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Photodiodes and Receivers



          108  Chapter Seven


                      In addition, the photodetector needs to
                      ■ Be insensitive to temperature variations
                      ■ Be compatible with the physical dimensions of the fiber
                      ■ Have a reasonable cost compared to that of other system components
                      ■ Have a long operating lifetime

                        Semiconductor-based photodiodes are the main devices that satisfy this set of
                      requirements. The two types of devices used are called a pin photodiode and an
                      avalanche photodiode (APD). This section addresses characteristics of pin photo-
                      diodes, and Sec. 7.2 discusses the APD.


          7.1.1. Operation of a pin photodiode
                      The most common photodetector is the semiconductor pin photodiode, shown
                      schematically in Fig. 7.1. The device structure consists of p and n semiconduc-
                      tor regions separated by a very lightly n-doped intrinsic (i) region. In normal
                      operation a reverse-bias voltage is applied across the device so that no free elec-
                      trons or holes exist in the intrinsic region.
                        Recall from Sec. 6.1 that electrons in semiconductor materials are allowed to
                      reside in only two specific energy bands, as shown in Fig. 7.2. The two allowed
                      bands are separated by a forbidden region called an energy gap. The energy dif-
                      ference between the top and bottom bands is referred to as the bandgap energy.
                        Now suppose an incident photon comes along that has an energy greater than
                      or equal to the bandgap energy of the semiconductor material. This photon can
                      give up its energy and excite an electron from the valence band to the conduc-
                      tion band. This process, which occurs in the intrinsic region, generates free
                      (mobile) electron-hole pairs. These charge carriers are known as photocarriers,
                      since they are generated by a photon. The electric field across the device causes
                      the photocarriers to be swept out of the intrinsic region, thereby giving rise
                      to a current flow in an external circuit. This current flow is known as the
                      photocurrent.

















                      Figure 7.1. Schematic of a  pin photodiode circuit with an
                      applied reverse bias.


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