
Light-induced effects in semiconductors, such as carrier dynamics and defect indication, without doping.Semiconductor light interaction refers to the various ways light and semiconductors affect each other, particularly the generation and dynamics of charge carriers (electrons and holes) when photons are absorbed. This interaction is fundamental to many optoelectronic devices, but it also reveals subtle material properties. For instance, light can excite carriers that then recombine, emitting light or heat, and the details of these processes can indicate the presence of defects or impurities without the need for chemical doping.
The photoelectric effect in semiconductors was first explained by Albert Einstein in 1905, but the modern understanding of carrier dynamics emerged with the development of semiconductor physics in the mid-20th century, particularly through the work of William Shockley and others at Bell Labs.
When a photon with energy greater than the semiconductor's band gap strikes the material, it can be absorbed, promoting an electron from the valence band to the conduction band, leaving behind a hole. These photo-generated carriers can move, recombine, or be trapped by defects. The dynamics — such as carrier lifetime, diffusion length, and recombination pathways — are sensitive to the material's quality and can be probed using techniques like time-resolved photoluminescence or transient absorption spectroscopy. These measurements reveal how light interacts with the semiconductor's electronic structure, including the role of dark states (non-emissive excited states) and charge-transfer states.
This interaction is exploited in solar cells, photodetectors, and LEDs, and it is also used in non-destructive testing of semiconductor wafers to identify defects that could impair device performance.
In some semiconductors, light can be 'slowed down' to speeds of just a few meters per second by creating special quantum states, a phenomenon used in optical delay lines and quantum memory.










