Published August 1, 2012 | Version v1
Journal article

THE STRUCTURE AND EMISSION MODEL OF THE RELATIVISTIC JET IN THE QUASAR 3C 279 INFERRED FROM RADIO TO HIGH-ENERGY γ-RAY OBSERVATIONS IN 2008-2010

  • 1. Kavli Institute for Particle Astrophysics and Cosmology, SLAC National Accelerator Laboratory, Stanford University, 2575 Sand Hill Road M/S 29, Menlo Park, CA 94025 (United States)
  • 2. University of Colorado, UCB 440, Boulder, CO 80309 (United States)
  • 3. Nicolaus Copernicus Astronomical Center, 00-716 Warsaw (Poland)
  • 4. Space Science Institute, Boulder, CO 80301 (United States)
  • 5. Infrared Processing and Analysis Center, California Institute of Technology Pasadena, CA 91125 (United States)
  • 6. Max-Planck Institut für Extraterrestrische Physik, 85748 Garching (Germany)
  • 7. Department of Physics, Stockholm University, AlbaNova, SE-106 91 Stockholm (Sweden)
  • 8. Department of Physical Sciences, Hiroshima University, Higashi-Hiroshima, Hiroshima 739-8526 (Japan)
  • 9. Institute of Space and Astronautical Science, JAXA, 3-1-1 Yoshinodai, Chuo-ku, Sagamihara, Kanagawa 252-5210 (Japan)
  • 10. Cahill Center for Astronomy and Astrophysics, California Institute of Technology, Pasadena, CA 91125 (United States)
  • 11. Agenzia Spaziale Italiana (ASI) Science Data Center, I-00044 Frascati (Roma) (Italy)
  • 12. NASA Goddard Space Flight Center, Greenbelt, MD 20771 (United States)

Description

We present time-resolved broadband observations of the quasar 3C 279 obtained from multi-wavelength campaigns conducted during the first two years of the Fermi Gamma-ray Space Telescope mission. While investigating the previously reported γ-ray/optical flare accompanied by a change in optical polarization, we found that the optical emission appears to be delayed with respect to the γ-ray emission by about 10 days. X-ray observations reveal a pair of 'isolated' flares separated by ∼90 days, with only weak γ-ray/optical counterparts. The spectral structure measured by Spitzer reveals a synchrotron component peaking in the mid-infrared band with a sharp break at the far-infrared band during the γ-ray flare, while the peak appears in the millimeter (mm)/submillimeter (sub-mm) band in the low state. Selected spectral energy distributions are fitted with leptonic models including Comptonization of external radiation produced in a dusty torus or the broad-line region. Adopting the interpretation of the polarization swing involving propagation of the emitting region along a curved trajectory, we can explain the evolution of the broadband spectra during the γ-ray flaring event by a shift of its location from ∼1 pc to ∼4 pc from the central black hole. On the other hand, if the γ-ray flare is generated instead at sub-pc distance from the central black hole, the far-infrared break can be explained by synchrotron self-absorption. We also model the low spectral state, dominated by the mm/sub-mm peaking synchrotron component, and suggest that the corresponding inverse-Compton component explains the steady X-ray emission.

Availability note (English)

Available from http://dx.doi.org/10.1088/0004-637X/754/2/114

Additional details

Identifiers

Publishing Information

Journal Title
Astrophysical Journal
Journal Volume
754
Journal Issue
2
Journal Page Range
[22 p.]
ISSN
0004-637X
CODEN
ASJOAB