One of the important phenomena of the equatorial and midlatitude ionosphere is the equatorial ionization anomaly (EIA). It forms as a consequence of the equatorial fountain effect (Appleton, 1946;Martyn, 1947;MITRA, 1946;Schunk & Nagy, 2000), caused by the upward vertical E × B/B 2 plasma drift that elevates the F region ionosphere plasma to higher altitudes over the magnetic equator, followed by diffusion along the geomagnetic field lines, that moves the plasma down and away from the equator, forming ionization crests in both sides of the magnetic equator and an ionization trough over the dip equator. The latitudinal plasma distribution that characterizes the EIA (a trough at the magnetic equator and two crests at approximately ±17° magnetic latitude) is well reproduced by many theoretical models (