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Callister - An introduction - 8th edition

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856 • Chapter 21 / Optical Properties<br />

electroluminescence<br />

lightemitting<br />

diode<br />

(LED)<br />

In Section 18.15 we discussed semiconductor p–n<br />

junctions, and how they may be used as diodes<br />

or as rectifiers of an electric current. 1 Furthermore,<br />

in some situations, when a forward-biased<br />

potential of relatively high magnitude is applied<br />

across a p–n junction diode, visible light (or infrared<br />

radiation) will be emitted. This conversion<br />

of electrical energy into light energy is termed<br />

electroluminescence, and the device that produces<br />

it is termed a light-emitting diode (LED). The<br />

forward-biased potential attracts electrons on<br />

the n-side toward the junction, where some of<br />

them pass into (or are “injected” into) the p-side<br />

(Figure 21.11a). Here, the electrons are minority<br />

charge carriers and therefore “recombine” with,<br />

or are annihilated by, the holes in the region near<br />

the junction, according to Equation 21.17, where<br />

the energy is in the form of photons of light<br />

(Figure 21.11b). <strong>An</strong> analogous process occurs on<br />

the p-side—holes travel to the junction and<br />

recombine with the majority electrons on the<br />

n-side.<br />

The elemental semiconductors, silicon and<br />

germanium, are not suitable for LEDs due to the<br />

detailed natures of their band gap structures.<br />

Rather, some of the III-V semiconducting compounds<br />

such as gallium arsenide (GaAs), indium<br />

phosphide (InP), and alloys composed of these<br />

materials (i.e., GaAs x P 1–x , where x is a small number<br />

less than unity) are frequently used. Furthermore,<br />

the wavelength (i.e., color) of the emitted<br />

radiation is related to the band gap of the semiconductor<br />

(which is the normally the same for<br />

both n- and p-sides of the diode). For example,<br />

red, orange, and yellow colors are possible for the<br />

GaAs–InP system. Blue and green LEDs have also<br />

been developed using (Ga,In)N semiconducting<br />

MATERIALS OF IMPORTANCE<br />

Light-Emitting Diodes<br />

alloys. Thus, with this complement of colors, fullcolor<br />

displays are possible using LEDs.<br />

Several important applications for semiconductor<br />

LEDs include digital clocks and illuminated<br />

watch displays, optical mice (computer input<br />

devices), and film scanners. Electronic remote controls<br />

(for televisions, DVD players, etc.) also employ<br />

LEDs that emit an infrared beam; this beam<br />

transmits coded signals that are picked up by detectors<br />

in the receiving devices. In addition, LEDs<br />

are now being used for light sources. They are<br />

more energy efficient than incandescent lights,<br />

generate very little heat, and have much longer<br />

lifetimes (because there is no filament that can<br />

burn out). Most new traffic control signals use<br />

LEDs instead of incandescent lights.<br />

We noted in Section 18.17 that some polymeric<br />

materials may be semiconductors (both<br />

+ + –<br />

+<br />

+<br />

Injection of electron into p-side<br />

p-side<br />

n-side<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

(a)<br />

– –<br />

–<br />

–<br />

–<br />

–<br />

–<br />

–<br />

Battery<br />

Recombination (annihilation of electron)<br />

p-side<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

+<br />

–<br />

– –<br />

–<br />

–<br />

–<br />

–<br />

–<br />

–<br />

–<br />

n-side<br />

Photon<br />

emitted<br />

–<br />

–<br />

Battery<br />

1 Schematic diagrams showing electron and hole distributions<br />

on both sides of the junction, with no applied<br />

electric potential, as well as for both forward<br />

and reverse biases are presented in Figure 18.21. In<br />

addition, Figure 18.22 shows the current-versusvoltage<br />

behavior for a p–n junction.<br />

(b)<br />

Figure 21.11 Schematic diagram of a forward-biased<br />

semiconductor p–n junction showing (a) the injection<br />

of an electron from the n-side into the p-side, and<br />

(b) the emission of a photon of light as this electron<br />

recombines with a hole.

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