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Pair Production in AGN

Published online by Cambridge University Press:  07 August 2017

C. Done
Affiliation:
Institute of Astronomy, Madingley Road, Cambridge CB3 0HA, U.K.
A. C. Fabian
Affiliation:
Institute of Astronomy, Madingley Road, Cambridge CB3 0HA, U.K.

Extract

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The X-ray luminosity and variability of many AGN are sufficiently extreme that any hard γ-rays produced in the source will collide with the X-rays and create electron-positron pairs, rather than escape. A small region where vast amounts of energy are produced, such as an AGN, is an ideal place to accelerate particles to relativistic energies and so produce γ-rays by Compton scattering. The observed X-ray spectra of AGN are hard and indicate that most of the luminosity is at the highest energies so that absorption of the γ-rays represents a large fraction of the energy flux, which can then be re-radiated at lower energies. Pairs can thus effectively reprocess much of the radiant power in an AGN.

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

References

Done, C., and Fabian, A.C. 1988, preprint.Google Scholar
Fabian, A.C., Blandford, R.D., Guilbert, P.W., Phinney, E.S., and Cuellar, L. 1986, M.N.R.A.S., 221, 931.Google Scholar
Guilbert, P.W., Fabian, A.C., and Rees, M.J. 1983, M.N.R.A.S., 205, 593.CrossRefGoogle Scholar
Lightman, A.P., and Zdziarski, A.A. 1987, Ap. J., 319, 643.Google Scholar
Mushotzky, R.F. 1982, Ap.J., 256, 92.Google Scholar
Svensson, R. 1987, M.N.R.A.S., 227, 403.Google Scholar
Turner, T.J., and Pounds, K.A. 1988, preprint.Google Scholar