critical parameter for almost all applications involving photon absorption or emission, such as solar cells, solid-state lighting, detectors, displays, sensors, lasers and photocatalytic reactions. In solar cells, only photon energies close to the bandgap energy can be converted into electricity: higher-energy photons lose energy by thermalization and phonon generation, whereas lower-energy photons are simply transmitted through the solar cell. Thus, efficient solar cells require the combined use of multiple semiconductors with various bandgaps. Multicolour or multiwavelength photodetectors and on-chip spectrometers would be enabled by semic onductors with a larger range of bandgaps. In solid-state lighting, illumination and displays, direct red-green-blue (RGB) or multicolour emission is desired to achieve, in the long term, high efficiency and low-cost fabrication. This requires semi conductors with bandgaps in the range 1.77-3.1 eV. For solid-state lighting, it is still impossible to realize all-semiconductor white light-emitting diodes (LEDs) from a single mono lithic semiconductor to enable light sources with high luminosity and long lifetimes. The conventional approaches still use non-semiconductor phosphors combined with a semiconductor emitter for the generation of white light, which results in inefficient and low-quality lighting.