1996
DOI: 10.1086/177137
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Is the Accretion Flow in NGC 4258 Advection Dominated?

Abstract: The mass of the central black hole in the active galaxy NGC 4258 (M106) has been measured to be M = 3:6 10 7 M (Miyoshi et al. 1995). The Eddington luminosity corresponding to this mass is L E = 4:5 10 45 erg s 1 . By contrast the X-ray luminosity of the nucleus of NGC 4258 between 2 10 keV is (4 1) 10 40 erg s 1 while the optical/UV luminosity is less than 1:5 10 42 erg s 1 . The luminosity of NGC 4258 is therefore extremely sub-Eddington, L 10 5 L E in X-rays and L 3 10 4 L E even if we take the maximum opti… Show more

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Cited by 233 publications
(270 citation statements)
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“…These should be particularly relevant to transient binaries. In quiescence, their inner disk regions are described well by optically thin advection-dominated accretion flows (ADAFs; see e.g., Lasota et al 1996;Dubus et al 2001). However, a few black hole systems (e.g., GRS 1915+105 and LMC X-3) have been observed in thermal states corresponding to disk luminosities higher than 0.3L Edd (McClintock & Remillard 2003;Steiner et al 2010), and modeling these require optically thick models going beyond the standard thin disks.…”
Section: Discussionmentioning
confidence: 99%
“…These should be particularly relevant to transient binaries. In quiescence, their inner disk regions are described well by optically thin advection-dominated accretion flows (ADAFs; see e.g., Lasota et al 1996;Dubus et al 2001). However, a few black hole systems (e.g., GRS 1915+105 and LMC X-3) have been observed in thermal states corresponding to disk luminosities higher than 0.3L Edd (McClintock & Remillard 2003;Steiner et al 2010), and modeling these require optically thick models going beyond the standard thin disks.…”
Section: Discussionmentioning
confidence: 99%
“…Irrespective of the detail, the outer cold disc in this scenario is expected to be truncated (Done et al 2007;Gilfanov 2010;Yuan & Narayan 2014). The truncation is also required in early stages of an outburst, given that the disc in quiescence does not extend down to the ISCO (Lasota, Narayan & Yi 1996). When the accretion rate increases further, the truncation radius decreases, the disc starts to penetrate the inner flow and eventually reaches the ISCO in the high/soft state (Remillard & McClintock 2006;Done et al 2007).…”
Section: Introductionmentioning
confidence: 99%
“…That is, an ADAF with a surrounding optically thick disk is found to be necessary in modeling the broadband spectrum from the radio to X-ray energy regime of LLAGNs (Lasota et al 1996;Quataert et al 1999;Di Matteo et al 2000Yuan et al 2009;Li et al 2009;Nemmen et al 2006Nemmen et al , 2012. The need for this truncation derives from both the continuum and line emission and, at times, from their variability.…”
Section: Introductionmentioning
confidence: 99%