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.

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

D'AMMANDO, FILIPPO;
2016

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 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.
2016
Ackermann M; Anantua R; Asano K; Baldini L; Barbiellini G; Bastieri D; Gonzalez JB; Bellazzini R; Bissaldi E; Blandford RD; Bloom ED; Bonino R; Bottacini E; Bruel P; Buehler R; Caliandro GA; Cameron RA; Caragiulo M; Caraveo PA; Cavazzuti E; Cecchi C; Cheung CC; Chiang J; Chiaro G; Ciprini S; Cohen-Tanugi J; Costanza F; Cutini S; DAmmando F; De Palma F; Desiante R; Digel SW; Di Lalla N; Di Mauro M; Di Venere L; Drell PS; Favuzzi C; Fegan SJ; Ferrara EC; Fukazawa Y; Funk S; Fusco P; Gargano F; Gasparrini D; Giglietto N; Giordano F; Giroletti M; Grenier IA; Guillemot L; Guiriec S; Hayashida M; Hays E; Horan D; Johannesson G; Kensei S; Kocevski D; Kuss M; La Mura G; Larsson S; Latronico L; Li J; Longo F; Loparco F; Lott B; Lovellette MN; Lubrano P; Madejski GM; Magill JD; Maldera S; Manfreda A; Mayer M; Mazziotta MN; Michelson PF; Mirabal N; Mizuno T; Monzani ME; Morselli A; Moskalenko IV; Nalewajko K; Negro M; Nuss E; Ohsugi T; Orlando E; Paneque D; Perkins JS; Pesce-Rollins M; Piron F; Pivato G; Porter TA; Principe G; Rando R; Razzano M; Razzaque S; Reimer A; Scargle JD; Sgro C; Sikora M; Simone D; Siskind EJ; Spada F; Spinelli P; Stawarz L; Thayer JB; Thompson DJ; Torres DF; Troja E; Uchiyama Y; Yuan Y; Zimmer S
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/595747
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