dc.contributor.author | Thomsen, Lars Lund | |
dc.contributor.author | Dai, Lixin | |
dc.contributor.author | Kara, Erin | |
dc.contributor.author | Reynolds, Chris | |
dc.date.accessioned | 2022-05-27T15:49:17Z | |
dc.date.available | 2022-04-20T15:15:10Z | |
dc.date.available | 2022-05-27T15:49:17Z | |
dc.date.issued | 2022-02 | |
dc.date.submitted | 2021-11 | |
dc.identifier.issn | 0004-637X | |
dc.identifier.issn | 1538-4357 | |
dc.identifier.uri | https://hdl.handle.net/1721.1/141963.2 | |
dc.description.abstract | <jats:title>Abstract</jats:title>
<jats:p>X-ray reverberation is a powerful technique that uses the echoes of the coronal emission reflected by a black hole (BH) accretion disk to map out the inner disk structure. While the theory of X-ray reverberation has been developed almost exclusively for standard thin disks, reverberation lags have recently been observed from likely super-Eddington accretion sources such as the jetted tidal disruption event Swift J1644+57. In this paper, we extend X-ray reverberation studies into the regime of super-Eddington accretion with a focus on investigating the lags in the fluorescent Fe K<jats:italic>α</jats:italic> line region. We find that the coronal photons are mostly reflected by the fast and optically thick winds launched from the super-Eddington accretion flow, and this funnel-like reflection geometry produces lag–frequency and lag–energy spectra with unique observable characteristics. The lag–frequency spectrum exhibits a step-function-like decline near the first zero-crossing point. As a result, the magnitude of the lag scales linearly with the BH mass for a large parameter space, and the shape of the lag–energy spectrum remains almost independent of the choice of frequency bands. Not only can these features be used to distinguish super-Eddington accretion systems from sub-Eddington systems, but they are also key for constraining the reflection geometry and extracting parameters from the observed lags. When fitting the observed reverberation lag of Swift J1644+57 to our modeling, we find that the super-Eddington disk geometry is slightly preferred over the thin disk geometry, and we obtain a BH mass of 5–6 × 10<jats:sup>6</jats:sup>
<jats:italic>M</jats:italic>
<jats:sub>☉</jats:sub> and a coronal height around 10 <jats:italic>R<jats:sub>g</jats:sub>
</jats:italic>.</jats:p> | en_US |
dc.language.iso | en | |
dc.publisher | American Astronomical Society | en_US |
dc.relation.isversionof | http://dx.doi.org/10.3847/1538-4357/ac3df3 | en_US |
dc.rights | Creative Commons Attribution 4.0 International license | en_US |
dc.rights.uri | https://creativecommons.org/licenses/by/4.0/ | en_US |
dc.source | The American Astronomical Society | en_US |
dc.title | Relativistic X-Ray Reverberation from Super-Eddington Accretion Flow | en_US |
dc.type | Article | en_US |
dc.identifier.citation | Thomsen, Lars Lund, Dai, Lixin, Kara, Erin and Reynolds, Chris. 2022. "Relativistic X-Ray Reverberation from Super-Eddington Accretion Flow." The Astrophysical Journal, 925 (2). | en_US |
dc.contributor.department | MIT Kavli Institute for Astrophysics and Space Research | |
dc.relation.journal | Astrophysical Journal | en_US |
dc.eprint.version | Final published version | en_US |
dc.type.uri | http://purl.org/eprint/type/JournalArticle | en_US |
eprint.status | http://purl.org/eprint/status/PeerReviewed | en_US |
dc.date.updated | 2022-04-20T15:07:00Z | |
dspace.orderedauthors | Thomsen, LL; Dai, L; Kara, E; Reynolds, C | en_US |
dspace.date.submission | 2022-04-20T15:07:02Z | |
mit.journal.volume | 925 | en_US |
mit.journal.issue | 2 | en_US |
mit.license | PUBLISHER_CC | |
mit.metadata.status | Authority Work Needed | en_US |