Astron. Astrophys. 324, 395-409 (1997)
4. The -ray photosphere
We now discuss the initial height of a plasma blob from which TeV
-ray emission as observed from Mrk 421 can
escape freely. Since BL Lac objects have very dilute emission line
clouds, backscattering of accretion disk radiation into the trajectery
of emitted -rays is negligible.
Then, the optical depth for a photon of dimensionless energy
, emitted at height due
to interaction with accretion disk radiation is calculated as
![[EQUATION]](img209.gif)
![[EQUATION]](img210.gif)
where is the differential number of
accretion disk photons at height z, is
the pair production cross section
![[EQUATION]](img213.gif)
![[EQUATION]](img214.gif)
![[EQUATION]](img215.gif)
and we assumed for simplicity that the -ray
is emitted along the symmetry axis. The result for different injection
heights is illustrated in Fig. 6. and shows
that the -ray photosphere for
-rays of energy 500 GeV - 1 TeV is located
slightly above pc in the case of an accretion
disk of luminosity erg s-1.
![[FIGURE]](img219.gif) |
Fig. 6. Pair production optical depth for high-energy -rays, emitted at different heights ( ), interacting with direct accretion disk radiation ( erg/s, )
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© European Southern Observatory (ESO) 1997
Online publication: May 26, 1998
helpdesk.link@springer.de  |