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  • STAR-JET INTERACTIONS AND G...
    Khangulyan, D V; BARKOV, M V; Bosch-Ramon, V; Aharonian, F A; DORODNITSYN, A V

    The Astrophysical journal, 09/2013, Letnik: 774, Številka: 2
    Journal Article

    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 (a red giant) crosses the jet close to the central black hole. The study includes an analytical treatment of the evolution of the envelope lost by the star within the jet, and calculations of the related high-energy radiation. The model readily explains the day-long that varies on timescales of hours, GeV gamma-ray flare from 3C454.3, observed during 2010 November on top of a plateau lasting weeks. In the proposed scenario, the plateau state is caused by a strong wind generated by the heating of the stellar atmosphere due to 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 sub(BH) Asymptotically = to 10 super(9) M sub(middot in circle), the total jet power: L sub(j) Asymptotically = to 10 super(48) erg s super(-1), and the Doppler factor of the gamma-ray emitting clouds: delta Asymptotically = to20. 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 directlyaccelerated electrons. An injected proton distribution is proportional to E super(-1) or harder below the relevant energies would be favored to alleviate the tight energetic constraints and to avoid the violation of the observational low-energy constraints.