2010ApJ...722..235V


Query : 2010ApJ...722..235V

2010ApJ...722..235V - Astrophys. J., 722, 235-247 (2010/October-2)

Off-axis gamma-ray burst afterglow modeling based on a two-dimensional axisymmetric hydrodynamics simulation.

VAN EERTEN H., ZHANG W. and MacFADYEN A.

Abstract (from CDS):

Starting as highly relativistic collimated jets, gamma-ray burst outflows gradually slow down and become nonrelativistic spherical blast waves. Although detailed analytical solutions describing the afterglow emission received by an on-axis observer during both the early and late phases of the outflow evolution exist, a calculation of the received flux during the intermediate phase and for an off-axis observer requires either a more simplified analytical model or direct numerical simulations of the outflow dynamics. In this paper, we present light curves for off-axis observers covering the long-term evolution of the blast wave, calculated from a high-resolution two-dimensional relativistic hydrodynamics simulation using a synchrotron radiation model. We compare our results to earlier analytical work and calculate the consequence of the observer angle with respect to the jet axis both for the detection of orphan afterglows and for jet break fits to the observational data. We confirm earlier results in the literature finding that only a very small number of local type Ibc supernovae can harbor an orphan afterglow. For off-axis observers, the observable jet break can be delayed up to several weeks, potentially leading to overestimation of the beaming-corrected total energy. In addition we find that, when using our off-axis light curves to create synthetic Swift X-ray data, jet breaks are likely to remain hidden in the data.

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Journal keyword(s): acceleration of particles - gamma-ray burst: general - hydrodynamics - methods: numerical - relativistic processes - shock waves

Simbad objects: 10

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Number of rows : 10
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 050904 gB 00 54 50.794 +14 05 09.42           ~ 496 0
2 SN 1984L SN* 02 35 30.54 -07 09 30.3   14.0       SNIb 197 1
3 GRB 070125 gB 07 51 17.80 +31 09 04.8           ~ 188 0
4 GRB 080916C gB 07 59 23.24 -56 38 16.8           ~ 386 0
5 SN 1954A SN* 12 15 45 +36 16.2   9.3       SNIb 104 1
6 SN 1991D SN* 13 41 13.58 -14 38 47.6     16.4     SNIb 35 1
7 GRB 080319B gB 14 31 41.04 +36 18 09.2           ~ 508 0
8 GRB 080721A gB 14 57 55.76 -11 43 24.9           ~ 180 0
9 Fermi bn090902462 gB 17 39 45.26 +27 19 28.1           ~ 440 0
10 Fermi bn090926181 gB 23 33 36.18 -66 19 25.9           ~ 339 0

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