2010ApJ...712.1232W


Query : 2010ApJ...712.1232W

2010ApJ...712.1232W - Astrophys. J., 712, 1232-1240 (2010/April-1)

Klein-nishina effects on the high-energy afterglow emission of gamma-ray bursts.

WANG X.-Y., HE H.-N., LI Z., WU X.-F. and DAI Z.-G.

Abstract (from CDS):

Extended high-energy (≳100 MeV) gamma-ray emission that lasts much longer than the prompt sub-MeV emission has been detected from quite a few gamma-ray bursts (GRBs) by Fermi-Large Area Telescope (LAT) recently. A plausible scenario is that this emission is the afterglow synchrotron emission produced by electrons accelerated in the forward shocks. In this scenario, the electrons that produce synchrotron high-energy emission also undergo inverse Compton (IC) loss and the IC scattering with the synchrotron photons should be in the Klein-Nishina (KN) regime. Here we study effects of the KN scattering on the high-energy synchrotron afterglow emission. We find that at early times the KN suppression effect on those electrons that produce the high-energy emission is usually strong and therefore their IC loss is small with a Compton parameter Y ≲ a few for a wide range of parameter space. This leads to a relatively bright synchrotron afterglow at high energies that can be detected by Fermi-LAT. As the KN suppression effect weakens with time, the IC loss increases and could dominate over the synchrotron loss in some parameter spaces. This will lead to a faster temporal decay of the high-energy synchrotron emission than is predicted by the standard synchrotron model, which may explain the observed rapid decay of the early high-energy gamma-ray emission in GRB090510 and GRB090902B.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - radiation mechanisms: non-thermal

Simbad objects: 5

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Number of rows : 5
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
2 GRB 080825C gB 15 28.8 -04 54           ~ 71 0
3 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
4 4B 941017 gB 20 06.2 +09 49           ~ 93 0
5 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0

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