2011ApJ...733...22H


Query : 2011ApJ...733...22H

2011ApJ...733...22H - Astrophys. J., 733, 22 (2011/May-3)

On the high-energy emission of the short GRB 090510.

HE H.-N., WU X.-F., TOMA K., WANG X.-Y. and MESZAROS P.

Abstract (from CDS):

Long-lived high-energy (>100 MeV) emission, a common feature of most Fermi-LAT-detected gamma-ray burst, is detected up to ∼102 s in the short GRB 090510. We study the origin of this long-lived high-energy emission, using broadband observations including X-ray and optical data. We confirm that the late >100 MeV, X-ray, and optical emission can be naturally explained via synchrotron emission from an adiabatic forward shock propagating into a homogeneous ambient medium with low number density. The Klein-Nishina effects are found to be significant, and effects due to jet spreading and magnetic field amplification in the shock appear to be required. Under the constraints from the low-energy observations, the adiabatic forward shock synchrotron emission is consistent with the later-time (t ≳ 2 s) high-energy emission, but falls below the early-time (t < 2 s) high-energy emission. Thus we argue that an extra high-energy component is needed at early times. A standard reverse-shock origin is found to be inconsistent with this extra component. Therefore, we attribute the early part of the high-energy emission (t ≲ 2 s) to the prompt component, and the long-lived high-energy emission (t ≳ 2 s) to the adiabatic forward shock synchrotron afterglow radiation. This avoids the requirement for an extremely high initial Lorentz factor.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - gamma-ray burst: individual: GRB 090510 - 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 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
3 Fermi bn081024891 gB 21 31 36.00 +21 12 14.4           ~ 91 0
4 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
5 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0

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