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ULF wave effects on high frequency signal propagation through the ionosphere

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Figure

Fig. 1.171  f6kULF wave fields at L=1.6 for local midday summer. Thesolid lines are the X (north-south), the dotted lines are the Y (east-west) and the dashed lines are the Z (vertical) ULF field com-ponents
Fig. 2. ULF wave fields at L=2.4 for local midday winter (NorthHemisphere). The solid lines are the X (north-south), the dottedlines are the Y (east-west) and the dashed lines are the Z (vertical)ULF field components
Fig. 3. ULF wave fields at L=2.4 for early morning (06:00 LT) win-ter (North Hemisphere)
Fig. 4.The differential phases for noon and summer at L=1.6(South Hemisphere) for a 70 MHz signal due to changes in TECfrom a 50 mHz ULF wave as a function of the ULF wave spatialscale size

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