“…In general, R Auger is more significant at the high current densities, while R SRH is dominant at the low current densities (thus, under general operating conditions of micro-LED devices). In view of the high perimeter-to-area ratios of micro-LEDs, the trap-assisted surface non-radiative recombination occurring at mesa surfaces was also considered [ 3 ], setting the trap levels 0.46 eV above the valence band and 0.24 eV below the conduction band [ 25 ], and setting the surface recombination velocities (SRVs) for both electrons and holes ( v s,n and v s,p , respectively) around 1000 cm/s ( Table 1 ) [ 13 ]. Through electrical simulation under different biases, the spatial distributions of carrier concentrations, current flows, various recombination rates, and spontaneous emission rates as a function of bias, J–V characteristics, and electroluminescence (EL) and IQE as a function of bias can be analyzed.…”