TY - JOUR
T1 - Jet simulations and gamma-ray burst afterglow jet breaks
AU - van Eerten, H. J.
AU - Meliani, Z.
AU - Wijers, R.A.M.J.
AU - Keppens, R.
PY - 2010
Y1 - 2010
N2 - The conventional derivation of the gamma-ray burst afterglow jet break time uses only the blast
wave fluid Lorentz factor and therefore leads to an achromatic break. We show that in general
gamma-ray burst afterglow jet breaks are chromatic across the self-absorption break. Depending
on circumstances, the radio jet break may be postponed significantly. Using high-accuracy
adaptive mesh fluid simulations in one dimension, coupled to a detailed synchrotron radiation
code, we demonstrate that this is true even for the standard fireball model and hard-edged jets.
We confirm these effects with a simulation in two dimensions. The frequency dependence of
the jet break is a result of the angle dependence of the emission, the changing optical depth in
the self-absorbed regime and the shape of the synchrotron spectrum in general. In the optically
thin case the conventional analysis systematically overestimates the jet break time, leading to
inferred opening angles that are underestimated by a factor of ∼1.3 and explosion energies
that are underestimated by a factor of ∼1.7, for explosions in a homogeneous environment.
The methods presented in this paper can be applied to adaptive mesh simulations of arbitrary
relativistic fluid flows. All analysis presented here makes the usual assumption of an on-axis
observer.
AB - The conventional derivation of the gamma-ray burst afterglow jet break time uses only the blast
wave fluid Lorentz factor and therefore leads to an achromatic break. We show that in general
gamma-ray burst afterglow jet breaks are chromatic across the self-absorption break. Depending
on circumstances, the radio jet break may be postponed significantly. Using high-accuracy
adaptive mesh fluid simulations in one dimension, coupled to a detailed synchrotron radiation
code, we demonstrate that this is true even for the standard fireball model and hard-edged jets.
We confirm these effects with a simulation in two dimensions. The frequency dependence of
the jet break is a result of the angle dependence of the emission, the changing optical depth in
the self-absorbed regime and the shape of the synchrotron spectrum in general. In the optically
thin case the conventional analysis systematically overestimates the jet break time, leading to
inferred opening angles that are underestimated by a factor of ∼1.3 and explosion energies
that are underestimated by a factor of ∼1.7, for explosions in a homogeneous environment.
The methods presented in this paper can be applied to adaptive mesh simulations of arbitrary
relativistic fluid flows. All analysis presented here makes the usual assumption of an on-axis
observer.
U2 - 10.1111/j.1365-2966.2010.17582.x
DO - 10.1111/j.1365-2966.2010.17582.x
M3 - Article
SN - 0035-8711
VL - 410
SP - 2016
EP - 2024
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 3
ER -