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weakened optical signal is pumped into the ingress edge of a semiconductor optical amplifier. The active layer of the semiconductor substrate amplifies the signal and regenerates it on the other side. The primary downside to these devices is their size. They are small, and their light-collecting capabilities are therefore somewhat limited. A typical single-mode fiber generates an intense spot of light that is roughly 10 microns in diameter. The point upon which that light impinges upon the semiconductor amplifier is less than a micron in diameter, meaning that a lot of the light is lost. Other problems also crop up, including polarization issues, reflection, and variable gain. As a result, these devices are not in widespread use; EDFAs and Raman amplification techniques are far more common.

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battery B, resistor R, milliammeter mA, and diode D. At A, forward bias results in current flow; at B, reverse bias results in no current.

half-wave rectifier. At B, the output of a fullwave rectifier. Note the difference in how the effective (eff ) voltages compare with the peak voltages.

electrons, is made even more deficient. The N-type material constantly feeds electrons to the P-type in an attempt to create an electron balance, and the battery or power supply keeps robbing electrons from the P-type material. This is shown in Fig. 19-5A and is known as forward bias. When the polarity is switched so the N-type material is positive with respect to the P type, things get interesting. This is called reverse bias. Electrons in the N-type material

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Creating EAN - 13 Barcodes with C# - CodeProject
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So far, we have discussed the sources of light, including LEDs and laser diodes. We have briefly described the various flavors of optical fiber and the problems they encounter as transmission media. Now we turn our attention to the devices that receive the transmitted signal. The receive devices used in optical networks have a single responsibility: to capture the transmitted optical signal and convert it into an electrical signal that can then be processed by the end equipment. Various stages of amplification may be used to ensure that the signal is strong enough to be acted upon, and demodulation circuitry may be used to recreate the originally transmitted electronic signal.

A better scheme for changing ac to dc takes advantage of both halves of the ac cycle A full-wave center-tap rectifier has a transformer with a tapped secondary (Fig 21-1B) The center tap is connected to electrical ground, also called chassis ground This produces voltages and currents at the ends of the winding that are in phase opposition with respect to each other These two ac waves can be individually half-wave rectified, cutting off one half of the cycle and then the other, over and over The effective output voltage from a power supply that uses a full-wave center-tap rectifier is greater, relative to the peak voltage, than is the case with the half-wave rectifier (Fig 21-2B) The PIV across the diodes can, nevertheless, be as much as 28 times the applied rms ac voltage Therefore, the diodes should have a PIV rating of at least 4.

P-N junction; at B, reverse bias. Electrons are shown as small dots, and holes are shown as open circles.

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