TY - JOUR
T1 - On the high-energy emission of the short GRB090510
AU - He, Hao Ning
AU - Wu, Xue Feng
AU - Toma, Kenji
AU - Wang, Xiang Yu
AU - Mészáros, Peter
PY - 2011/5/20
Y1 - 2011/5/20
N2 - 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 GRB090510. 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.
AB - 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 GRB090510. 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.
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U2 - 10.1088/0004-637X/733/1/22
DO - 10.1088/0004-637X/733/1/22
M3 - Article
AN - SCOPUS:79956317695
SN - 0004-637X
VL - 733
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 22
ER -