Infrared light-emitting diodes are currently fabricated from direct-gap semiconductors using epitaxy, which makes them expensive and difficult to integrate with other materials. Light-emitting diodes based on colloidal semiconductor quantum dots, on the other hand, can be solution-processed at low cost, and can be directly integrated with silicon 1 . However, so far, exciton dissociation and recombination have not been well controlled in these devices, and this has limited their performance [2][3][4][5][6][7][8] . Here, by tuning the distance between adjacent PbS quantum dots, we fabricate thin-film quantumdot light-emitting diodes that operate at infrared wavelengths with radiances (6.4 W sr 21 m 22 ) eight times higher and external quantum efficiencies (2.0%) two times higher than the highest values previously reported. The distance between adjacent dots is tuned over a range of 1.3 nm by varying the lengths of the linker molecules from three to eight CH 2 groups, which allows us to achieve the optimum balance between charge injection and radiative exciton recombination. The electroluminescent powers of the best devices are comparable to those produced by commercial InGaAsP light-emitting diodes. By varying the size of the quantum dots, we can tune the emission wavelengths between 800 and 1,850 nm.Colloidal quantum dots have been proposed for the development of low-temperature solution-processed quantum-dot devices, including next-generation photovoltaics, photodetectors and lightemitting diodes (LEDs) [1][2][3][4][5][6][7][8][9][10][11] . In particular, the development of high-power, efficient and low-cost infrared LEDs will further progress in applications such as night vision, optical communications and sensing. Early efforts to exploit quantum dots in LEDs were based on hybrid device structures in which the quantum dots were interfaced with conjugated polymers. Quantum dots with long capping ligands were either mixed with an organic host or directly sandwiched between organic carrier-transporting layers to form the LED structure 4,5,8 . The operating mechanism of such devices is based mainly on Förster transfer, in which exciton energy transfers from the organic host to the quantum dots by means of a dipole-dipole interaction. Owing to the long capping ligands and low carrier mobility of the organic materials, these devices suffer from low current density, charge injection imbalance and exciton ionization caused by large applied bias voltages 12 .Recently, an infrared quantum-dot LED based on direct exciton generation through carrier injection achieved 1.15% external quantum efficiency (EQE), but the organic carrier-injection layer limited the current density and, as a result, the radiance 4). In visiblewavelength quantum-dot LEDs, inorganic charge-transport layers (ZnO:SnO 2 alloy for electrons and NiO for holes) have recently been used to increase the current density to a few amperes per square centimetre, with a consequent significant improvement in radiance 6 . These results directly reflect the impro...