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In the world of semiconductor photonic device fabrication, one
important objective may be to extract as much light as possible
from the device. In these devices, photons are created when
electrons recombine with holes by transitioning from a high- energy
state to a lower one. Unfortunately, electron-hole recombination
does not always result in the formation of a photon. There are
three basic types of recombination: the first results in the
formation of a photon and is called radiative recombination; and
the second and third, known as Shockley-Read-Hall and Auger
recombination, result in the heating of the device and do not
produce photons and are therefore called non-radiative
recombination. All three processes occur simultaneously in a
device, and either a radiative or non-radiative recombination
coefficient can be associated with the relative rate of each. The
lifetime of an electron in a high-energy state is so small, on the
order of nanoseconds, that there is no way to measure these
coefficients directly. However, sum frequency generation is a
technique to indirectly measure these coefficients by taking
advantage of the speed of light to resolve these processes in time.
From the resulting data, these recombination coefficients can be
extracted.
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