2013ApJ...775...49S


Query : 2013ApJ...775...49S

2013ApJ...775...49S - Astrophys. J., 775, 49 (2013/September-3)

Constraining sub-parsec binary supermassive black holes in quasars with multi-epoch spectroscopy. I. The general quasar population.

SHEN Y., LIU X., LOEB A. and TREMAINE S.

Abstract (from CDS):

We perform a systematic search for sub-parsec binary supermassive black holes (BHs) in normal broad-line quasars at z < 0.8, using multi-epoch Sloan Digital Sky Survey (SDSS) spectroscopy of the broad Hβ line. Our working model is that (1) one and only one of the two BHs in the binary is active; (2) the active BH dynamically dominates its own broad-line region (BLR) in the binary system, so that the mean velocity of the BLR reflects the mean velocity of its host BH; (3) the inactive companion BH is orbiting at a distance of a few RBLR, where RBLR∼ 0.01-0.1 pc is the BLR size. We search for the expected line-of-sight acceleration of the broad-line velocity from binary orbital motion by cross-correlating SDSS spectra from two epochs separated by up to several years in the quasar rest frame. Out of ∼700 pairs of spectra for which we have good measurements of the velocity shift between two epochs (1σ error ∼40 km/s), we detect 28 systems with significant velocity shifts in broad Hβ, among which 7 are the best candidates for the hypothesized binaries, 4 are most likely due to broad-line variability in single BHs, and the rest are ambiguous. Continued spectroscopic observations of these candidates will easily strengthen or disprove these claims. We use the distribution of the observed accelerations (mostly non-detections) to place constraints on the abundance of such binary systems among the general quasar population. Excess variance in the velocity shift is inferred for observations separated by longer than 0.4 yr (quasar rest frame). Attributing all the excess to binary motion would imply that most of the quasars in this sample must be in binaries, that the inactive BH must be on average more massive than the active one, and that the binary separation is at most a few times the size of the BLR. However, if this excess variance is partly or largely due to long-term broad-line variability, the requirement of a large population of close binaries is much weakened or even disfavored for massive companions. Future time-domain spectroscopic surveys of normal quasars can provide vital prior information on the structure function of stochastic velocity shifts induced by broad-line variability in single BHs. Such surveys with improved spectral quality, increased time baseline, and more epochs can greatly improve the statistical constraints of this method on the general binary population in broad-line quasars, further shrink the allowed binary parameter space, and detect true sub-parsec binaries.

Abstract Copyright: ∼

Journal keyword(s): black hole physics - galaxies: active - line: profiles - quasars: general - surveys

Simbad objects: 30

goto Full paper

goto View the references in ADS

Number of rows : 30
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 [VV2006] J012016.7-092028 QSO 01 20 16.7297353800 -09 20 28.736128176   17.97 18.00     ~ 27 0
2 2MASS J01583626+0106320 QSO 01 58 36.2621191968 +01 06 32.058828756   18.07 17.74     ~ 26 0
3 PB 6739 QSO 02 12 25.5667246680 +01 00 56.148118164   18.64 18.57     ~ 53 3
4 SDSS J030100.23+000429.2 QSO 03 01 00.2364029208 +00 04 29.359692696   19.66 19.51     ~ 29 0
5 PB 7009 Sy1 03 06 39.5824276346 +00 03 43.161393991   18.00 17.54     ~ 79 0
6 [VV2006] J032205.1+001200 QSO 03 22 05.0504499384 +00 12 01.459850904   17.45 17.36     ~ 32 0
7 KUV 03197+0045 Sy1 03 22 13.9031891472 +00 55 13.438904772   16.82 16.57     ~ 55 0
8 2MASS J07470020+2856086 QSO 07 47 00.1948158504 +28 56 08.499587748   19.42 19.27     ~ 10 0
9 [VV2006c] J080811.0+070510 Sy1 08 08 11.0077438944 +07 05 10.689298044   19.62 19.55     ~ 20 0
10 [VV2006] J083042.2+415143 QSO 08 30 42.1956334656 +41 51 42.850111356   18.87 18.79     ~ 28 0
11 PG 0851+202 BLL 08 54 48.8749846272 +20 06 30.639583620   15.649 15.146 15.446   ~ 2513 1
12 US 737 QSO 09 35 02.5322373288 +43 31 10.637924844   15.92 15.93     ~ 78 1
13 NGC 3393 Sy2 10 48 23.4653152920 -25 09 43.487648784   13.10 13.95 11.67 12.2 ~ 471 1
14 2MASS J11201009+1843132 QSO 11 20 10.1515388088 +18 43 13.322156988   19.04 18.73     ~ 15 0
15 [VV2006] J122909.5-003530 QSO 12 29 09.5268749208 -00 35 30.091132536   18.38 18.39     ~ 29 0
16 2QZ J135252.0+003758 Sy1 13 52 52.1439008376 +00 37 58.579293648   18.24 18.15     ~ 37 0
17 2MASS J13582958+0109085 Sy1 13 58 29.5777199232 +01 09 08.499689316   18.65 18.25     ~ 32 0
18 2QZ J140030.1+002207 Sy1 14 00 30.1431255432 +00 22 08.488818372   18.54 18.22     ~ 28 0
19 [VV2006] J141020.6+364322 QSO 14 10 20.5713846888 +36 43 22.766600784   18.57 18.56     ~ 28 0
20 2MASS J15370594+0055228 Sy1 15 37 05.9562688200 +00 55 22.872386604   17.66 17.28     ~ 34 0
21 2MASS J15465664+0057197 Sy1 15 46 56.6220861600 +00 57 19.609976628   18.94 18.53     ~ 21 0
22 2MASX J15505317+0521119 Sy1 15 50 53.1634739928 +05 21 12.188158884   17.54 17.13     ~ 34 0
23 SDSS J165638.87+362121.0 Sy1 16 56 38.8666796160 +36 21 21.063624516   20.09 19.72     ~ 20 0
24 [VV2006] J224623.6+130335 QSO 22 46 23.5406652024 +13 03 35.936029980   18.08 18.04     ~ 26 0
25 2MASS J23094616+0000496 Sy1 23 09 46.1482273416 +00 00 48.892288032   19.37 18.95     ~ 37 0
26 PHL 507 QSO 23 25 25.3283710344 +00 03 52.183149480   18.77 18.54     ~ 32 0
27 2SLAQ J234018.85-011027.2 Sy1 23 40 18.8546335008 -01 10 27.325414344   19.95 19.65     ~ 29 0
28 [VV2006] J234145.5-004640 QSO 23 41 45.5163804312 -00 46 40.584076248   18.04 17.93     ~ 40 0
29 PB 5546 QSO 23 49 32.7696958104 -00 36 45.828403740   17.95 17.63     ~ 50 0
30 LBQS 2353+0032 QSO 23 55 45.5149776888 +00 49 23.149032312   18.40 18.28     ~ 39 0

To bookmark this query, right click on this link: simbad:objects in 2013ApJ...775...49S and select 'bookmark this link' or equivalent in the popup menu