2010MNRAS.401..633D


Query : 2010MNRAS.401..633D

2010MNRAS.401..633D - Mon. Not. R. Astron. Soc., 401, 633-665 (2010/January-1)

Modelling the orientation of accretion discs in quasars using hα emission.

DOWN E.J., RAWLINGS S., SIVIA D.S. and BAKER J.C.

Abstract (from CDS):

Infrared spectroscopy of the Hα emission lines of a subsample of 19 high-redshift (0.8 < z < 2.3) Molonglo quasars, selected at 408MHz, is presented. These emission lines are fitted with composite models of broad and narrow emission, which include combinations of classical broad-line regions (BLRs) of fast-moving gas clouds lying outside the quasar nucleus, and/or a theoretical model of emission from an optically thick, flattened, rotating accretion disc, with velocity shifts allowed between the components. All bar one of the 19 sources are found to have emission consistent with the presence of an optically emitting accretion disc, with the exception appearing to display complex emission including at least three broad components. 10 of the quasars have strong Bayesian evidence for broad-line emission arising from an accretion disc together with a standard BLR, selected in preference to a model with two simple broad lines. Thus, the best explanation for the complexity required to fit the broad Hα lines in this sample is optical emission from an accretion disc in addition to a region of fast-moving clouds. We derive estimates of the angle between the rotation axis of the accretion disc and the line of sight. Deprojecting radio sources on the assumption of jets emerging perpendicular to the accretion disc gives rough agreement with expectations of radio source models. The distribution in disc angles is broadly consistent with models in which a Doppler boosted core contributes to the chances of observing a source at low inclination to the line of sight, and in which the radio jets expand at constant speed up to a size of ∼1Mpc. A weak correlation is found between the accretion disc angle and the logarithm of the low-frequency radio luminosity. This is direct, albeit tenuous, evidence for the receding torus model in which the opening angle of the torus widens with increasing radio luminosity. The highest accretion disc angle measured is 48°, consistent with the opening angle predicted for radio-luminous sources. Velocity shifts of the broad Hα components are analysed and the results found to be consistent with a two-component model comprising one single-peaked broad line emitted at the same redshift as the narrow lines, and emission from an accretion disc which appears to be preferentially redshifted with respect to the narrow lines for high-redshift sources and blueshifted relative to the narrow lines for low-redshift sources. An additional analysis is performed in which the disc emission is fixed at the redshift of the narrow-line region; although only two quasars show a robust change in fitted angle, the radio luminosity - disc angle correlation falls sharply in probability, and so is strongly model dependent in this sample.

Abstract Copyright: © 2009 The Authors. Journal compilation © 2009 RAS

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

Simbad objects: 23

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Number of rows : 23
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 [VV98] J022516.7-221523 QSO 02 25 16.6171451568 -22 15 21.884140008     19.70     ~ 15 1
2 QSO B0327-241 Bla 03 29 54.07555386 -23 57 08.7734327   19.68 18.1 19.31   ~ 88 1
3 QSO B0346-279 Bla 03 48 38.14457039 -27 49 13.5657855   20.08 18.63 17.72   ~ 219 1
4 QSO B0413-296 QSO 04 15 08.6933643384 -29 29 03.254910792     19.0     ~ 24 1
5 QSO B0413-210 QSO 04 16 04.35973734 -20 56 27.5175262   18.5 18.5     ~ 91 1
6 PMN J0420-2840 rG 04 20 36.376 -28 41 14.98     21.1     ~ 13 1
7 [VV2000] J043217.7-274625 QSO 04 32 17.6805610368 -27 46 25.228056972     19.60     ~ 12 1
8 QSO B0437-244 QSO 04 39 09.2940514728 -24 22 08.333670072     18.0     ~ 34 1
9 QSO B0450-221 QSO 04 52 44.7804085920 -22 01 19.894766376     18.5     ~ 35 1
10 QSO B0549-213 QSO 05 51 58.2374330040 -21 19 49.964189484     20.0     ~ 31 1
11 [VV98] J102126.9-230154 QSO 10 21 27.5859778224 -23 01 54.538359636     20.90     ~ 12 1
12 QSO B1114-220 QSO 11 16 54.6080742768 -22 16 52.331453868     20.20     ~ 22 1
13 QSO J1210-2758 QSO 12 10 43.7817588144 -27 58 58.977248988     18.80     ~ 22 1
14 QSO J1220-2113 QSO 12 20 22.0001173896 -21 13 15.467258532     20.00     ~ 16 1
15 LEDA 2827122 Sy1 12 25 01.3244584296 -29 38 19.589259444     18.70     ~ 23 1
16 3C 277 rG 12 51 43.581 +50 34 24.90   21       ~ 57 1
17 QSO B1256-243 Bla 12 59 12.6258211992 -24 36 05.508060660     19.5 19.2   ~ 43 1
18 [VV98] J130415.1-252442 QSO 13 04 14.6270 -25 24 36.814     21.00     ~ 16 1
19 QSO B1349-265 QSO 13 52 10.3014616224 -26 49 28.267233852     19.5     ~ 30 1
20 QSO J1358-2352 QSO 13 58 32.7332124744 -23 52 21.240830208     19.20     ~ 19 1
21 [VV98] J135838.0-214855 QSO 13 58 38.2269934296 -21 48 55.048074624     20.60     ~ 19 1
22 QSO B1359-281 Bla 14 02 02.40166665 -28 22 25.1442369   18.7 19.7 19.1   ~ 55 1
23 Mrk 668 BLL 14 07 00.39441712 +28 27 14.6901341   16.13 15.35 10.29   ~ 826 3

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