2000PASP..112..320B


Query : 2000PASP..112..320B

2000PASP..112..320B - Publ. Astron. Soc. Pac., 112, 320-327 (2000/March-0)

Microlensing of broad absorption line quasars: polarization variability.

BELLE K.E. and LEWIS G.F.

Abstract (from CDS):

Roughly 10% of all quasars exhibit broad absorption line (BAL) features which appear to arise in material outflowing at high velocity from the active galactic nucleus. The details of this outflow are, however, very poorly constrained, and the particular nature of the BAL material is essentially unknown. Recently, new clues have become available through polarimetric studies, which have found that BAL troughs are more polarized than the quasar continuum radiation. To explain these observations, researchers have developed models where the BAL material outflows equatorially across the surface of the dusty torus. In these models, however, several sources of the BAL polarization are possible. Here we demonstrate how polarimetric monitoring of gravitationally lensed quasars, such as H1413+117, during microlensing events not only can distinguish between two currently popular models but also can provide further insight into the structure at the cores of BAL quasars.

Abstract Copyright: ∼

Journal keyword(s): Galaxies: Quasars: Absorption Lines - quasars: individual (H1413+117)

Simbad objects: 8

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Number of rows : 8
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 QSO J0831+5245 QSO 08 31 41.7108197808 +52 45 17.616994560   19.2   14.5 13.9 ~ 574 1
2 QSO B1115+080A QSO 11 18 16.951 +07 45 58.23   16.61 16.44     ~ 703 2
3 QSO B1120+0154 QSO 11 23 20.7258496872 +01 37 47.506567620   16.45 16.12     ~ 135 1
4 QSO J1415+1129 QSO 14 15 46.25 +11 29 43.4   17.63 17.23     ~ 678 0
5 QSO B1520+530 QSO 15 21 44.8 +52 54 49   18.2       ~ 123 2
6 QSO B2149-2745 QSO 21 52 07.4534 -27 31 49.718   18.70 18.39     ~ 108 2
7 QSO J2240+0321 QSO 22 40 30.234 +03 21 30.63           ~ 705 1
8 Z 378-15 AGN 22 40 30.23447 +03 21 30.6290           ~ 636 0

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