TY - JOUR
T1 - Time-dependent models for blazar emission with the second-order fermi acceleration
AU - Asano, Katsuaki
AU - Takahara, Fumio
AU - Kusunose, Masaaki
AU - Toma, Kenji
AU - Kakuwa, Jun
PY - 2014/1/1
Y1 - 2014/1/1
N2 - The second-order Fermi acceleration (Fermi-II) driven by turbulence may be responsible for the electron acceleration in blazar jets. We test this model with time-dependent simulations. The hard electron spectrum predicted by the Fermi-II process agrees with the hard photon spectrum of 1ES 1101-232. For other blazars that show softer spectra, the Fermi-II model requires radial evolution of the electron injection rate and/or diffusion coefficient in the outflow. Such evolutions can yield a curved electron spectrum, which can reproduce the synchrotron spectrum of Mrk 421 from the radio to the X-ray regime. The photon spectrum in the GeV energy range of Mrk 421 is hard to fit with a synchrotron self-Compton model. However, if we introduce an external radio photon field with a luminosity of 4.9 × 1038 erg s-1, GeV photons are successfully produced via inverse Compton scattering. The temporal variability of the diffusion coefficient or injection rate causes flare emission. The observed synchronicity of X-ray and TeV flares implies a decrease of the magnetic field in the flaring source region.
AB - The second-order Fermi acceleration (Fermi-II) driven by turbulence may be responsible for the electron acceleration in blazar jets. We test this model with time-dependent simulations. The hard electron spectrum predicted by the Fermi-II process agrees with the hard photon spectrum of 1ES 1101-232. For other blazars that show softer spectra, the Fermi-II model requires radial evolution of the electron injection rate and/or diffusion coefficient in the outflow. Such evolutions can yield a curved electron spectrum, which can reproduce the synchrotron spectrum of Mrk 421 from the radio to the X-ray regime. The photon spectrum in the GeV energy range of Mrk 421 is hard to fit with a synchrotron self-Compton model. However, if we introduce an external radio photon field with a luminosity of 4.9 × 1038 erg s-1, GeV photons are successfully produced via inverse Compton scattering. The temporal variability of the diffusion coefficient or injection rate causes flare emission. The observed synchronicity of X-ray and TeV flares implies a decrease of the magnetic field in the flaring source region.
KW - acceleration of particles
KW - BL Lacertae objects: individual (1ES 1101-232, Mrk 421)
KW - radiation mechanisms: non-thermal
KW - turbulence
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U2 - 10.1088/0004-637X/780/1/64
DO - 10.1088/0004-637X/780/1/64
M3 - Article
AN - SCOPUS:84890478046
SN - 0004-637X
VL - 780
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 64
ER -