The Astrophysical Journal Letters · 2016 · 259 citations · 47 references
Natural SciencesAstronomyPhysicsAstrophysicsObservational AstronomyRadio AstronomyExtragalactic Gamma-ray AstronomyGamma-ray BurstsGamma-ray SourcesGround-based Gamma-ray ObservatoriesHigh-energy Astrophysical SourcesSpace-based Gamma-ray ObservatoriesFlux MeasurementFlux Variability AnalysisGamma-ray Burst ObservationsGamma-ray Emission From The Galactic Center RegionOrbital PeriodTiming Of Gamma-ray Bursts
ABSTRACT 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 ∼3.6 × 10 −5 photons cm −2 s −1 , averaged over orbital period intervals. It is historically the highest γ -ray flux observed from the source, including past EGRET observations, with the γ -ray isotropic luminosity reaching ∼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 (Γ) of 35 is necessary to avoid both internal γ -ray absorption and super-Eddington jet power. In the standard external radiation Comptonization scenario, Γ should be at least 50 to avoid overproducing the synchrotron self-Compton component. However, this predicts extremely low magnetization (∼5 × 10 −4 ). Equipartition requires Γ as high as 120, unless the emitting region is a small fraction of the dissipation region. Alternatively, we consider γ rays originating as synchrotron radiation of γ e ∼ 1.6 × 10 6 electrons, in a magnetic field B ∼ 1.3 kG, accelerated by strong electric fields E ∼ B in the process of magnetoluminescence. At such short distance scales, one cannot immediately exclude the production of γ -rays in hadronic processes.
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