A magnetospheric substorm is a process where magnetic flux and energy stored in the magnetotail lobes are unloaded by reconnection in the near-Earth tail, causing a global reconfiguration of the magnetosphere (Hones, 1979; review by Baker et al., 1996). The shape of the magnetotail changes from a stretched configuration to a more dipolar configuration during the unloading, and a field-aligned current system, known as the substorm current wedge, develops near midnight (McPherron et al., 1973; review by Kepko et al., 2015). The current wedge closes in the ionosphere, leading to an enhancement of the westward electrojet. This enhancement causes a pronounced negative bay in the northward component of magnetometers in the auroral zone, a signature that is directly linked to the auroral substorm, as first described by Akasofu (1964). The auroral substorm starts with an onset, which is a sudden, localized brightening of the aurora, typically located at the equatorial boundary of the discrete aurora. The intensified region then expands, both longitudinally and poleward; this period of the substorm is referred to as the expansion phase. The expansion phase is followed by a recovery phase, in which the magnetospheric system slowly reverts toward its preonset