High-latitude precipitation of charged particles is a crucial driver of ionospheric electrodynamics (e.g., Kivelson & Russell, 1995). These particles precipitate from the near-Earth plasma environment to form the aurora, and enhance the electrical conductance in the polar regions (e.g., Schunk & Nagy, 2009). Auroral precipitation is broadly defined into two types: diffuse and discrete aurora. Particles scattered into the loss cone by plasma waves create the diffuse aurora (Nishimura et al., 2020a and references therein). Diffuse particles precipitate into the upper atmosphere without the need of acceleration, and can consist of both electrons (e.g., Evans & Moore, 1979) and ions (e.g., Sergeev et al., 1983). Conversely, the discrete aurora is generated by particles that are accelerated into the ionosphere (e.g., Korth et al., 2014). These particles can be accelerated by geomagnetic field-aligned electric fields (monoenergetic; e.g., Evans, 1974;Knight, 1973) or by dispersive Alfvén waves (broadband; e.g., Chaston et al., 2003;Ergun et al., 1998). The conductance enhancements caused by auroral precipitation are important to investigative studies of magnetosphere-ionosphere coupling (e.g., Öztürk et al., 2020), since it regulates the closure of field-aligned currents (FACs;Iijima & Potemra, 1976) and maintain the nonlinear feedback