4.6 Article

MINUTE-TIMESCALE > 100 MeV γ-RAY VARIABILITY DURING THE GIANT OUTBURST OF QUASAR 3C 279 OBSERVED BY FERMI-LAT IN 2015 JUNE

Journal

ASTROPHYSICAL JOURNAL LETTERS
Volume 824, Issue 2, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.3847/2041-8205/824/2/L20

Keywords

galaxies: active; galaxies: jets; gamma rays: galaxies; quasars: individual (3C 279); radiation mechanisms: non-thermal

Funding

  1. NASA (United States)
  2. DOE (United States)
  3. CEA/Irfu (France)
  4. IN2P3/CNRS (France)
  5. ASI (Italy)
  6. NFN (Italy)
  7. MEXT (Japan)
  8. KEK (Japan)
  9. JAXA (Japan)
  10. K.A. Wallenberg Foundation
  11. Swedish Research Council
  12. National Space Board (Sweden)
  13. INAF (Italy)
  14. CNES (France)
  15. JSPS KAKENHI [JP15K17640]
  16. ICREA Funding Source: Custom
  17. Grants-in-Aid for Scientific Research [16K05291, 15K17640] Funding Source: KAKEN

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On 2015 June 16, Fermi- LAT observed a giant outburst from the flat spectrum radio quasar 3C 279 with a peak >100 MeV flux of similar to 3.6 x 10(-5) photons cm(-2) s(-1), averaged over orbital period intervals. It is historically the highest gamma-ray flux observed from the source, including past EGRET observations, with the gamma-ray isotropic luminosity reaching similar to 10(49) erg s(-1). During the outburst, the Fermi spacecraft, which has an orbital period of 95.4 minutes, was operated in a special pointing mode to optimize the exposure for 3C 279. For the first time, significant flux variability at sub-orbital timescales was found in blazar observations by Fermi- LAT. The source flux variability was resolved down to 2-minute binned timescales, with flux doubling times of less than 5 minutes. The observed minute-scale variability suggests a very compact emission region at hundreds of Schwarzschild radii from the central engine in conical jet models. A minimum bulk jet Lorentz factor (Gamma) of 35 is necessary to avoid both internal gamma-ray absorption and super-Eddington jet power. In the standard external radiation Comptonization scenario, G should be at least 50 to avoid overproducing the synchrotron self-Compton component. However, this predicts extremely low magnetization (similar to 5 x 10(-4)). Equipartition requires Gamma as high as 120, unless the emitting region is a small fraction of the dissipation region. Alternatively, we consider. rays originating as synchrotron radiation of gamma e similar to 1.6 x 10(6) electrons, in a magnetic field B similar to 1.3 kG, accelerated by strong electric fields E similar to B in the process of magnetoluminescence. At such short distance scales, one cannot immediately exclude the production of gamma-rays in hadronic processes.

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