LEDs are simply diodes that are designed to give off light. When
a diode is forward-biased so that electrons and holes are zipping back and
forth across the junction, they're constantly combining and wiping one another
out. Sooner or later, after an electron moves from the n-type into the p-type
silicon, it will combine with a hole and disappear. That makes an atom complete
and more stable and it gives off a little burst of energy (a kind of "sigh
of relief") in the form of a tiny "packet" or photon of light.
This diagram summarizes what happens:
1. N-type silicon (red) has extra electrons
(black).
2. P-type silicon (blue) has extra holes (white).
3. Battery connected across the p-n junction
makes the diode forward biased, pushing electrons from the n-type to the p-type
and pushing holes in the opposite direction.
4. Electrons and holes cross the junction and
combine.
5. Photons (particles of light) are given off as
the electrons and holes recombine.
Types of LEDs
LEDs are specifically designed so they make light of a certain wavelength and they're built into rounded plastic bulbs to make this light brighter and more concentrated. Red LEDs produce light with a wavelength of about 630–660 nanometers—which happens to look red when we see it, while blue LEDs produce light with shorter wavelengths of about 430–500 nanometers, which we see as blue. (You can find out more about the wavelengths of light produced by different-colored LEDs on this handy page by oksolar). You can also get LEDs that make invisibleinfrared light, which is useful in things like "magic eye" beams that trigger photoelectric in things like optical smokedetectors and intruder alarms. Semiconductor lasers work in a similar way to LEDs but make purer and more precise beams of light.
Photo: LEDs are transparent so light will pass through them. You
can see the two electrical contacts at one end (on the right) and the rounded lens
at the other end. The lens helps the LED to produce a bright, focused beam of
light—just like a miniature light bulb.
invented LEDs
Whom should we thank
for this fantastic little invention? Nick Holonyak: he came up with the idea of the light-emitting diode in 1962
while he was working for the General Electric Company. You might like to watch
a short (4-minute) video about nick holonyaks and
work and his thoughts about the future of LEDs
(courtesy of the Lemelson Foundation); if you're feeling more technically
minded, you can read all about the solid-state physics behind LEDs in the
patents listed in the references below.
LED COLOR
Typical LED
Characteristics
|
|||
Semiconductor
Material |
Wavelength
|
Colour
|
VF @
20mA
|
GaAs
|
850-940nm
|
Infra-Red
|
1.2v
|
GaAsP
|
630-660nm
|
Red
|
1.8v
|
GaAsP
|
605-620nm
|
Amber
|
2.0v
|
GaAsP:N
|
585-595nm
|
Yellow
|
2.2v
|
AlGaP
|
550-570nm
|
Green
|
3.5v
|
SiC
|
430-505nm
|
Blue
|
3.6v
|
GaInN
|
450nm
|
White
|
4.0v
|
Thus, the actual colour of a light emitting diode is determined
by the wavelength of the light emitted, which in turn is determined by the
actual semiconductor compound used in forming the PN junction during
manufacture.
Therefore the colour of the light emitted by an LED is NOT
determined by the colouring of the LED’s plastic body although these are
slightly coloured to both enhance the light output and to indicate its colour
when its not being illuminated by an electrical supply.
Light emitting diodes are available in a wide range of colours
with the most common being red , amber,yellow and green and are thus widely used as visual indicators
and as moving light displays.
Recently developed blue and white coloured LEDs are also
available but these tend to be much more expensive than the normal standard
colours due to the production costs of mixing together two or more
complementary colours at an exact ratio within the semiconductor compound and
also by injecting nitrogen atoms into the crystal structure during the doping
process.
From the table above we can see that the main P-type dopant used
in the manufacture of Light Emitting Diodes is Gallium (Ga, atomic number 31) and that the
main N-type dopant used is Arsenic (As, atomic number 33) giving the resulting
compound of Gallium Arsenide (GaAs) crystalline structure.
The problem with using Gallium Arsenide on its own as the
semiconductor compound is that it radiates large amounts of low brightness
infra-red radiation (850nm-940nm approx.) from its junction when a forward
current is flowing through it.
The amount of infra-red light it produces is okay for television
remote controls but not very useful if we want to use the LED as an indicating
light. But by adding Phosphorus (P, atomic number 15), as a third dopant the
overall wavelength of the emitted radiation is reduced to below 680nm giving
visible red light to the human eye. Further refinements in the doping process
of the PN junction have resulted in a range of colours spanning the spectrum of
visible light as we have seen above as well as infra-red and ultra-violet
wavelengths.
By mixing together a variety of semiconductor, metal and gas
compounds the following list of LEDs can be produced.


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