“…First, as electrons and low‐energy ions are magnetized above the collisional atmosphere, magnetic topology is important for characterizing energetic electron precipitation and low‐energy ion escape. More specifically, solar wind electrons and solar energetic particle electrons can precipitate along open field lines (e.g., Dubinin, Fraenz, Woch, Winnigham, et al, ; Dubinin, Fraenz, Woch, Roussos, et al, ; Lillis & Brain, ; Lillis et al, , , ; Xu et al, ), and ionospheric photoelectrons can precipitate onto the nightside atmosphere along cross‐terminator closed field lines (e.g., Liemohn et al, ; Ulusen et al, ; Xu, Mitchell, et al, ; Xu, Mitchell, Liemohn, et al, ), causing heating (e.g., Fox & Dalgarno, ; Sakai et al, ), ionization (e.g., Adams et al, ; Cui et al, ; Fillingim et al, , ; Xu, Mitchell, et al, ), and auroral emission (e.g., Bertaux et al, ; Brain et al, ; Haider et al, ; Leblanc et al, , ; Schneider et al, , ; Seth et al, ; Shane et al, ). At the same time, low‐energy ions can escape along open field lines (e.g., Ergun et al, ; Jakosky et al, ), accelerated partly by ambipolar electric fields (e.g., Collinson et al, ; Xu, Mitchell, et al, ), and on draped field lines through the J × B force and/or the convection electric field (e.g., Cravens et al, ; Fang et al, ; Halekas, Brain, et al, ).…”