On the need of an ultramassive black hole in OJ 287

  • Mauri J. Valtonen*
  • , Staszek Zola
  • , A. Gopakumar
  • , Anne Lähteenmäki
  • , Merja Tornikoski
  • , Lankeswar Dey
  • , Alok C. Gupta
  • , Tapio Pursimo
  • , Emil Knudstrup
  • , Jose L. Gomez
  • , Rene Hudec
  • , Martin Jelínek
  • , Jan Štrobl
  • , Andrei V. Berdyugin
  • , Stefano Ciprini
  • , Daniel E. Reichart
  • , Vladimir V. Kouprianov
  • , Katsura Matsumoto
  • , Marek Drozdz
  • , Markus Mugrauer
  • Alberto Sadun, Michal Zejmo, Aimo Sillanpää, Harry J. Lehto, Kari Nilsson, Ryo Imazawa, Makoto Uemura, James W. Davidson
*Tämän työn vastaava kirjoittaja

Tutkimustuotos: LehtiartikkeliArticleScientificvertaisarvioitu

6 Sitaatiot (Scopus)
42 Lataukset (Pure)

Abstrakti

The highly variable blazar OJ 287 is commonly discussed as an example of a binary black hole system. The 130 yr long optical light curve is well explained by a model where the central body is a massive black hole of 18.35 109 solar mass that supports a thin accretion disc. The secondary black hole of 0.15 109 solar mass impacts the disc twice during its 12 yr orbit, and causes observable flares. Recently, it has been argued that an accretion disc with a typical Active Galactic Nuclei (AGN) accretion rate and above mentioned central body mass should be at least six magnitudes brighter than OJ 287's host galaxy and would therefore be observationally excluded. Based on the observations of OJ 287's radio jet, detailed in Marscher and Jorstad (2011), and up-to-date accretion disc models of Azadi et al. (2022), we show that the V-band magnitude of the accretion disc is unlikely to exceed the host galaxy brightness by more than one magnitude, and could well be fainter than the host. This is because accretion power is necessary to launch the jet as well as to create electromagnetic radiation, distributed across many wavelengths, and not concentrated especially on the optical V-band. Further, we note that the claimed V-band concentration of accretion power leads to serious problems while interpreting observations of other AGN. Therefore, we infer that the mass of the primary black hole and its accretion rate do not need to be smaller than what is determined in the standard model for OJ 287.

AlkuperäiskieliEnglanti
Sivut1153-1157
Sivumäärä5
JulkaisuMonthly Notices of the Royal Astronomical Society
Vuosikerta525
Numero1
DOI - pysyväislinkit
TilaJulkaistu - 1 lokak. 2023
OKM-julkaisutyyppiA1 Alkuperäisartikkeli tieteellisessä aikakauslehdessä

Rahoitus

This work was partly funded by Narodowe Centrum Nauki (NCN) grant no. 2018/29/B/ST9/01793 (SZ) and Japan Society for the Promotion of Science (JSPS) KAKENHI grant no. 19K03930 (KM). SC acknowledges support by Agenzia Spaziale Italiana (ASI) through contract ASI-INFN 2021-43-HH.0 for SSDC, and Instituto Nazionale di Fisica Nucleare (INFN). RH acknowledges the EU project H2020 AHEAD2020, grant agreement 871158, and internal Czech Technical University (CTU) grant SGS21/120/OHK3/2T/13. ACG is partially supported by Chinese Academy of Sciences (CAS) President’s International Fellowship Initiative (PIFI; grant no. 2016VMB073). MJV acknowledges a grant from the Finnish Society for Sciences and Letters.

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