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The X-ray Spectra of High Redshift Quasars

Published online by Cambridge University Press:  07 August 2017

Claude R. Canizares
Affiliation:
Department of Physics and Center for Space Research, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, MA 02139, U.S.A.
Julia L. White
Affiliation:
Department of Physics and Center for Space Research, Massachusetts Institute of Technology, 77 Massachusetts Avenue, Cambridge, MA 02139, U.S.A.

Abstract

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We present mean spectral parameters for various ensembles of quasars observed with the Einstein Observatory Imaging Proportional Counter (IPC). Our sample contains 71 optically or radio selected quasars with 0.1 < z < 3.5, Galactic NH < 1021 cm−2, total counts of 30 −500, and IPC gain < 19. Quasars are grouped into ensembles according to radio properties (Flat Radio Spectrum [FRS], Steep Radio Spectrum [SRS] or Radio Quiet [RQ]), and either redshift or X-ray luminosity, lx. We find a clear correlation between radio properties and α. FRS quasars have α∼0.4, SRS quasars have α∼0.7 and RQ quasars have α ∼1–1.4. There is no evidence for a dependence of α on z nor, for the FRS and SRS ensembles, on lx over nearly three decades. FRS quasars with 2.0 < z < 3.5 have just as flat mean spectra as those with low z, implying that a single power law, which is flatter than the canonical one with α ∼ 0.65, continues into the 1–10 keV band (in which the observed softer X-rays were emitted). Unfortunately, the results for high redshift and high lx RQ quasars are ambiguous because of systematic uncertainties in the ensemble means. Thus we cannot test the two-component spectral hypothesis of Wilkes and Elvis for these objects. SRS X-ray spectra could be steeper than FRS spectra because of the mixing of two components, although a single intrinsically steeper spectrum is easier to reconcile with the absence of z dependence. The uncertainty in a for RQ quasars with high z leaves open the important question of their contribution to the cosmic X-ray background.

Type
Part 3: X-rays and the Central Source
Copyright
Copyright © Kluwer 1989 

References

Avni, Y., and Tananbaum, H. 1986, Ap. J., 305, 83.Google Scholar
Fabian, A. C. 1988 (preprint).Google Scholar
Giacconi, R. et al. 1979, Ap. J., 230, 540.Google Scholar
Kembhavi, A. K. and Fabian, A. C. 1982, M.N.R.A.S., 198, 921.Google Scholar
Maccacaro, T., Gioia, I., Wolter, A., Zamorani, G. and Stocke, J. T., 1988, Ap. J., 326, 680.Google Scholar
Mushotzky, R.F., 1984, Adv. Space Res., 3, 157.Google Scholar
Tananbaum, H., Avni, Y., Green, R.F., Schmidt, M., and Zamorani, G. 1986, Ap. J., 305, 57.Google Scholar
Urry, M. 1988, in Cordova, F. (ed.), Multiwavelength Astrophysics, (in press).Google Scholar
Wilkes, B., and Elvis, M. 1987, Ap. J., 323, 243.CrossRefGoogle Scholar
Worrall, D.M., Giommi, P., Tananbaum, H., and Zamorani, G. 1987, Ap. J., 313, 596.Google Scholar