The Hard X-ray Emission of Cen A
  The radio galaxy Cen A has been detected all the way up to the TeV energy
range. This raises the question about the dominant emission mechanisms in the
high-energy domain. Spectral analysis allows us to put constraints on the
possible emission processes. Here we study the hard X-ray emission as measured
by INTEGRAL in the 3-1000 keV energy range, in order to distinguish between a
thermal and non-thermal inverse Compton process. The hard X-ray spectrum of Cen
A shows a significant cut-off at energies Ec = 434 (+106 -73) keV with an
underlying power law of photon index 1.73 +- 0.02. A more physical model of
thermal Comptonisation (compPS) gives a plasma temperature of kT = 206+-62 keV
within the optically thin corona with Compton parameter y = 0.42 (+0.09 -0.06).
The reflection component is significant at the 1.9 sigma level with R = 0.12
(+0.09 -0.10), and a reflection strength R>0.3 can be excluded on a 3 sigma
level. Time resolved spectral studies show that the flux, absorption, and
spectral slope varied in the range f(3-30 keV) = (1.2 - 9.2)e-10 erg/cm**2/s,
NH = (7 - 16)e22 1/cm**2, and photon index 1.75 - 1.87. Extending the cut-off
power law or the Comptonisation model to the gamma-ray range shows that they
cannot account for the high-energy emission. On the other hand, also a broken
or curved power law model can represent the data, therefore a non-thermal
origin of the X-ray to GeV emission cannot be ruled out. The analysis of the
SPI data provides no sign of significant emission from the radio lobes and
gives a 3 sigma upper limit of f(40-1000 keV) < 0.0011 ph/cm**2/s. While
gamma-rays, as detected by CGRO and Fermi, are caused by non-thermal (jet)
processes, the main process in the hard X-ray emission of Cen A is still not
unambiguously determined, being either dominated by thermal inverse Compton
emission, or by non-thermal emission from the base of the jet.
