Owing to some refinements in the dynamics, we can follow the overall evolution of a realistic jet numerically until its bulk velocity is as small as βc ∼ 10-3c. We find no obvious break in the optical light curve during the relativistic phase itself. However, an obvious break does exist at the transition from the relativistic phase to the non-relativistic phase, which typically occurs at time t ∼ 106-106.5 s (i.e. 10-30 d). The break is affected by many parameters, such as the electron energy fraction ξe, the magnetic energy fraction ξ2B the initial half-opening angle θ0 and the medium number density n. Increasing any of them to a large enough value will make the break disappear. Although the break itself is parameter-dependent, afterglows from jetted GRB remnants are uniformly characterized by a quick decay during the non-relativistic phase, with power-law timing index a α ≥ 2.1. This is quite different from that of isotropic fireballs, and may be of fundamental importance for determining the degree of beaming in γ-ray bursts observationally.
CITATION STYLE
Huang, Y. F., Dai, Z. G., & Lu, T. (2000). On the optical light curves of afterglows from jetted gamma-ray burst ejecta: Effects of parameters. Monthly Notices of the Royal Astronomical Society, 316(4), 943–949. https://doi.org/10.1046/j.1365-8711.2000.03683.x
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