The variability of ionospheric plasma in the polar regions is strongly related to complex coupling between the ionosphere and magnetosphere (Kamide & Baumjohann, 1993). Physical processes in the ionosphere such as plasma instabilities and turbulence can result in plasma structuring and irregularities at various scales. Such irregularities can in turn impact the propagation of trans-ionospheric radio waves through diffractive and refractive processes, and consequently lead to scintillations in the phase and amplitude of the received wave. Hence, the quality of services relying on radio signals, such as the Global Navigation Satellite Systems (GNSS) can be reduced. On the other hand, while monitoring such signals, one can infer the state of the ionosphere, and with supporting data, associate the plasma irregularities with physical processes in the ionosphere.A common approach to ionospheric scintillations is the phase screen model, which assumes a thin layer of irregularities that acts as a phase screen, where the wave propagation is disturbed by the Huygens principle. As the wave propagates further, scintillations can occur both in phase and amplitude (Yeh & Liu, 1982).For spatial scales of irregularities less than the radius of the first-Fresnel zone (r F = E L , where λ-is the wavelength of the signal and L-is the distance between the receiver and irregularity layer), both phase and amplitude scintillations are present. For the GNSS signals in the L-band, the Fresnel scale at 350 km altitude is ca. 360 m, but note that the effective Fresnel frequency is drift dependent (