2000MNRAS.319..685C


Query : 2000MNRAS.319..685C

2000MNRAS.319..685C - Mon. Not. R. Astron. Soc., 319, 685-699 (2000/December-2)

Spectropolarimetry of broad Hα lines in radio galaxies: constraints on the geometry of the broad-line and scattering regions.

CORBETT E.A., ROBINSON A., AXON D.J. and YOUNG S.

Abstract (from CDS):

We present optical spectropolarimetric observations of three radio-loud broad-line active galactic nuclei: 3C332, 3C351 and 4C73.18, together with new observations of 3C390.3, which we observed previously. Intrinsically polarized broad Hα emission was detected in 3C332 and 3C390.3 at levels of ∼3 per cent and ∼1 per cent, respectively. Significant polarization was not detected in 3C351, while the polarization measured in 4C73.18 (∼1 per cent) is consistent with foreground contamination by the galactic interstellar medium. Although 3C332 and 3C390.3 both exhibit `double-peaked' broad Hα line profiles, their polarization properties differ significantly. The polarized Hα emission in 3C332 has a similar profile to that seen in total flux and the continuum and line emission is polarized at 70° to the axis of the radio source. In 3C390.3, however, the double peaks seen in total flux are suppressed in polarized flux and the Hα line and continuum are polarized at ∼5° to the axis of the radio emission. Comparison of these new observations of 3C390.3 with data obtained 2 years previously reveals significant variations in both total and polarized flux.

The implications of these observations for the relationship between the geometry of the broad-line region and that of the scattering medium are discussed. We argue that models in which the Hα emission arises in a relativistically rotating disc cannot easily explain the observed polarization properties of 3C332 and, in particular, 3C390.3. We consider instead a model in which the line emission originates in a bipolar outflow and present calculations showing that the observed polarization properties of 3C390.3 can be broadly explained by scattering from the inner wall of an obscuring torus, while those of 3C332 are consistent with scattering by particles situated above the poles of the torus. We outline a scheme in which either toroidal or polar scattering dominates in a given object, depending on the orientation of its radio jet axis to our line of sight.


Abstract Copyright: 2000, Royal Astronomical Society

Journal keyword(s): line - profiles - polarization - scattering - galaxies - active - galaxies - jets - quasars - emission lines

Simbad objects: 17

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Number of rows : 17
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 HD 20487 SB* 03 19 47.2567107576 +48 37 40.513080216   7.72 7.66     A0Vn 66 0
2 7C 095855.9+290131 Sy2 10 01 49.5227371368 +28 47 08.943487440   18.21 17.27     ~ 447 1
3 NGC 3516 Sy1 11 06 47.4632200800 +72 34 07.298374656   13.12 12.40     ~ 1638 0
4 QSO J1305-1033 Bla 13 05 33.0150535680 -10 33 19.430383680   15.18 15.23 14.46   ~ 624 1
5 Mrk 668 BLL 14 07 00.39441712 +28 27 14.6901341   16.13 15.35 10.29   ~ 826 3
6 NGC 5548 Sy1 14 17 59.5400291832 +25 08 12.603122268   14.35 13.73     ~ 2895 0
7 IRAS 15599+0206 Sy1 16 02 27.3724911037 +01 57 56.238625559   17.70 16.31     ~ 250 1
8 3C 332.0 Sy1 16 17 42.5380089648 +32 22 34.372277976   18.25 17.45     ~ 268 1
9 8C 1704+608 Bla 17 04 41.3742408840 +60 44 30.520617000   15.65 15.40 15.30   ~ 782 1
10 HD 155197 * 17 10 15.7466372208 -04 50 03.657092136   10.16 9.56     F0V 53 0
11 Z 252-40 Bla 17 19 14.4925971408 +48 58 49.423205136   15.86 14.81 9.44   ~ 335 1
12 HD 161056 * 17 43 47.0221609752 -07 04 46.594311996 6.26 6.68 6.32 5.94 5.67 B3II/III 201 0
13 Z 173-14 Sy1 18 35 03.3896172576 +32 41 46.855964616   16.50 15.39 10.50   ~ 688 1
14 3C 390.3 Bla 18 42 08.9904975672 +79 46 17.127835104   16.06 15.38     ~ 1381 1
15 4C 73.18 BLL 19 27 48.4947009120 +73 58 01.572558816     16.06 15.11   ~ 562 2
16 ICRF J204237.3+750802 Sy1 20 42 37.3079247456 +75 08 02.445851940     14.46 13.80   ~ 281 1
17 LEDA 68751 Sy1 22 23 49.5398449645 -02 06 12.856394895   16.93 15.77 16.02   ~ 511 2

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