“…We consider a weakly ionized plasma in which (a10-alO-* + a,o-a,o-* + a,o- the increase in collision frequency; therefore, the absorption at crests is small and near troughs it is large; this pattern results in the overmodulation of the wave, whereas for the ordinary mode the absorption coefficient increases with the collision frequency; this pattern results in the demodulation of the wave. These results for the extraordinary mode are in qualitative agreement with the experimental results obtained by Bachynski and Gibbs [1969]. When the amplitude modulated wave is received at the ground after propagating a certain distance in the ionosphere, the extraordinary mode will be absorbed within 5 to 6 km of its propagation inside the ionosphere (owing to high absorption coefficient at gyroresonance) and only the ordinary mode will reach the receiver.…”