The decay of the magnetospheric ring current during geomagnetic disturbances is associated with numerous processes. Particle precipitation is related to Coulomb collisions and ion-cyclotron instability owing to the interaction of hot protons of the ring current and cold particles of the outer plasmasphere (Cole, 1975;Cornwall et al., 1971). This decay tends to occur in the recovery phase of the geomagnetic disturbance when the expanding plasmasphere overlaps with the low-latitude fraction of the ring current. In other words, the most intense decay of the ring current occurs at the latitudes of the plasmapause. The precipitation of hot particles and heat flow owing to thermal conductivity, directed along the lines of the force, heat the ionosphere at the heights of the F2 layer. Because of ionospheric heating, an intense electron temperature (Te) peak and a stable auroral red (SAR) arc are formed (Hoch, 1973;Ievenko & Alekseev, 2004;Kozyra et al., 1986). The heating of the ionosphere also increases the recombination, inducing the formation of an ionization trough (Pavlov, 1996). Thus, the plasmapause, Te peak, SAR arc, and ionospheric trough are interrelated structures, at least during the recovery phase of a storm/substorm.