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Light Sources and Transmitters



          90  Chapter Six


                      device can be turned on and off by an electric signal to produce a corresponding
                      optical output pattern. As the next two sections describe, laser diodes can be
                      modulated significantly faster than LEDs. However, there is a speed limit
                      beyond which even the laser does not respond fast enough to the changes in an
                      electric signal. Beyond this point a steady light output stream from the laser
                      diode is fed into an external device, which can change the intensity of the light
                      that passes through it very rapidly. This process is known as external modula-
                      tion. Section 6.5 describes external modulators in greater detail.


          6.2. LEDs
                      If we look around us, we notice LEDs everywhere. They can be seen glowing
                      green, yellow, or red in vehicles, computer equipment, kitchen appliances, tele-
                      phones, cameras, and every imaginable piece of electronic equipment. They
                      are inexpensive and highly reliable light sources. The LEDs used in optical
                      communications are much smaller and emit in the infrared region, but com-
                      pared to the other telecommunication light sources used, they are much less
                      expensive and easier to use in transmitter designs. However, because of their
                      relatively low power output, broad emission pattern, and slow turn-on time,
                      their use is limited to low-speed (less than 200-Mbps), short-distance (up to a
                      few kilometers) applications using multimode fibers.

          6.2.1. Principles of operation
                      To create a material structure for an LED, n-type and p-type semiconductor
                      materials are joined together. The boundary between the two joined materials
                      is called a pn junction, as shown in Fig. 6.2. To create a supply of electrons and
                      holes that may flow across the pn junction to recombine and thereby emit light,
                      one applies a voltage across the junction. This is called a bias voltage. Variations
                      in the applied voltage, or the driving current, then correspond to a varying opti-
                      cal output from the device. Figure 6.3 shows a typical relationship between the
                      optical power generated by an LED and the drive current. Nominally LEDs

















                      Figure 6.2. Electrons and holes
                      recombine at a  pn junction and
                      thereby emit light.


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