The polar lower ionosphere is distinguished by its variability due to various effects of solar activity. They result in the appearance of sporadic E S structures, in excitation of the broad spectrum of plasma inhomogeneities, and in variations of the electron concentration. The goal of the present study is to reveal regularities in the variations of the night-side polar lower ionosphere on the basis of radio wave measurements on links from navigation GPS satellites to CHAMP satellite. These ionosphere variations are stipulated by the effect of the flare solar activity. To this end, it was necessary to determine the altitude profiles of the electron concentration N e ( h ) and to find the characteristics of both sporadic E S structures and plasma inhomogeneities. We used the data of 327 radio occultation events of the night side polar ionosphere in regions of latitudes higher than 65° N for the time period from October 25 to November 9, 2003, when particularly strong solar activity was observed. In the radio occultation events of the ionosphere, we have registered the amplitude E and the increments of the phase path ψ for two coherent signals with the frequencies of f 1 = 1.5 GHz and f 2 = 1.2 GHz [1‐3]. In order to determine the excitation degree for small-scale inhomogeneity of the ionosphere plasma, we analyzed random fluctuations of the radio-wave amplitude δ E . These fluctuations were subjected to the standard procedure of statistical processing in order to obtain the root-mean-square amplitude deviation σ . The fluctuations δ E are caused mostly by plasma inhomogeneities located in the ionosphere F region at altitudes h ≈ 200–300 km. The analysis of these fluctuations has shown that the quantity σ is subjected to variations with the minimum values being σ min ≈ 1 .5% and with the maximum fluctuation level attaining 20%. In Fig. 1, dots indicate values of root-mean-square deviations σ for the fluctuations of the amplitude E , which were registered within the period of October 26 to November 9, 2003 (measurement dates are indicated at the horizontal axis). In the beginning of this period, the fluctuation intensity attained σ ≈ 2%, whereas later, on October 27, an increase in the fluctuations was observed. The maximum of the field-intensity fluctuations took place on October 29, 30, and 31 when σ attained 10‐14%. Starting from November 1, the fluctuation intensity began to decrease, and on November 4, elevated values of σ were recorded again. In order to determine the amplitude fluctuations σ A more objectively, we have excluded the slight effect of continually present small fluctuations with σ min = 1.5%. We have used here the relationship = σ 2 – and have realized smoothing the dependence as a function of time by the sliding mean technique with time interval 6-hour.
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