Abstract

We study the contribution of thermal and non-thermal processes to the inverse Compton emission of the radio galaxy M 87 by modelling its broad-band emission. Through this we aim to derive insight into where within the AGN the X-ray, gamma-ray, and VHE emission is produced. We have analysed all available INTEGRAL IBIS/ISGRI data on M 87, spanning almost 10 years, to set an upper limit to the average hard X-ray flux of f(20−60 keV)<3×10−12f(20 - 60 \rm \, keV) < 3\times 10^{-12}  erg cm−2 s−1\rm \, erg \, cm^{-2} \, s^{-1}, using several techniques beyond the standard analysis which are also presented here. We also analysed hard X-ray data from Suzaku/PIN taken late November 2006, and we report the first hard X-ray detection of M 87 with a flux of f(20−60 keV)=10−11 erg cm−2 s−1f(20 - 60 \rm \, keV) = 10^{-11}\rm \, erg \, cm^{-2} \, s^{-1} . In addition we analyse data from Fermi/LAT, INTEGRAL/JEM-X, and Suzaku/XIS. We collected historical radio/IR/optical and VHE data and combined them with the X-ray and gamma-ray data, to create broad-band spectral energy distributions for the average low-flux state and the flaring state. The resulting spectral energy distributions are modelled by applying a single-zone SSC model with a jet angle of theta = 15 degrees. We also show that modelling the core emission of M 87 using a single-zone synchrotron self-Compton model does represent the SED, suggesting that the core emission is dominated by a BL Lac type AGN core. Using SED modelling we also show that the hard X-ray emission detected in 2006 is likely due to a flare of the jet knot HST-1, rather than being related to the core.

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