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A Limit Relation between Black Hole Mass and Hβ Width: Testing Super-Eddington Accretion in Active Galactic Nuclei

机译:黑洞质量与Hβ宽度之间的极限关系:测试活跃银河核中的超爱丁顿积聚

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We show that there is a limit relation between the black hole mass (MBH) and the width at half-maximum (υFWHM) of Hβ for active galactic nuclei (AGNs) with super-Eddington accretion rates. When a black hole has a super-Eddington accretion rate, the empirical relation derived from reverberation mapping can be applied in two possible ways. First, it reduces to a relation between the black hole mass and the size of the broad-line region because of photon-trapping effects inside the accretion disk. For the empirical reverberation relation of Kaspi et al., we obtain the limit relation MBH = (2.9–12.6) × 106 [vFWHM/(103?km?s-1)]6.67M⊙, called the Eddington limit. Second, the Eddington limit luminosity will be relaxed if the trapped photons can escape from the magnetized super-Eddington accretion disk via the photon bubble instability, and the size of the broad-line region will be enlarged according to the empirical reverberation relation, leading to a relatively narrow Hβ width. We call this the Begelman limit. Using this limit relation, we searched 164 AGNs for super-Eddington accretion. We find that most of them are well confined by the Eddington limit relation—that is, most have sub-Eddington accretion rates—but there are a handful of objects located between the Eddington and Begelman limit lines; they may be candidate super-Eddington accretors in a hybrid structure of photon trapping and photon bubble instability. The maximum Hβ width is in the range (3.0–3.8) × 10 3 km s-1 for the most massive black holes with super-Eddington accretion rates among AGNs. We suggest that the FWHM(Hβ)-MBH relation is a reliable and convenient method to test whether a source is super-Eddington and useful to probe the structure of the super-Eddington accretion process.
机译:我们表明,对于具有超爱丁顿积聚速率的活性银河核(AGN),黑洞质量(MBH)与Hβ的半最大宽度(υFWHM)之间存在极限关系。当黑洞具有超爱丁顿累积率时,可以以两种可能的方式应用从混响映射得出的经验关系。首先,由于吸积盘内部的光子俘获效应,它减小到黑洞质量和宽线区域的尺寸之间的关系。对于Kaspi等人的经验混响关系,我们得到极限关系MBH =(2.9–12.6)×106 [vFWHM /(103?km?s-1)]6.67M⊙,称为爱丁顿极限。其次,如果被捕获的光子可以通过光子气泡不稳定性从被磁化的超爱丁顿吸积盘中逸出,则爱丁顿极限光度将得到放宽,并且根据经验混响关系,宽线区域的尺寸将增大,从而导致Hβ宽度相对较窄。我们称其为Begelman极限。使用这个极限关系,我们搜索了164个AGN中的超级爱丁顿积聚。我们发现,它们中的大多数都受到爱丁顿极限关系的很好限制,也就是说,大多数具有次爱丁顿积聚率,但是在爱丁顿极限和Begelman极限线之间有少量物体;它们可能是光子俘获和光子气泡不稳定性的混合结构中的超级爱丁顿候选物。对于AGN中具有超爱丁顿积聚率的最大黑洞,最大Hβ宽度在(3.0–3.8)×10 3 km s-1范围内。我们建议FWHM(Hβ)-MBH关系是一种可靠且方便的方法,用于测试源是否为超级爱丁顿,并且对于探测超级爱丁顿积聚过程的结构很有用。

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