Jonathan Granot, Tsvi Piran
The dynamics of GRB jets during the afterglow phase have an important effect
on the interpretation of their observations and for inferring key physical
parameters such as their true energy and event rate. Semi-analytic models
generally predict a fast lateral expansion, where the jet opening angle
asymptotically grows exponentially with its radius. Numerical simulations,
however, show a much more modest lateral expansion, where the jet retains
memory of its initial opening angle for a very long time, and the flow remains
non-spherical until it becomes sub-relativistic, and only then gradually
approaches spherical symmetry. Here we suggest a new analytic model based on a
new physically derived recipe for the lateral expansion. We also generalize the
model by relaxing the common approximations of ultra-relativistic motion and a
narrow jet opening angle. We find that the new analytic model fits much better
the results of numerical simulations, mainly because it remains valid also in
the mildly relativistic, quasi spherical regime. This model shows that for
modest initial jet half-opening angles, \theta_0, the outflow is not
sufficiently ultra-relativistic when its Lorentz factor reaches \Gamma =
1/\theta_0 and therefore the sideways expansion is rather slow, showing no
rapid, exponential phase. On the other hand, we find that jets with an
extremely narrow initial half-opening angle, of about \theta_0 << 10^{-1.5} or
so, which are still sufficiently ultra-relativistic at \Gamma = 1/\theta_0, do
show a phase of rapid, exponential lateral expansion. However, even such jets
that expand sideways exponentially are still not spherical when they become
sub-relativistic.
View original:
http://arxiv.org/abs/1109.6468
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