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The Source of Power for AGNs

The diversity of AGN properties has been a source of confusion for astronomers; however, when they are considered carefully, certain common traits make them easier to understand as a whole. Foremost among these traits are their energy requirements.

The fact that AGNs are observable at all despite their immense distances imposes stringent constraints on their energy sources. Nuclear burning is not efficient enough. Even if all available matter is fused into iron nuclei, less than 1% of the available mass would be converted into energy. To produce the necessary energy to drive an AGN over a significant timescale, a substantial fraction of the mass of the entire galaxy would have to be consumed. Such a process would leave a high concentration of residual mass near the galactic nuclei, but there is no evidence of such massive relics. In addition, there's the problem of delivering this much mass from a galaxy tens of kiloparsecs across into a region less than 1/4 of a parsec across [Miyoshi et al., 1995]. The only known process that can reasonably produce the necessary power is the release of gravitational potential energy from a relativistic potential well. Theoretically, a rotating black hole could convert nearly 30% of the infalling mass into radiant energy. Even if we assume a more modest efficiency of 10%, the constraints of providing fuel are much more reasonable, and the remnant masses are consistent with observations. This has lead astronomers to believe that AGNs are powered by accreting black holes with masses of tex2html_wrap_inline138  [Lynden-Bell, 1969].

Numerous observations have provided much evidence (albeit circumstantial) in support of the supermassive black hole hypothesis. For instance, the extreme velocity dispersion observed at the center of M87 is most plausibly explained by the existence of a black hole with a mass of tex2html_wrap_inline140  [Young et al., 1978, Sargent et al., 1978]. Stronger evidence is found at the core of NGC 4258, where Miyoshi et al. have observed water maser emission from a swirling cloud in perfect Keplerian orbit, whose properties imply a central mass of tex2html_wrap_inline142 contained within a radius of at most 0.13 pc [Miyoshi et al., 1995]. One of the best pieces of evidence yet found for a supermassive black hole at the center of an active galaxy is the Fe K- tex2html_wrap_inline124 feature from the Seyfert 1 galaxy MGC-6-30-15, where the relativistically broad emission line is gravitationally reddened and appears to come from the innermost regions of an accretion disk around a spinning black hole [Tanaka et al., 1995, Iwasawa et al., 1996]. (Evidence has even been found for the existence of supermassive black holes at the centers of non-active galaxies. At the AAS meeting earlier this month, Andreas Eckart of the Max Planck Institute presented data based upon stellar proper motions which suggest that an object with a mass of tex2html_wrap_inline146 lies at the center of our own galaxy.)


next up previous
Next: The Unified Model Up: Using features of X-ray Previous: Seyfert Galaxies & Active

Jonathan Gelbord
Thu Mar 26 15:22:21 EST 1998