2016
DOI: 10.1051/0004-6361/201527636
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The slimming effect of advection on black-hole accretion flows

Abstract: Context. At super-Eddington rates accretion flows onto black holes have been described as slim (aspect ratio H/R 1) or thick (H/R > 1) discs, also known as tori or (Polish) doughnuts. The relation between the two descriptions has never been established, but it was commonly believed that at sufficiently high accretion rates slim discs inflate, becoming thick. Aims. We wish to establish under what conditions slim accretion flows become thick. Methods. We use analytical equations, numerical 1 + 1 schemes, and num… Show more

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Cited by 51 publications
(52 citation statements)
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“…h/R ∼ 10 −3 -0.1 (Thompson et al 2005). h/R ∼ 0.1-0.7 in super-Eddington ADAFs (Lasota et al 2016). fg depends on h/R, ρ disk and τAGN .…”
Section: Rate Of Black Hole Binary Mergers In Agn Disksmentioning
confidence: 87%
“…h/R ∼ 10 −3 -0.1 (Thompson et al 2005). h/R ∼ 0.1-0.7 in super-Eddington ADAFs (Lasota et al 2016). fg depends on h/R, ρ disk and τAGN .…”
Section: Rate Of Black Hole Binary Mergers In Agn Disksmentioning
confidence: 87%
“…While the increased radiation pressure within the disk itself acts to increase its scale height, once this scale height is significant, radiation pressure from the opposite face of the funnel must also act against any further closing of its opening angle, which could potentially help produce this effect. Furthermore, Lasota et al (2016) argue that at the highest accretion rates the disk may become fully advectiondominated, and that in this regime the scale height of the disk can no longer increase (or equivalently, the opening angle of the inner funnel can no longer close) with increasing accretion rate, as basically all the energy is advected over the horizon and is not able to further inflate the disk. A roughly constant opening angle for the inner disk, as may be required to explain the broadband Holmberg IX X-1…”
Section: Discussionmentioning
confidence: 99%
“…King 2008;Middleton et al 2015a). However, while this must happen over some range ofṀ in order for the disc structure to transition from the thin disc expected for standard sub-Eddington accretion to the funnel-like geometry expected for super-Eddington accretion, as discussed by Lasota et al (2016), once the disc reaches the point of being fully advection-dominated the opening angle of the disc should tend to a constant (H/R ∼ 1, where H is the scale height of the disc at radius R). Walton et al (2017) speculated that once this occurs, rather than closing the funnel further, an increase inṀ instead simply increases the characteristic radius within which geometric beaming occurs, such that emission that is already within this region (the highest energies probed) experiences no further collimation with an increase inṀ, while emission from larger radii (i.e.…”
Section: Modelmentioning
confidence: 99%