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H1821+643

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Quasar in theconstellation Draco
H1821+643
Chandra X-ray Observatory image of H1821+643
Observation data(Epoch J2000.0)
ConstellationDraco
Right ascension18h 21m 57.2365s
Declination+64° 20′ 36.226″
Redshift0.2970
Distance3.4 gigalight-years (1.0 Gpc)
TypeQuasar
Apparent magnitude (V)14.24
See also:Quasar,List of quasars

H1821+643 is an extraordinarily luminous, radio-quietquasar in theconstellation ofDraco.[1]The associated Active Galactic Nucleus (AGN) is situated in the Brightest Central Galaxy (BCG) of a massive (6.3×1014M{\displaystyle \sim 6.3\times 10^{14}M_{\odot }}), strongcooling flow cluster, CL 1821+64.[2] Russel et al. (2010) spatially isolated its X-ray signal from the surrounding cluster in Chandra X-ray observatory observations and computedL=1047erg/s{\displaystyle L_{\odot }=10^{47}erg/s} from the observed X-ray luminosity.[2]

Supermassive black hole

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The SMBH centred in CL 1821+64 is believed to be among the most massive in the known Universe.[2] A variety of techniques have found different values for the mass. 5 studies found valuesMBH109M{\displaystyle M_{BH}\sim 10^{9}M_{\odot }}. Kim et al. (2004) and Floyd et al. (2008) used galactic bulge luminosity fits derived from Hubble data to find109M{\displaystyle 10^{9}M_{\odot }} and3×109M{\displaystyle 3\times 10^{9}M_{\odot }} respectively. Russell et al. (2010) provided a rough estimate ofMBH3×109{\displaystyle M_{BH}\sim 3\times 10^{9}}M.[2] This was an underestimate withlog(ΔMBH/M)1{\displaystyle \log(\Delta M_{BH}/M_{\odot })\geq 1}. Kolman et al. (1991) and Shapovalova (2016) independently modelled the quasar UV spectrum to findMBH3×109M{\displaystyle M_{BH}\sim 3\times 10^{9}M_{\odot }}. Capellupo et al. (2017) foundMBH3×109{\displaystyle M_{BH}\sim 3\times 10^{9}} usingHβ{\displaystyle H\beta } line emissions. 2 independent X-ray studies found significantly higher values. Reynolds et al. (2014) found6×109M{\displaystyle 6\times 10^{9}M_{\odot }} by modelling reflection from the accretion disc and Walker et al. found3×1010M{\displaystyle 3\times 10^{10}M_{\odot }} by modelling the interaction of the black hole with the Intracluster medium (ICM) as a Compton-cooled feeding cycle.MBH{\displaystyle M_{BH}} is in the rangelog(MBH/M)9.210.5{\displaystyle \log(M_{BH}/M_{\odot })\sim 9.2-10.5}.[2]

TheSchwarzschild diameter of this black hole is between 9.4terametres (63 AU) and 188terametres (1,260 AU), which is about 16 times the diameter ofPluto's orbit. If the hole were a Euclidean sphere, the average density would be 18 g/m3,1%{\displaystyle \sim 1\%} the density ofair at sea level on Earth.[a]

Footnotes

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  1. ^Mass 3.0×1010 *2.0×1030=6.0×1040 kg.Volume at radius 8.6×1013 m is 2.66×1042 m3.

References

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  1. ^Walker, S. A.; Fabian, A. C.; Russell, H. R.; Sanders, J. S. (2014)."The effect of the quasar H1821+643 on the surrounding intracluster medium: Revealing the underlying cooling flow".Monthly Notices of the Royal Astronomical Society.442 (3): 2809.arXiv:1405.7522.Bibcode:2014MNRAS.442.2809W.doi:10.1093/mnras/stu1067.
  2. ^abcdeSisk-Reynés, Júlia; Reynolds, Christopher S.; Matthews, James H.; Smith, Robyn N. (2022)."Evidence for a moderate spin from X-ray reflection of the high-mass supermassive black hole in the cluster-hosted quasar H1821+643".Monthly Notices of the Royal Astronomical Society.514 (2): 2568.arXiv:2205.12974.Bibcode:2022MNRAS.514.2568S.doi:10.1093/mnras/stac1389.

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