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Journal Article

Star-Jet Interactions and Gamma-Ray Outbursts from 3C454.3

MPS-Authors
http://pubman.mpdl.mpg.de/cone/persons/resource/persons37746

Barkov,  Maxim
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;
Space Research Institute RAS, 84/32 Profsoyuznaya Street, Moscow, 117997, Russia;

http://pubman.mpdl.mpg.de/cone/persons/resource/persons30244

Aharonian,  Felix A.
Division Prof. Dr. Werner Hofmann, MPI for Nuclear Physics, Max Planck Society;
Dublin Institute for Advanced Studies, 31 Fitzwilliam Place, Dublin 2, Ireland;

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1305.5117.pdf
(Preprint), 816KB

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Citation

Khangulyan, D. V., Barkov, M., Bosch-Ramon, V., Aharonian, F. A., & Dorodnitsyn, A. V. (2013). Star-Jet Interactions and Gamma-Ray Outbursts from 3C454.3. Astrophysical Journal, 774(2): 113. doi:10.1088/0004-637X/774/2/113.


Cite as: http://hdl.handle.net/11858/00-001M-0000-0014-6D2A-3
Abstract
We propose a model to explain the ultra-bright GeV gamma-ray flares observed from the blazar 3C454.3. The model is based on the concept of a relativistic jet interacting with compact gas condensations produced when a star (red giant) crosses the jet close to the central black hole. The study includes an analytical treatment of the evolution of the envelop lost by the star within the jet, and calculations of the related high-energy radiation. The model readily explains the day-long, variable on timescales of hours, GeV gamma-ray flare from 3C454.3, observed during November 2010 on top of a weeks-long plateau. In the proposed scenario, the plateau state is caused by a strong wind generated by the heating of the star atmosphere by nonthermal particles accelerated at the jet-star interaction region. The flare itself could be produced by a few clouds of matter lost by the red giant after the initial impact of the jet. In the framework of the proposed scenario, the observations constrain the key model parameters of the source, including the mass of the central black hole: $M_{\rm BH}\simeq 10^9 M_{\odot}$, the total jet power: $L_{\rm j}\simeq 10^{48}\,\rm erg\,s^{-1}$, and the Doppler factor of the gamma-ray emitting clouds, $\delta\simeq 20$. Whereas we do not specify the particle acceleration mechanisms, the potential gamma-ray production processes are discussed and compared in the context of the proposed model. We argue that synchrotron radiation of protons has certain advantages compared to other radiation channels of directly accelerated electrons.