1999ApJ...519..556W


Query : 1999ApJ...519..556W

1999ApJ...519..556W - Astrophys. J., 519, 556-562 (1999/July-2)

Analytic model of spectral variability of blazars at high frequencies. I. Radiative losses.

WANG J., QIAN T., CEN X. and XU J.

Abstract (from CDS):

The evolution of the relativistic electron spectrum in a homogeneous jet due to the injection of fresh relativistic electrons, radiation losses, and particle escape is considered and applied to the interpretation of the spectral variability of blazars at high frequencies. The idea of wide and narrow injected electron spectra is discussed. The synchrotron spectra for wide and narrow injected electron spectra are calculated, taking into account radiation losses and electron escape. It is pointed out that the narrow electron spectrum can give rise to a lag of the emitting spectra between in soft and hard photons that approximately satisfies a ν–1/2 relation, and the wide electron spectrum will produce no peak delay and a largely differing variability of the emitting spectra at high frequencies; the timescale of the spectral delay is also proportional to ν–1/2. In the case of PKS 2155-304, it is concluded that the flares at UV through X-ray wavelengths in 1994 May can be attributed to a sudden injection of high-energy electrons with a narrow spectrum. In the case of Mrk 421, it is suggested that the TeV flare can be attributed to an injection of electrons with a narrow spectrum through synchrotron self-Compton emission and to the X-ray flare as the source of soft photons.

Abstract Copyright: ∼

Journal keyword(s): Galaxies: Jets - Radiation Mechanisms: Nonthermal - X-Rays: Bursts - X-Rays: Galaxies

Simbad objects: 3

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Number of rows : 3
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 Z 184-50 BLL 11 04 27.3140835504 +38 12 31.798495872   13.50 12.90 8.31   ~ 2841 1
2 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3205 2
3 PKS J2158-3013 BLL 21 58 52.0652249880 -30 13 32.118447792   13.36 13.09 12.62   ~ 1829 1

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