Fig. 5.

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Evolution of the light curve decay times in the simulations. Top: evolution of the decay time as a function of the anisotropy factor α, for emissions at 818 kHz. Bottom: evolution of the decay time as a function of the radio emission frequency (assuming fundamental emission) for an anisotropy factor of 0.3. On each plot, the decay time is determined at different angles from the radio source.

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