III-nitride light-emitting diodes (LEDs) and laser diodes (LDs) are ultimately limited in performance due to parasitic Auger recombination. For LEDs, the consequences are poor efficiencies at high current densities; for LDs, the consequences are high thresholds and limited efficiencies. Here, we present arguments for III-nitride quantum dots (QDs) as active regions for both LEDs and LDs, to circumvent Auger recombination and achieve efficiencies at higher current densities that are not possible with quantum wells. QD-based LDs achieve gain and thresholds at lower carrier densities before Auger recombination becomes appreciable. QD-based LEDs achieve higher efficiencies at higher currents because of higher spontaneous emission rates and reduced Auger recombination. The technical challenge is to control the size distribution and volume of the QDs to realize these benefits. If constructed properly, III-nitride light-emitting devices with QD active regions have the potential to outperform quantum well lightemitting devices, and enable an era of ultra-efficient solid-state lighting.diffusion lengths limit the carrier filling uniformity. The unfortunate reality is that, despite much effort, QW-based III-nitride LEDs are still only very efficient at lower current densities. Therefore, to further advance solid-state lighting (SSL) efficiency other (non-QW) solutions may be necessary.III-nitride laser diodes (LDs) have also achieved impressive peak PCEs of ß40% [15][16][17], and are gaining interest as an alternative source for SSL. They have many attributes that make them interesting for SSL [8,18] including system and cost benefits [2,18] and an ability for phosphor-converted LDs (pc-LDs) to produce white light with the same color rendering and color temperature as pc-LEDs [19][20][21][22]. Most interesting, in contrast to LEDs, LD operate under stimulated emission after lasing threshold, and parasitic recombination processes such as Auger are clamped at threshold. The result is III-nitride LDs have higher PCEs at much higher current densities than LEDs, and are a potential way to overcome efficiency droop [8]. Indeed, projections of the efficiency of QW-based LDs suggest they could achieve peak PCEs of ß70% which vastly exceed those of LEDs at high current densities [8]. However, peak PCEs of LDs are not as high as the 84% peak PCEs of LEDs, in large part because high thresholds from Auger recombination results in a peak PCE at very high C