“…The drift‐bounce resonant condition for poloidal mode ULF waves can be described theoretically by Southwood et al () as where ω and m are the wave angular frequency and azimuthal wave number, respectively; ω d and ω b are the particle drift and bounce angular frequencies, respectively; N is an integer depending on the wave harmonic modes. For odd mode (e.g., fundamental mode, third harmonic mode), N = 0, ±2, ...; for even mode (e.g., second harmonic mode, fourth harmonic mode), N =± 1, ±3, ... (Ren et al, , ; Southwood & Kivelson, , ; Takahashi et al, ).…”