4.7 Article

LEPTONIC AND HADRONIC MODELING OF FERMI-DETECTED BLAZARS

Journal

ASTROPHYSICAL JOURNAL
Volume 768, Issue 1, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/0004-637X/768/1/54

Keywords

galaxies: active; galaxies: jets; gamma rays: galaxies; radiation mechanisms: non-thermal; relativistic processes

Funding

  1. South African Department of Science and Technology through the National Research Foundation under NRF SARChI Chair grant [64789]
  2. NASA through Astrophysics Theory Program Award [NNX10AC79G]
  3. Fermi Guest Investigator Grant [NNX09AT82G]
  4. Marie Curie IRG grant within the FP7 Program [248037]

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We describe new implementations of leptonic and hadronic models for the broadband emission from relativistic jets in active galactic nuclei in a temporary steady state. For the leptonic model, a temporary equilibrium between particle injection/acceleration, radiative cooling, and escape from a spherical emission region is evaluated, and the self-consistent radiative output is calculated. For the hadronic model, a temporary equilibrium between particle injection/acceleration, radiative and adiabatic cooling, and escape is evaluated for both primary electrons and protons. A new, semianalytical method to evaluate the radiative output from cascades initiated by internal gamma gamma pair production is presented. We use our codes to fit snapshot spectral energy distributions (SEDs) of a representative set of Fermi-LAT-detected blazars. We find that the leptonic model provides acceptable fits to the SEDs of almost all blazars with parameters close to equipartition between the magnetic field and the relativistic electron population. However, the hard gamma-ray spectrum of AO 0235+164, in contrast to the very steep IR-optical-UV continuum, poses a severe problem for the leptonic model. If charge neutrality in leptonic models is provided by cold protons, the kinetic energy carried by the jet should be dominated by protons. We find satisfactory representations of the snapshot SEDs of most blazars in our sample with the hadronic model presented here. However, in the case of two quasars the characteristic break at a few GeV energies cannot be well modeled. All of our hadronic model fits require powers in relativistic protons in the range L-p similar to 10(47)-10(49) erg s(-1).

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