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The Infrared Spectra of Quasars - A Luminosity Dependence

Published online by Cambridge University Press:  19 July 2016

Beverley J. Wills*
Affiliation:
McDonald Observatory and Department of Astronomy, University of Texas, RLM 15.308 Austin, Texas 78712 U.S.A.

Extract

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The IR-optical-UV continua of quasars are often represented by two components: (i) a flat spectrum component dominating in the optical-UV (the “Big Bump”) and sometimes attributed to thermal radiation from an accretion disk with temperatures of about 20000 to 40000 K - we will call it the “disk” component - and (ii) a near IR component characterized by a steep rise, α ∼ 1 for λ > 1 μm, often thought to be a synchrotron spectrum - an extrapolation of the cm or mm wavelength radio spectrum - although some have preferred an explanation in terms of thermal re-radiation of the ionizing continuum by hot dust (e.g., Hyland and Allen 1982, Neugebauer et al. 1979).

Type
Chapter XI: Quasi-Stellar Objects: Distribution and General Properties
Copyright
Copyright © Reidel 1987 

References

Hyland, A.R., and Allen, D.A. 1982, MNRAS, 199, 943.Google Scholar
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Neugebauer, G., Oke, J.B., Becklin, E.E., and Matthews, K. 1979, Ap. J., 230, 79.Google Scholar
Puetter, R.C., and Hubbard, E.N. 1985, Ap. J., 295, 394.Google Scholar
Soifer, B.T., Neugebauer, G., Oke, J.B., Matthews, K., and Lacy, J.H. 1983, Ap. J., 265, 18.CrossRefGoogle Scholar
Wills, B.J. 1986, Ap. J., submitted.Google Scholar