Title: Location of the TEVemitting region in PKS 2155304
1Location of the TEV-emitting region in PKS
2155-304
- Geoff Bicknell
- Research School of Astronomy Astrophysics
- Australian National University
- Stefan Wagner
- Landessternwarte
- University of Heidelberg
2Variability of PKS 2155-304
3Where is the emitting region?
If the emitting region is close to the black hole
then conventional values of Doppler factor 10
may be OK
If the emitting region 1016 cm in size then
Doppler factor may be 100
4Absorption of Gamma Rays by pair production
- Jet irradiated by emission from accretion disk
gt Pair production - Complicated by fact that radiation from disk can
be reduced by power in disk wind
5Pair production from photon-photon collisions
Threshold energy
Minimum threshold
6Calculation of pair opacity
7Pair opacity (Gould Schreder, 1967 Donea
Protheroe, 2003)
8Disk spectrum
Kinetic power of Poynting flux dominated jet (GB
Li, 2008 Kuncic GB, 2004)
Shakura-Sunyaev disk temperature
9Accretion rate
Jet power
Begelman, Fabian Rees (2008)
Estimates from prior models (e.g Aharonian, Sol
et al.)
10Results
11Turbulent jets (3D Simulations by Toby Potter)
Density
Pressure
Mach 1 turbulent jets illustrate the formation of
shocks and high pressure (high emissivity)
regions in turbulent flow
122 component models
Increased emission in GeV - TeV range
13Main points
- TeV (and lower energy) photons strongly absorbed
near accretion disk - Relative opacity depends on height gt Spectral
index of moving blob would change when
propagating away from the black hole - One way to avoid significant opacity is for the
disk emission to be strongly suppressed (e.g. by
diversion of energy into a wind)
14- 2 component models may possibly get around some
of the problems associated with one-zone models - Inidcations are that emission in the GLAST energy
range will be more significant