Photonics and Lasers

Chapter 24 - Optical Communications

Chapter 24

 

Optical Communications

We have seen in the preceding chapters how light is generated for photonics applications, how that light propagates, both in fibers and in free space, and how the light can be detected and transformed into an electrical signal. In this final chapter, we show how these different parts all work together in one important application, that of optical communications. This is by no means the only important application, but it nicely illustrates the elements of design that are common in photonic systems. Some of these design issues have already been mentioned earlier in the text. We will now take more of a systems point of view, and consider how the behavior of the various components affects the overall performance of a communications system.

24-1. FIBER OPTIC COMMUNICATIONS SYSTEMS

  In the introductory chapter, we overviewed the topics to be covered by relating them to the simplified optical communications scheme of Fig. 1-2. This overall scheme is repeated in Fig. 24-1, but now with more detail about the choices for the various components. The data can be in analog or digital form, and can modulate the light source either directly, by varying the source s drive current, or indirectly by passing the light through an external modulator. An example of an external modulator is the electrooptic Mach Zehnder device (Fig. 9-21). The light source can be an LED or a laser diode, and the laser diode can be either multiple longitudinal mode (MLM) or single longitudinal mode (SLM). The MLM laser has no frequency-selective element other than the natural Fabry Perot resonances between end facets, and is sometimes referred to as a Fabry Perot laser diode (FP). The SLM laser has an additional frequency-selective element, such as the Bragg grating in a distributed feedback (DFB) or distributed Bragg reflector (DBR) laser. Light can be coupled into the fiber using an evanescent wave device such as the fused biconical taper coupler (Fig. 7-4) or a fiber grating (Fig. 8-5). The fiber can be step-index or graded index, and the step index fiber can be single-mode or multimode. Finally, light exiting the far end of the fiber can be detected with a PIN photodiode or avalanche photodiode (APD).

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