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High Optical Polarization in Flat-Spectrum Radio Sources

Published online by Cambridge University Press:  07 August 2017

D. Wills
Affiliation:
University of Texas
Beverley J. Wills
Affiliation:
University of Texas
R.R.J. Antonucci
Affiliation:
STScI
Richard Barvainis
Affiliation:
NRAO
Michel Breger
Affiliation:
University of Vienna
J. A. Bailey
Affiliation:
AAO
J. H. Hough
Affiliation:
Hatfield Polytechnic, UK
K. Ballard
Affiliation:
University of Edinburgh

Extract

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We have made a polarimetric survey of 84 quasi-stellar objects, to supplement published polarization measurements for two samples of quasars identified with flat-spectrum (core-dominant) radio sources in 5 GHz surveys made at Bonn (Kühr 1980) and at the VLA (Perley 1982). The observations were made using the McDonald 2.1m Struve reflector and the polarimeter described by Breger (1979); the typical accuracy is 0.5% for an 18 mag object after half an hour. Earlier surveys, such as those by Stockman, Moore and Angel (1984), included objects of various radio spectral types, and only a small fraction of the objects showed high polarization (> 3%), but our sample of flat-spectrum quasars reveals many more (about half) of the objects to be highly polarized. Some of them are, expectedly, of the BL Lac class, but many of them have strong broad emission lines. There are two striking correlations among the results:

  1. (1) The degree of polarization is strongly correlated with the dominance of the radio core - specifically, with the ratio, R, of core to lobe luminosity (Fig. 1). For example, about 75% of the objects with log R > 1.25 and redshift z < 1 have p > 3%. This relation implies that if the radio core radiation is beamed, as seems likely, then so is the optical synchrotron component.

  2. (2) The fraction of objects with p > 3% is inversely correlated with redshift (e.g. Fig. 2). The most likely interpretation of this result is that quasars' degree of polarization decreases with decreasing rest wavelength, and the shorter wavelengths are shifted into our wide observational passband at higher redshifts.

Type
Part 5: Structure of the Central Object and NLR
Copyright
Copyright © Kluwer 1989 

References

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