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LEPTONIC AND HADRONIC MODELING OF<i>FERMI</i>-DETECTED BLAZARS

M. BöttcherCentre for Space Research, North-West University, Potchefstroom, 2531, South AfricaA. ReimerInstitut für Theoretische Physik, Universität Innsbruck, Technikerstraße 25, A-6020 Innsbruck, AustriaKevin Sweeney#N# Astrophysical Institute, Department of Physics and Astronomy, Ohio University, Athens, OH 45701, USAAbhishek Prakash#N# Astrophysical Institute, Department of Physics and Astronomy, Ohio University, Athens, OH 45701, USA
2013en
ABI

Аннотация

We describe new implementations of leptonic and hadronic models for the broadband emission from relativistic jets in AGN 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, semi-analytical method to evaluate the radiative output from cascades initiated by internal gamma-gamma pair production is presented. We use our codes to fit snap-shot spectral energy distributions 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 can not be well modelled. All of our hadronic model fits require powers in relativistic protons in the range L_p ~ 1e47 - 1e49 erg/s.

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