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IT'S
ALL ABOUT THE CHEMICALS: Blue LEDs have been getting much attention over the
past few years because
their
production had researchers stumped. How did they finally produce blue LEDs? This
article will discuss some of the
interesting
details of blue diode fabrication.
InGaN
films with a high amount of indium are needed to produce blue LEDs. Gallium
nitride platelets can be used but is
difficult
to fabricate. Some other choices are sapphire, aluminum nitride (AIN) and
silicon carbide (SiC). The major reason
sapphire
would be abandoned is the dislocation density created by a large lattice
mismatch when using gallium nitride. AlN
is
more desirable because it matches the crystalline structure of GaN. One of the
advantages of using SiC is it draws heat
from
the PN junction at ten times the rate of sapphire, and SiC's natural cleave
plane can channel energy from a blue
emitting
device. Despite this, sapphire is used simply because it is widely available,
needs no special equipment to use, and
needs
no complex cleaning procedures before growth is begun.
The
problem with the lattice mismatch occurs between the substrate and active layers
of the PN junction, but lateral
epitaxial
overgrowth is the desired method to minimize these dislocation defects. Lateral
epitaxial overgrowth is a process
where
parts of the sapphire substrate are masked and then GaN is grown on top of it.
Ultraviolet photolithography and wet
chemical
etching are used to partially remove the mask before the GaN can be grown.
(However, wet etching is slow but
good
for reducing density).
After
the correct chemicals have been determined and the epitaxial process has been
done, crystals must be grown so the
blue
diode can finally be used. The first step is making the buffer layer. It is
grown after the substrate wafers are etched in
buffered
HG for one minute. This takes place at 900 degrees C using the Metal Organic
Chemical Vapor Deposition
(MOCVD)
process. The GaN starts to come together through a nucleation stage of epitaxial
growth. The third step is
geometric
selection, then the small nuclides fuse to form an island. Then, the islands
expand to cover the buffer area. Lastly,
they
form crystalline planes. Once this is made, it is doped into the P/N junction.
The
brightest LEDs are either single or multiple quantum well structures and
consists of a low temperature GaN or AlN
buffer
layer on a c-plane sapphire or silicon-doped GaN layers. Blue LEDs are III-V
nitride products that are based on
either
a SQW or MQW structure, which vastly improves the efficiency and color purity.
The width of the spectrum for
these
lamps is narrower than the Zn-Si codeped LEDs before them, which makes much
better color saturation. With this
technology,
there are now solid state LED colors that span the entire spectrum.
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