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Optical monitoring of the broad-line radio galaxy 3C390.3

  • Matthias Dietrich
  • , Bradley M. Peterson
  • , Catherine J. Grier
  • , Misty C. Bentz
  • , Jason Eastman
  • , Stephan Frank
  • , Raymond Gonzalez
  • , Jennifer L. Marshall
  • , Darren L. Depoy
  • , Jose L. Prieto

Research output: Contribution to journalArticlepeer-review

Abstract

We have undertaken a new ground-based monitoring campaign on the broad-line radio galaxy 3C390.3 to improve the measurement of the size of the broad emission-line region and to estimate the black hole mass. Optical spectra and g-band images were observed in late 2005 for three months using the 2.4m telescope at MDM Observatory. Integrated emission-line flux variations were measured for the hydrogen Balmer lines Hα, Hβ, Hγ, and for the helium line He IIλ4686, as well as g-band fluxes and the optical active galactic nucleus (AGN) continuum at λ =5100 Å. The g-band fluxes and the optical AGN continuum vary simultaneously within the uncertainties, τcent = (0.2 ± 1.1)days. We find that the emission-line variations are delayed with respect to the variable g-band continuum by τ(Hα) = 56.3+2.4-6.6days, τ(Hβ) = 44.3+3.0-3.3days, τ(Hγ) = 58.1 +4.3-6.1days, and τ(He II4686) = 22.3 +6.5-3.8days. The blue and red peaks in the double-peaked line profiles, as well as the blue and red outer profile wings, vary simultaneously within ±3 days. This provides strong support for gravitationally bound orbital motion of the dominant part of the line-emitting gas. Combining the time delay of the strong Balmer emission lines of Hα and Hβ and the separation of the blue and red peaks in the broad double-peaked profiles in their rms spectra, we determine Mvir bh = 1.77+0.29-0.31 × 108 MȮ and using σline of the rms spectra M vir bh = 2.60+0.23-0.31 × 108 MȮ for the central black hole of 3C390.3, respectively. Using the inclination angle of the line-emitting region which is measured from superluminal motion detected in the radio range, accretion disk models to fit the optical double-peaked emission-line profiles, and X-ray observations, the mass of the black hole amounts to Mbh = 0.86 +0.19-0.18 × 109 MȮ (peak separation) and Mbh = 1.26+0.21-0.16 × 109 MȮline), respectively. This result is consistent with the black hole masses indicated by simple accretion disk models to describe the observed double-peaked profiles, derived from the stellar dynamics of 3C390.3, and with the AGN radius-luminosity relation. Thus, 3C390.3 as a radio-loud AGN with a low Eddington ratio, L edd/L bol = 0.02, follows the same AGN radius-luminosity relation as radio-quiet AGNs.

Original languageEnglish (US)
Article number53
JournalAstrophysical Journal
Volume757
Issue number1
DOIs
StatePublished - Sep 20 2012
Externally publishedYes

Keywords

  • galaxies: active
  • quasars: emission lines
  • quasars: individual (3C390.3)

ASJC Scopus subject areas

  • Astronomy and Astrophysics
  • Space and Planetary Science

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