A Structured Leptonic Jet Model of the "Orphan" TeV Gamma-Ray Flares in TeV Blazars
arXiv:astro-ph/0607063 · doi:10.1086/507403
Abstract
The emission spectra of TeV blazars extend up to tens of TeV and the emission mechanism of the TeV -rays is explained by synchrotron self-Compton scattering in leptonic models. In these models the time variabilities of X-rays and TeV -rays are correlated. However, recent observations of 1ES 1959+650 and Mrk 421 have found the ``orphan'' TeV -ray flares, i.e., TeV -ray flares without simultaneous X-ray flares. In this paper we propose a model for the ``orphan'' TeV -ray flares, employing an inhomogeneous leptonic jet model. After a primary flare that accompanies flare-up both in X-rays and TeV -rays, radiation propagates in various directions in the comoving frame of the jet. When a dense region in the jet receives the radiation, X-rays are scattered by relativistic electrons/positrons to become TeV -rays. These -ray photons are observed as an ``orphan'' TeV -ray flare. The observed delay time between the primary and ``orphan'' flares is about two weeks and this is accounted for in our model for parameters such as , cm, , and , where is the bulk Lorentz factor of the jet, is the distance between the central black hole and the primary flare site, is the angle between the jet axis and the direction of the motion of the dense region that scatters incoming X-rays produced by the primary flare, and is the angle between the jet axis and the line of sight.
arXiv comment12page, 6 figures, accepted by ApJ
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- Baryon Loading Efficiency and Particle Acceleration Efficiency of Relativistic Jets: Cases For Low Luminosity BL Lacs
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- The Study of TeV Variability and Duty Cycle of Mrk 421 from 3 Years of Observations with the Milagro Observatory
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- CANGAROO-III Observations of the 2006 Outburst of PKS2155-304
- Could a plasma in quasi-thermal equilibrium be associated to the "orphan" TeV flares ?
- A Ring of Fire Orphan γ-Ray Flare in the Neutrino Candidate 3C 120