2016
DOI: 10.1093/mnras/stw739
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Formation of very hard electron and gamma-ray spectra of flat-spectrum radio quasars in the fast-cooling regime

Abstract: In external Compton scenario, we investigate the formation of the very hard electron spectrum in the fast-cooling regime, using a time-dependent emission model. It is shown that a very hard electron distribution N ′ e (γ ′ ) ∝ γ ′ −p with the spectral index p ∼ 1.3 is formed below the minimum energy of injection electron when inverse Compton scattering takes place in the Klein-Nishina regime, i.e., inverse Compton scattering of relativistic electrons on broad-line region radiation in flat spectrum radio quasar… Show more

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Cited by 12 publications
(8 citation statements)
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References 63 publications
(86 reference statements)
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“…Furthermore, more physical processes could be considered instantly. For example, the scattering of electrons by various external radiation fields (Yan et al 2016) may also be an important cooling mechanism. Additionally, the electrons that are not efficiently accelerated (the low-energy electrons of Maxwellian distribution) may provide considerable lowenergy seed photons.…”
Section: Discussionmentioning
confidence: 99%
“…Furthermore, more physical processes could be considered instantly. For example, the scattering of electrons by various external radiation fields (Yan et al 2016) may also be an important cooling mechanism. Additionally, the electrons that are not efficiently accelerated (the low-energy electrons of Maxwellian distribution) may provide considerable lowenergy seed photons.…”
Section: Discussionmentioning
confidence: 99%
“…For the study of expected multi-wavelength variability in the internal-shock model, we first focus on Flare C (yellow in Figure 2), which is characterized by an almost unchanged Compton dominance compared to the quiescent state during period A. One natural interpretation is that this and other flares closely sample the accelerator/injector (e.g., Yan, Zhang & Zhang 2016). Therefore, such flaring behaviour can plausibly be reproduced by merely increasing the number of radiating non-thermal electrons generated by the shock, thus enhancing the synchrotron and EIC emission at the same rate.…”
Section: C 279 -Flare Cmentioning
confidence: 99%
“…A similar strategy, based on an analytical solution to the steady-state electron distribution, was adopted by Lewis et al [52], also requiring a significant reduction of the magnetic field to suppress a simultaneous optical synchrotron flare. Yan et al [53] modelled the orphan-flare SED using a time-dependent single-zone model with rapid electron cooling. However, it is unclear whether a transition from the quiescent to this flaring state may be produced in a natural way.…”
Section: Summary Discussion and Conclusionmentioning
confidence: 99%