 active galactic nuclei (AGNs) show a double-peaked [O III] narrow emission line profile in their spatially integrated spectra. Such features are usually interpreted as either due to kinematics, such as biconical outflows and/or disk rotation of the narrow line region (NLR) around single black holes, or due to the relative motion of two distinct NLRs in a merging pair of AGNs. Here, we report follow-up near-infrared (NIR) imaging and optical slit spectroscopy of 31 double-peaked [O III] type 2 AGNs drawn from the Sloan Digital Sky Survey (SDSS) parent sample presented in Liu et al. The NIR imaging traces the old stellar population in each galaxy, while the optical slit spectroscopy traces the NLR gas. These data reveal a mixture of origins for the double-peaked feature. Roughly 10% of our objects are best explained by binary AGNs at (projected) kpc-scale separations, where two stellar components with spatially coincident NLRs are seen. ∼50% of our objects have [O III] emission offset by a few kpc, corresponding to the two velocity components seen in the SDSS spectra, but there are no spatially coincident double stellar components seen in the NIR imaging. For those objects with sufficiently high-quality slit spectra, we see velocity and/or velocity dispersion gradients in [O III] emission, suggestive of the kinematic signatures of a single NLR. The remaining ∼40% of our objects are ambiguous and will need higher spatial resolution observations to distinguish between the two scenarios. Our observations therefore favor the kinematics scenario with a single AGN for the majority of these double-peaked [O III] type 2 AGNs. We emphasize the importance of combining imaging and slit spectroscopy in identifying kpc-scale binary AGNs, i.e., in no cases does one of these alone allow an unambiguous identification. We estimate that ∼0.5%-2.5% of the z ≲ 0.3 type 2 AGNs are kpc-scale binary AGNs of comparable luminosities, with a relative orbital velocity ≳ 150 km/s.

Abstract Copyright: ∼

Journal keyword(s): black hole physics - galaxies: active - galaxies: interactions - galaxies: nuclei - galaxies: Seyfert - quasars: general

Simbad objects: 38

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Number of rows : 38
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 2MASS J00024907+0045051 Sy1 00 02 49.0771278648 +00 45 04.933132632   19.05 18.23     ~ 29 0
2 LEDA 3099131 Sy2 00 09 11.6026757880 -00 36 54.780123708 18 19.09 18.27 15.92   ~ 52 1
3 2MASS J01165957-1025392 AGN 01 16 59.5874406000 -10 25 39.124455528           ~ 5 0
4 2MASS J01354691-0058584 AGN 01 35 46.9352965728 -00 58 58.484591688           ~ 5 0
5 LEDA 1461975 Sy2 01 35 55.8263420472 +14 35 29.635003716   18.51 17.88     ~ 14 0
6 2MASX J01560516-0007219 Sy2 01 56 05.1412176504 -00 07 21.775066824   18.64 17.84     ~ 16 0
7 M 77 Sy2 02 42 40.7091669408 -00 00 47.859690204 9.70 9.61 8.87 10.1 9.9 ~ 4897 2
8 2MASX J04000160-0652543 Sy2 04 00 01.5920782560 -06 52 54.307469064   19.37 18.44     ~ 19 0
9 Mrk 78 Sy2 07 42 41.7033384240 +65 10 37.447730076   15.57 14.58     ~ 386 3
10 2MASS J08371348+1500371 AGN 08 37 13.49 +15 00 37.1           ~ 9 0
11 2MASS J08512194+1327020 Sy2 08 51 21.9373979232 +13 27 02.131677108           ~ 8 0
12 PG 0851+202 BLL 08 54 48.8749846272 +20 06 30.639583620   15.649 15.146 15.446   ~ 2513 1
13 2MASS J09420582+1254338 Sy1 09 42 05.8316229312 +12 54 33.640993620   18.95 18.28     ~ 12 0
14 2dFGRS TGN285Z051 Sy1 09 58 33.1980376152 -00 51 18.666040536   18.62 17.84 15.783   ~ 16 0
15 SDSS J100921.26+013334.5 Sy2 10 09 21.2619680184 +01 33 34.587543420   19.30 18.56 17.460   ~ 16 0
16 2MASX J10192756+0134223 Sy1 10 19 27.5553487608 +01 34 22.378904112   18.62 17.93 15.978   ~ 11 0
17 2MASS J10385014+0255550 AGN 10 38 50.1322229952 +02 55 55.126928676           ~ 5 0
18 IRAS F11062+0715 Sy2 11 08 51.0361186344 +06 59 01.452945264   18.89 18.45     ~ 37 0
19 2dFGRS TGN236Z106 Sy1 11 31 26.085 -02 04 59.31   18.062   16.604   ~ 13 0
20 2dFGRS TGN240Z213 Sy2 11 46 10.0430866944 -02 26 19.151641464   18.246   16.863   ~ 11 0
21 2MASS J11464254+5110305 Sy2 11 46 42.473 +51 10 29.60   19.36 18.62     ~ 27 0
22 SDSS J115714.97+081632.0 Sy1 11 57 14.978 +08 16 32.03   20.27 19.47     ~ 10 0
23 NGC 4151 Sy1 12 10 32.5759813872 +39 24 21.063527532   12.18 11.48     ~ 3938 2
24 NGP9 F324-1070509 Sy1 13 22 31.868 +26 31 59.83           ~ 12 0
25 SDSS J133226.34+060627.4 Sy1 13 32 26.3421972720 +06 06 27.299476224   20.29 19.42     ~ 19 0
26 LEDA 3811983 Sy2 13 41 14.8769094408 +22 19 57.628254756           ~ 7 0
27 SDSS J135646.10+102609.0 Sy2 13 56 46.106 +10 26 09.09   18.90 18.11     ~ 95 0
28 2MASS J14505061+0838326 Sy2 14 50 50.5956478656 +08 38 32.547836976           ~ 6 0
29 2MASX J15170926+3353250 Sy2 15 17 09.240 +33 53 24.60   19.56 18.65     ~ 39 1
30 QSO J1536+0441 QSO 15 36 36.2230215960 +04 41 27.067415352   17.75 17.41     ~ 81 1
31 2MASS J15520593+0433172 Sy2 15 52 05.9034745450 +04 33 17.550568794           ~ 15 0
32 2MASX J15561929+0948551 Sy2 15 56 19.2978089376 +09 48 55.465772400           ~ 22 0
33 2MASS J16305676+1649572 Sy1 16 30 56.7514524528 +16 49 57.080157168           ~ 19 0
34 2MASX J22525292+0029289 Sy2 22 52 52.9391844936 +00 29 28.464158904   20.31 19.32     ~ 8 0
35 SDSS J225510.12-081234.3 Sy2 22 55 10.1183747448 -08 12 34.357768524   19.83 19.10     ~ 13 0
36 LEDA 989436 Sy2 23 04 42.8246931384 -09 33 45.348723216   15.83   14.59   ~ 32 0
37 2dFGRS TGS886Z108 Sy2 23 10 51.9549319608 -09 00 11.962756332   17.372   16.161   ~ 16 0
38 PKS 2330+005 Sy2 23 33 13.1657733024 +00 49 11.776280052   19.64 18.84     ~ 24 0

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