We use high-resolution relativistic MHD simulations coupled with a radiative
transfer code to compute multiwavelength afterglow light curves of magnetized
ejecta of gamma-ray bursts interacting with a uniform circumburst medium. The
aim of our study is to determine how the magnetization of the ejecta at large
distance from the central engine influences the afterglow emission, and to
assess whether observations can be reliably used to infer the strength of the
magnetic field. We find that, for typical parameters of the ejecta, the
emission from the reverse shock peaks for magnetization σ0∼0.01−0.1 of the flow, and that it is greatly suppressed for higher σ0. The
emission from the forward shock shows an achromatic break shortly after the end
of the burst marking the onset of the self-similar evolution of the blast wave.
Fitting the early afterglow of GRB 990123 and 090102 with our numerical models
we infer respective magnetizations of σ0∼0.01 and σ0∼0.1 for these bursts. We argue that the lack of observed reverse shock
emission from the majority of the bursts can be understood if \sigma_0
\simmore 0.1, since we obtain that the luminosity of the reverse shock
decreases significantly for σ0∼1. For ejecta with \sigma_0
\simmore 0.1 our models predict that there is sufficient energy left in the
magnetic field, at least during an interval of ~10 times the burst duration, to
produce a substantial emission if the magnetic energy can be dissipated (for
instance, due to resistive effects) and radiated away.Comment: 9 pages, 9 figures. Submitted to MNRAS